Dew Harvesting -- Dozens of articles & abstracts re:
condensation & collection of atmospheric humidity


**[![](0logo.gif)](../index.htm)  
[rexresearch.com](../index.htm)**


---

**Dew Harvesting**



---



---

**[Gabin Koto
NaGobias Dew Collector](#1inspiring)****[Nikolayev : Water recovery from dew](#2nikol)****[Nikolayev : Water recovery from dew](#3fog)****[Beysens, et al. : Water production in an
ancient sarcophagus at Arles-sur-Tech](#4arles)****[Beysens & Milimouk : The Case For
Alternative Fresh Water Sources](#5case)****[Beysens, et al. : Collecting dew as a
water source on small islands: the dew equipment for water
project in Bisjevo (Croatia)](#6croatia)****[New Architectural Forms to Enhance Dew
Collection](#7arch)****[Estimates of global dew collection
potential on artificial surfaces](#8estimates)****[Khalil, et al. : A review: dew water
collection from radiative passive collectors to recent
developments of active collectors](#9review)****[Wahlgren : Atmospheric water vapour
processor designs for potable water production: a review](#10atmsovap)****[Nikolayev : Water recovery from dew](#11waterrecov)****[Muselli : Dew and rain water
collection in the Dalmatian Coast, Croatia](#12dewrain)****[Muselli : A comparative study of two
large radiative dew water condensers](#13compar)****[MuA+/-oz-GarcA-a : Water harvesting for
young trees using Peltier modules powered by photovoltaic
solar energy](#14waterharv)****[Milani : Evaluation of using
thermoelectric coolers in a dehumidification system to
generate freshwater from ambient air](#15evaluation)****[Maestre-Valeroa, et al. :
Estimation of dew yield from radiative condensers by means of
an energy balance model](#16estimation)****[Maestre-Valero, et al. ;
Comparative analysis of two polyethylene foil materials for
dew harvesting in a semi-arid climate](#17companalys)****[Lekoucha, et al. : Rooftop dew, fog
and rain collection in southwest Morocco and predictive dew
modeling using neural networks](#18rooftop)****[Kabeel, et al. : Water production
from air using multi-shelves solar glass pyramid system](#19waterprod)****[Jacobs ; Passive dew collection in a
grassland area, The Netherlands](#20passive)****[Hamed : Application of Solar
Energy for Recovery of Water from Atmospheric Air in Climatic
Zones of Saudi Arabia](#21application)****[Hamed : A technical review on the
extraction of water from atmospheric air in arid zones.](#22techrev)****[Gindel : Irrigation of Plants with
Atmospheric Water within the Desert](#23gindel)****[O. Clus, et al. : Comparison of
various radiation-cooled dew condensers using computational
fluid dynamics](#24comparison)****[O. Clus, et al. : Study of dew water
collection in humid tropical islands](#25study)****[D. Beysens, et al. : Collecting dew
as a water source on small islands: the dew equipment for
water project in Bis?evo (Croatia)](#26collecting)****[D. Beysens, et al. : Chemical and
biological characteristics of dew and rain water in an urban
coastal area (Bordeaux, France)](#27chemical)****[Daniel Beysens ; Using radiative
cooling to condense atmospheric vapor: a study to improve
water yield](#28radiative)****[Alnaser & Barakat : Use of
condensed water vapour from the atmosphere for irrigation in
Bahrain](#29condensed)****[Beysens : Dew collection roof retrofit](#30dewcoll)****[Beysens : Application of passive
radiative cooling for dew condensation](#31application)****[Tomaszkiewicz : Dew as a sustainable
non-conventional water resource: a critical review](#32dew)****[Beysens : Use of a composition
comprising a polymeric matrix and a charge containing kaolin
for radiative cooling](#33fr2917)****[Air Well Patents](#patents)**  



---

[**http://inspiringfuture.org/wordpress/2014/05/21/dew-harvesting-as-a-means-to-get-clean-drinking-water/**](http://inspiringfuture.org/wordpress/2014/05/21/dew-harvesting-as-a-means-to-get-clean-drinking-water/)**[ Excerpts ]**  
  
**Gabin Koto NaGobias Dew Collector**  
  
The lack of water in the Northern region of his home country Benin
motivated Gabin Koto NaGobi to design a dew collector.  
  
His prototype is made out of local materials which makes it
sustainable and accessible. It harvests up to 4 liters of water
per night...  
  

[ Click to enlarge ]

![](GabinKotoNGobi.jpg)

  
**geometrical shapes and efficiency**  
  
These designs might make you wonder about the effect of different
shapes on the efficiency of dew collecting. During summer and fall
2009 experiments have been done (Pessac, France) to get an answer
to this question. The results were published in aNew Architectural
Forms to Enhance Dew Collectiona (Daniel Beysens, Filippo
Broggini, Iryna Milimouk-Melnytchouk, Jalil Ouazzani, Nicolas
Tixier)  
   
**a. conical**  
  

![](conical.jpg)

60A deg cone angle (30A deg from horizontal)  
  
the 30A deg angle has been found to give the best cooling efficiency.
This angle also allows water to easily flow by gravity as the
gravity forces are only reduced by 50% with respect to vertical.  
  
YIELDS: an average of 22% larger than the planar reference
condenser (30% at wind speeds below 1.5 m/s to 0% above 3 m/s).
The gains are larger for low dew yields.  
  
**b. inverted pyramid**

**![](pyramid.jpg)**

  
Here the surface also has an angle of 30A deg from horizontal  
  
YIELDS: an average of 20% larger than the planar reference
condenser. The gains are larger for low dew yields, these
increased gains are lower though than with the conical shape.  
  
As these shapes are somewhat unpractical when making constructions
to collect dew on large scale, tests were also made with hollow
shapes that could be atileda on a bigger surface, like a roof. In
this way the collecting surface can be increased without needing
more horizontal space nor an unpractical increase of vertical
space.  
  
**c. egg-box**

**![](eggbox.jpg)**

  
YIELDS: an average of 10% larger than the planar reference
condenser.  
  
Note that part of the formed dew canat be collected because of the
areas where the angle is too low for the drops to flow off (the
flat tops of the egg bumps)  
  
**d. origami**

**![](origami.jpg)**

  
YIELDS: an average of 120% larger than the planar reference
condenser, with much higher gains for low dew yields (up to 400%)  
  
So we can see that the geometrical shape of the collectors is of
great influence to the amount of dew that can be collected. The
big advantage of hollow shapes lies in the fact that influences of
the wind are decreased, and thus the cooling is increased...  
  
    The ability to absorb water vapor from the
atmosphere enables ticks to survive without drinking water for
many months. The tick rehydrates using a three-stage process.
First, it uses its foremost pair of legs to detect microregions of
high humidity, such as those surrounding water droplets. Once a
suitable water source is detected, the tick secretes a hydrophilic
solution from its mouth. Once it is saturated, the tick draws the
now hydrated secretion back into its mouth. The secretion is a
hygroscopic salt solution. Once ejected from the mouth, the
solution dries at low ambient humidities, leaving a crystalline
substance behind. When the humidity increases, the hydrophilic
crystalline substance dissolves and is swallowed back into the
body of the tick. The adaptation allows exophilic ticks to absorb
water vapor from close to saturation down to 43% relative
humidity. Mites and soil-dwellings use a similar mechanism to
absorb water vapor.-- asknature.org  
  
**footnotes:**  
  
1)  
to calculate the dew point:  
  
Td = 243.12 \* A / (17.62 a A)  
  
where:  
  
A = Log(RH / 100) / Log(2.718282) + (17.62 \* Ta / (243.12 + Ta))  
  
RH = relative humidity (%)  
  
Ta = air temperature (degrees celsius)  
  
Td = dew point (degrees celsius)  
2)  
  
the OPUR condensing foil is 0.39 mm thick and made of 5.0 vol %  
of TiO2 microspheres of 0.19 Aum diameter, and 2.0 vol. % of BaSO4
of 0.8 Aum diameter embedded in a matrix of low-density
polyethylene (LDPE). It also contains approximately 1 vol % of a
surfactant additive non-soluble in water. This material improves
the mid-infrared emitting properties to provide radiative cooling
at room temperature and efficiently reflects the visible (sun)
light  
  


---

  
[**https://hal.archives-ouvertes.fr/hal-01264194/document**](https://hal.archives-ouvertes.fr/hal-01264194/document)

**Water recovery from dew**  
**by N. Nikolayev  
[ [PDF](nikolayevwaterecoverydew.pdf) ]**

  


---

  
[**https://arxiv.org/ftp/arxiv/papers/0707/0707.2931.pdf**](https://arxiv.org/ftp/arxiv/papers/0707/0707.2931.pdf)

**Fog and dew collection projects in croatia
- arXiv.org**

**[ [PDF](fogdewcollextioncroatia.pdf)
]**

  


---

  
[**http://www.opur.fr/angl/publications\_ang.htm**](http://www.opur.fr/angl/publications_ang.htm)**International Organization For Dew Utilization** [**http://www.opur.fr/fr/Arles-fr.pdf**](http://www.opur.fr/fr/Arles-fr.pdf)  
**Atmospheric Research, 57, 201-212, 2001**  

**Water production in an ancient sarcophagus
at Arles-sur-Tech (France),**   
**D. Beysens, M. Muselli, J.-P. Ferrari, A. Junca,**   
**[ [PDF](Arles-fr.pdf) ]**

  


---

  
[**http://www.opur.fr/angl/Secheresse-angl.pdf**](http://www.opur.fr/angl/Secheresse-angl.pdf)**SA(c)cheresse, Vol. 11, nA deg 4, dA(c)cembre 2000**

**The Case For Alternative Fresh Water
Sources**  
**D. Beysens, I. Milimouk**  
**[ [PDF](Secheresse.pdf) ]**



---

  
[**http://iramis.cea.fr/spec/Phocea/Pisp/index.php?nom=vadim.nikolayev**](http://iramis.cea.fr/spec/Phocea/Pisp/index.php?nom=vadim.nikolayev)

**Vadim Nikolayev**

**Service de Physique de l'Etat CondensA(c)****p. 227, BAcentt. 772, Orme des Merisiers****91191 Gif sur Yvette Cedex****France****tel.jpg +33 1 69 08 94 88****fax.png +33 1 69 08 87 86****email.gif vadim.nikolayev(at)cea.fr**  
[**http://inac.cea.fr/sbt/Phocea/Vie\_des\_labos/Ast/ast\_visu.php?id\_ast=432**](http://inac.cea.fr/sbt/Phocea/Vie_des_labos/Ast/ast_visu.php?id_ast=432)

**Condensation de vapeur daeau atmosphA(c)rique
(rosA(c)e)**  
**D. Beysens, V. Nikolayev, M. Muselli, O. Clus, I. Melnytchouk**

  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0360544206002684**](http://www.sciencedirect.com/science/article/pii/S0360544206002684)

**Collecting dew as a water source on small
islands: the dew equipment for water project in Bisjevo
(Croatia)**  
**D. Beysens, O. Clus, M. Miletac, I.
Milimouk, M. Muselli, V.S. Nikolayev**

**Abstract**  
In many regions and geographical settings, dew water collection
can serve as a water source, supplementing rain and fog water
collection. This is particularly useful when precipitation is low
or lacking, especially in remote areas and islands in the dry
season. A project called Dew Equipment for Water (DEW) was
initiated for a 15.1 m2 roof in the island of BiA!evo (Croatia),
equipped with commercial plastic cover selected for its superior
dew collection properties. Measurements of both rain and dew water
will be performed over several years and data will be correlated
with meteorological data collected in situ. Preliminary
measurements during the period 21 Aprila21 October 2005 showed
that dew water contributed significantly, 26% of the total
collected water.  
  


---

  
[**http://www.aidic.it/cet/13/34/014.pdf**](http://www.aidic.it/cet/13/34/014.pdf)

**New Architectural Forms to Enhance Dew
Collection**  
**[ [PDF](archforms.pdf) ]**

  


---

  
[**http://www.hydrol-earth-syst-sci.net/19/601/2015/hess-19-601-2015.pdf**](http://www.hydrol-earth-syst-sci.net/19/601/2015/hess-19-601-2015.pdf)

**Estimates of global dew collection
potential on artificial surfaces**  
**[ [PDF](hess.pdf) ]**

  


---

  
[**http://link.springer.com/article/10.1007/s40899-015-0038-z**](http://link.springer.com/article/10.1007/s40899-015-0038-z)**Sustainable Water Resources Management, March 2016, Volume
2, Issue 1, pp 71a86**

**A review: dew water collection from
radiative passive collectors to recent developments of active
collectors**  
**B. Khalil, et al.**

**Abstract**  
Dew water is water droplets formed due to condensation of
atmospheric water vapor on surfaces of temperature below its dew
point temperature. Dew water can be seen as a nonconventional
source of water and may be exploited in regions where weather
conditions favor dew formation and inadequate supply and quality
of water is a prevalent problem. There are two main types of dew
condenser, the apparatus used to collect dew water, namely
radiative (also called passive) and active condensers. Radiative
passive collectors rely on exploiting the physical processes
responsible for dew formation to collect dew water without any
additional energy input. Previous studies indicate that a 1 m2
radiative condenser yields between 0.3 and 0.6 L/day of dew water
in arid and semi-arid regions. Active condensers have been
designed as an alternative method of collection that produces
higher yields by using additional energy inputs. Several designs
of active condensers have been patented for which the yield can
reach 20 L/day for portable devices, and up to 200,000 L/day for
larger agricultural water devices. Active condensers are also
known as atmospheric water generators, dehumidifiers, and air to
water devices. Most of the active condensers are based on a
regenerative desiccant that attracts and holds large volumes of
water from the air or on a means of cooling the condensing surface
below the dew point temperature (refrigeration circuit). The
larger yields and wider range of environmental conditions in which
dew can be collected make active condensers a promising option as
an alternative or supplemental source of water in water scarce
regions. The aim of this paper was to provide a comprehensive
review of radiative and active condensers, including dew formation
processes, methods of dew collection, and parameters that
influence the dew collection. Subsequently, patents of active
condensers were reviewed to ascertain how they ca n be integrated
with different types of renewable energy and to assess the
potential use of such integrated systems as a sustainable source
of water in regions that suffer water scarcity and/or as a
sustainable source of water for agriculture.  
  
**Introduction**  
  
Dew water collection can be considered as a non-conventional
source of water which can enhance water supply in certain
climates/regions. Hence, it can be considered as a possible
alternative or supplementary source of water in many water scarce
regions of the world where weather conditions favor dew formation.
The atmospheric air can be considered as a huge renewable
reservoir of water which can be used as a water source everywhere
on the earth (Hamed et al. 2010). The amount of water in air is
assessed as 14,000 km3, while the amount of fresh water in the
earth is about 1200 km3 (Hamed et al. 2010). Despite this
significant volume of potentially extractable fresh water in many
places where weather conditions favor dew formation, dew water
collection systems are rare, suggesting dew collection is an
under-explored alternative for providing good quality water.  
  
Current dew water collectors are divided into two main types:
radiative (or passive) and active dew water condensers. Research
on radiative condensers started in the early 1960s (Gindel 1965).
Since then, research has focused on the condenser materials,
architecture, influence of meteorological parameters, and other
factors that affect the volume of dew water collected using
radiative condensers. According to the radiative energy available
for condensation, the upper limit of dew yield is 0.8 L/day/m2
(Monteith and Unsworth 1990). However, the maximum recorded yields
of dew water in arid and semi-arid climates typically fall within
a range of 0.3a0.6 L/day/m2 of surface area (Muselli et al. 2009;
Maestre-Valero et al. 2011; Lekouch et al. 2012). Studies
conducted in more humid climates showed lower yield; for example,
in a perennial grassland environment in the Netherlands, the
maximum water collected was 0.19 L/day/m2 (Jacobs et al. 2008);
for a humid tropical island in French Polynesia, the maximum
amount was 0.23 L/day/m2 (Clus et al. 2008); and in an
agricultural environment near an urban area in
Sainte-Anne-de-Bellevue, QC, Canada, the maximum amount was 0.37
L/day/m2 (Khalil et al. 2015).  
  
Early designs for active dew condensers were developed in the
1930s, but innovation has increased since the commercialization of
mechanical refrigeration (Wahlgren 2000). Active condensers are
now considered an innovative option for locally managed water
supply systems in areas with water quality and/or quantity
problems (Wahlgren 2000). Active condensers work in a manner
similar to that of a dehumidifier to extract water from the air.
Although they are more effective than the radiative condensers in
terms of water yield per day, they require a source of energy
which makes their operating costs much higher than those of
radiative condensers which do not require an energy source.
However, recent active condensers are designed to minimize the
energy required or make use of renewable energy resources that can
be integrated into the condenser. For example, most modern solar
stills integrate additional solar cells to provide supplementary
energy to the system (Bundschuh and Hoinkins 2012). Active
condensers are also often equipped with filtration and
purification units such as ozone treatment units. The water yield
of active condensers varies depending on the design/purpose;
yields fall within the range of 15a50 L/day for a small portable
drinking water unit to up to 200,000 L/day for larger agricultural
scale designs (Peters et al. 2013). In this paper, a comprehensive
review for different radiative and active condensers was provided
and their potential for agricultural uses was discussed.  
  
**Radiative systems**  
Understanding the principles of dew formation is important for
designing both effective radiative as well as active dew
condensers that exploit these processes to collect dew. Dew
formation is a natural occurrence where a phase transition from
gaseous to liquid water occurs on an exposed surface (Beysens
1995; Agam and Berliner 2006). Dew formation is affected by
several factors such as vapor pressure, air temperature, relative
humidity, and wind speed. The vapor pressure is defined as the
pressure exerted by the gaseous water in equilibrium with its
liquid phase at a given temperature (McCabe et al. 1993). If the
pressure increases, it will reach a maximum point where, passed
that point, there will be a net loss of molecules from the
atmosphere (i.e., condensation). This maximum pressure reached by
the water vapor is called the saturation vapor pressure and is the
point where the atmosphere is completely saturated with water
molecules. The saturated vapor pressure is a function of the air
temperature, and their relationship can be described by the
following equation (Alnaser and Barakat 2000):  
  
es=0.611exp(17.27(Ta-273)Ta-36)  
(1)  
  
where es is the saturated vapor pressure in kPa and Ta represents
the ambient temperature in Kelvin.  
  
When a constant atmospheric pressure is assumed, an increase or
decrease in ambient temperature will also increase or decrease the
saturated vapor pressure. If air is cooled at constant humidity to
become saturated, the corresponding temperature at a given point
is called the dew point temperature. If the temperature of an
exposed surface is equal to or lower than the dew point
temperature, condensation will occur (Agam and Berliner 2006).
Moreover, if the exposed surface is maintained at a lower
temperature than the air above it, according to Eq. (1), the
saturated vapor pressure will be lower near that surface. This
difference in vapor pressure is the gradient for mass transfer to
take place since the water molecules in the atmosphere will go
from high to low vapor pressure, allowing condensation to occur
near the exposed surface without bringing the bulk of the air to
its dew point temperature.  
  
The dew formation rate depends on the amount of water vapor in the
air; this amount is related to the absolute humidity (i.e., the
amount of gaseous molecules in the air) and the difference between
the dew point and ambient temperature. This notion is expressed by
the relative humidity (RH), which is defined as the amount of
water vapor in the air at a given temperature with respect to the
maximum amount of water vapor that the air can hold at that same
temperature. It can also be defined as the contribution made by
water vapor to the total atmospheric pressure over the maximum
pressure that the water vapor can exert at the current temperature
(Alnaser and Barakat 2000):  
  
RH=e(Ta)es(Ta)A100  
(2)  
  
where RH is the relative humidity in % and e is the vapor pressure
in kPa. Given the definition of the dew point temperature, the
relative humidity can also be expressed as follows (Alnaser and
Barakat 2000):  
  
RH=es(Td)es(Ta)A100  
(3)  
  
where Td is the dew point temperature in Kelvin. The RH depends on
both the difference between the dew point and the ambient
temperature, and the humidity of the air (Alnaser and Barakat
2000).  
  
Based on these principles, a radiative condenser (also called a
passive dew condenser) rely on exploiting the physical processes
responsible for dew formation to collect dew water without any
additional energy input. The surface of radiative condensers has a
high emittance in the infrared region of the spectrum that allows
it to cool faster than other surfaces at night-time. Therefore, to
attain the required dew point temperature and induce the
collection of dew water, the environmental conditions have to be
conducive to surface cooling and the exposed surface (i.e., the
condenser) has to be optimized to enhance cooling.  
  
Several parameters influence radiative dew collection (Fig. 1).
The imposed parameters describe the meteorological conditions that
enhance or reduce the formation of dew. They are related to the
physical principles behind the technology of the radiative
systems. The variable parameters are the components of the
condenser that are modified to optimize the collection of dew.  
  
**Fig. 1****Factors affecting dew collection**

**![](Fig1.gif)**

**Weather conditions**  
Dew water condensation occurs during the early morning (Jacobs et
al. 1998; Kidron 2000) when the environmental conditions are
favorable. It is important to consider the dependency of dew
formation on weather conditions, such as sky emissivity, relative
humidity, and wind speed, in the study of dew water condensation
(Beysens et al. 2003, 2006; Shank 2006).  
  
**Sky emissivity**  
  
Low emissivity through the sky is known to prevent water vapor
condensing, as it does not allow radiation to escape from surfaces
at ground level (GlAcurrencyser and Ulrich 2013); therefore, higher
emissivity is ideal for condensation to occur. Dew formation is
more likely to occur under clear skies. For example, studies in
continental and coastal areas showed that yield was directly
proportional to atmospheric transparency and sky visibility to
infrared radiation (Beysens et al. 2006; Muselli et al. 2009).  
  
Surfaces cool at night since there is a net flux of radiation
energy emitted toward the sky. This radiation lies in the infrared
region of the spectrum (?, 8a13 Aum), which is the region
associated with thermal radiation (Alnaser and Barakat 2000).
During the night, the net radiation of a surface is emitted toward
the sky and a fraction of the radiation is lost to space. However,
the radiative energy can partially be absorbed by the water and
carbon dioxide in the atmosphere, and part of this absorbed energy
is radiated back to the surface, reducing the net long wave
radiative cooling effect (Beysens et al. 2007). Therefore, clear
nights when there is a lot of water held in the atmosphere are
more conducive to thermal cooling of radiative surfaces than
cloudy nights.  
  
As clear nights allow greater surface cooling, they are optimum
for dew formation, as opposed to cloudy nights (Kidron 2000).
Muselli et al. (2009) found that dew yields decreased
approximately linearly with the increase of mean cloud cover,
which was used as an indicator of thermal emissivity of the sky,
as described by the following equation:  
  
h=h0(10-N-)  
(4)  
  
where N- is the mean night-time cloud cover that was equal to 0
for clear sky and 10 for totally cloudy sky; h is the mean dew
yield (mm/day) and h0 is the mean dew yield when the cloud cover
was equal to zero. It is important to note that in this experiment
the maximum yield did not correspond to N- being zero but to N-
being approximately three. In fact, the dew yield was relatively
low for the nights that were totally clear; for two sites situated
in the Mediterranean basin, h0 was equal to 0.018 and 0.016 mm,
which is relatively low when considering that the mean dew yield
was 0.138 and 0.108 mm, respectively.  
  
The discrepancy between mean dew yield and yield when skies were
clear can be explained by the fact that a clearer sky also
corresponded to drier air (Muselli et al. 2009), showing that a
certain level of absolute humidity is required for dew
condensation to occur. For example, it has been found that the
frequency at which dew events occurred in humid environments was
20 % higher than in semi-arid Mediterranean climates, which
resulted in a higher cumulative dew water formation during the
summer in the humid environment (5.58 L/m2/summer) than in the
semi-arid environment (3.5 L/m2/summer) (Clus et al. 2008). In
addition, a study in Morocco concluded that circulation of humid
marine air was an important factor controlling dew yield (Lekouch
et al. 2012), again showing the importance of atmospheric water
content for dew condensation.  
  
However, the absolute humidity of the atmosphere also affects the
emissivity of the sky, with radiation being reduced when absolute
humidity is high. For example, the high absolute humidity in
environments such as wetland ecosystems or tropical climates
hinders dew formation (Clus et al. 2008; Xu et al. 2013).
Conversely, the drier Mediterranean climate allows for higher dew
yields (Clus et al. 2008).  
  
**Relative humidity**  
  
The relative humidity is highly correlated to dew water yields. In
a study comparing two large (30 m2 in area) passive dew condensers
in Ajaccio, France, Muselli et al. (2006) found that the limiting
value of humidity below which dew did not form was 80.7 and 79.3 %
for both condensers. Similarly in southwest Morocco, Lekouch et
al. (2012) found that water mostly condensed when the relative
humidity was between 74 and 92 %. In the same study, the authors
defined the relationship between the relative humidity and the air
and dew point temperature difference as (LeKouch et al. 2012):  
  
ln(RH)=k(Ta-Td)  
(5)  
  
where k is a constant that varied only slightly with the air
temperature Ta in Kelvin. This relationship was found to be
important since nearly all the data points were below the line
described by the equation (Clus et al. 2008; Lekouch et al. 2012):  
  
h=h'?T0[?T0-(Td-Ta)]  
(6)  
  
where h' is the maximum yield for one night (L/m2/day) and ?T0 was
the maximum difference in temperature between the surface of the
condenser and the air (Clus et al. 2008; Lekouch et al. 2012). The
?T0 can be used as a measure of the performance of the dew
condenser in a specific location; for example, ?T0 was used to
compare the efficiency of dew collection in three locations:
Morocco, Zadar and Komiza (Croatia). In Morocco it was found that
the maximum temperature difference between the surface of the
condenser and the air temperature was -5.3 A degC, whereas the
difference was slightly greater in the two locations situated in
the Adriatic area of the Mediterranean basin; in Zadar it was -9.2
A degC, and in Komiza it was -8.0 A degC (Muselli et al. 2009; Lekouch et
al. 2012). Thus, it can be concluded that the surface of the
condenser cooled to a greater extent in the Adriatic locations
than in Morocco.  
  
The linear relationship described in Eq. (6) suggests that the
difference between air and dew point temperature, or the relative
humidity, can be the main parameter that limits the dew yield. In
fact, several studies have found a linear relationship between the
dew yield and difference between the air and dew point temperature
and, therefore, a logarithmic relationship with the relative
humidity (Sharan et al. 2007; Muselli et al. 2009). However,
Muselli et al. (2009) did not find this linearity statistically
significant. Muselli et al. (2009) concluded that the relative
humidity alone was not enough to model dew yield, and that the
night net radiation was another important parameter in the
formation of dew on condensers.  
  
**Wind speed**  
  
Wind has both a hindering and enhancing effect on dew
condensation. It is necessary to bring humid air, but also reduces
radiative cooling by increasing the heat exchange between the
warmer air and the surface of the collector (Beysens et al. 2003).
Gandhidasan and Abualhamayel (2005) suggested that in dry
conditions, strong winds do not favor dew condensation. In a study
conducted in the humid tropical island of French Polynesia, dew
yields declined rapidly for wind velocities higher than 3 m/s, and
dew was almost absent for velocities higher than 4 m/s (Clus et
al. 2008). Similarly, the limiting wind speed for condensation in
the Adriatic area of the Mediterranean basin was 4.7 m/s,
according to a study conducted in Zadar (Muselli et al. 2009).
Therefore, protecting the condenser from direct wind can be
beneficial for improving dew condensation. On the other hand, low
wind speeds are necessary to bring atmospheric water vapor to the
surface of the condenser; a study in southwest Morocco found that
dew formed when wind was in the range of 0.15a0.7 m/s (Lekouch et
al. 2012).  
  
The technology behind radiative dew water collection system is
relatively simple as it relies on exploiting the physical
processes of dew formation, and no additional energy input is
necessary. However, the radiative cooling power of passive dew
collectors is a function of the weather (ambient temperature,
relative humidity, and cloud cover), which affects yield in
relatively complex ways. Overall, however, the ideal weather
conditions are usually found in arid and semi-arid climates, which
also tend to be water scarce. By implementing this technology, it
will be possible to produce drinkable water with no additional
energy input and consequently with a very small footprint.
However, due to the very particular weather conditions necessary
for maximum condensation of dew (i.e., relative humidity ~80 %,
and cloud cover and wind speed low but greater than zero), the
water yield per day is typically relatively low and difficult to
predict. This makes dew collection using radiative condensers a
non-reliable water source, although optimizing condenser design
can go some way to improving yields.  
  
**Design of radiative dew condensers**  
Given the dependence of radiative systems on the dew formation
physical processes, their design has to be optimized to allow
surface cooling without any external energy input. In particular,
there are a number of factors that must be optimized to increase
the yield. First, it is important to maximize the infrared
wavelength emitting properties of the condensing surface to allow
surface cooling at night. Second, absorption of the visible light
must be reduced to prevent daytime warming of the condenser, which
means having a higher reflectivity in the visible part of the
spectrum (i.e., white materials). Third, the heating effect of the
wind must be reduced by lowering its velocity, which is usually
achieved by having a tilt angle on the condenser or a specific
shape. Fourth, a hydrophilic surface is needed to recover most of
the water, so it can be collected in a container, and to avoid
evaporation of the water in the early morning. Finally, it is
important to have a light condenser to reduce heat inertia, making
it easier to change the temperature of the surface, and to have
good insulation to avoid heat transfer from the ground (Beysens et
al. 2006, 2007; Clus et al. 2009). This said, it is possible to
divide the optimization factors of the design and location of
radiative systems into the material, shape, and size of the
collector, and its position.  
  
**Surface material**  
Dew formation is influenced by the properties of the material used
for the surface of the condenser. By selecting the appropriate
material, the energy barrier at the liquidavapor interface can be
lowered to enhance water recovery. Alnaser and Barakat (2000)
tested three different types of materials and the results showed
that aluminum had the highest potential use as a dew water
collecting surface, followed by glass and polyethylene. They came
to the conclusion that a polished surface enhances dew collection
by letting the water easily run along the surface. Kidron (2010)
found that a smooth Plexiglas surface collected 0.21 L/m2/day of
dew water, compared to a rough surface that collected 0.1
L/m2/day.  
  
Another property that affects dew condensation is the mass of the
material, which affects the ability of the condenser to lower its
temperature, since condensers with a higher mass have higher
thermal inertia. For this reason, insulation beneath the condenser
is necessary to prevent heat transfer between the soil (or the
condenser frame) and the surface sheet of the dew condenser
(Beysens 1995; Nikolayev et al. 1996). For example, a study in
North West India of plain, uninsulated corrugated galvanized iron
roofs measured a maximum cooling temperature of 2 A degC, while a
condenser that was thermally insulated using a foil with a higher
emissivity had a maximum cooling of around 3.4a3.7 A degC.  
  
In addition to being light, having high wetting properties, and
being thermally insulated from the ground, the condenser material
needs to have a high emittance in the infrared region of the
spectrum to enhance its cooling properties (Alnaser and Barakat
2000). The standard foil recommended by the International
Organization for Dew Utilization (OPUR) is a white hydrophilic
foil of titanium dioxide and barium sulfate microspheres embedded
in polyethylene. The OPUR standard foil is said to improve
emitting properties in the near infrared region by providing
radiative cooling at normal ambient temperatures. At the same
time, it reflects visible light, thus increasing the time for dew
collection in the early morning. Maestre-Valero et al. (2011)
compared the standard white hydrophilic foil recommended by the
OPUR (yield 17.36 L) with a low-cost black polyethylene foil (BF)
used for mulching in horticulture (yield 20.76 L). The OPUR foil
and BF foil had the same emissivity in the wavelength of 7a14 Aum
(e = 0.976). However, the BF had a higher emissivity in the
wavelength of 2.5a7 Aum (BF: 0.996; OPUR foil: 0.833) and 14a25 Aum
(BF: 0.998; OPUR foil: 0.990). The better performance of the BF
showed that the increase of emissivity in the infrared spectrum
resulted in a higher yield than an increase in the surface
hydrophilic properties. This indicates the importance of the
emittance of the material, with high emittance being needed not
only in the near infrared spectrum but also in the entire
mid-infrared spectrum (Maestre-Valero et al. 2012).  
  
**Shape**  
The shape of the dew water collector and its influence on water
yield has been studied in terms of simple hollow structures and
non-plane sheets. Dew collection from hollow funnel-like
structures showed an increase in the collector efficiency compared
to a 1 m2 standard planar collector. This standard collector is a
polyethylene sheet embedded with microspheres of titanium dioxide
and barium sulfate tilted at a 30A deg angle to the horizontal.
Beysens et al. (2012) hypothesized that hollow forms reduced the
heat exchange between the air and the condenser surface by
reducing free convection; it was found that a cone half-angle of
30A deg gave the best results among all the tested inclinations (25A deg,
30A deg, 35A deg, 40A deg, and 50A deg). In a grassland area in the Netherlands,
an inverted pyramid with an angle of 30A deg collected 20 % more water
than a standard 1 m2 planar dew collector (Jacobs et al. 2008).   
  
Similarly, a simulation done under typical meteorological
conditions (i.e., clear sky, ambient temperature of 15 A degC and
relative humidity of 85 %) showed that a funnel shaped condenser
with a half-angle of 30A deg had a higher performance by 40 % compared
to the reference plate. The funnel shape was found to reduce the
flow of warm air and block the heavier cold air at the bottom,
thus avoiding natural convention (Clus et al. 2009).  
  
Concerning non-planar collectors, three shapes of sheet with
different relief have been tested: egg-box, origami and
multi-ridge. The origami structure compared to the egg-box
structure showed better performance because the egg-box structure
hindered the flow of dew water due to its flat top (Beysens et al.
2012). The multi-ridge condenser did not show any difference in
performance compare to a flat reference condenser, but when the
wind speed increased above 1.5 m/s, the multi-ridge condenser
showed an increase in efficiency of 40 % (Clus et al. 2009).  
  
**Size**  
  
The size of the condenser has been found to influence its
performance. For example, an on-ground 900 m2 condenser showed a
decrease in yield of 42 % compared to four 1 m2 standard
condensers. It was suggested that the large size of the condenser
allowed the foil to fold, which increased water stagnation, thus
affecting the radiative cooling effect (Sharan et al. 2007).
However, Kidron (2010) found that a decrease in size from a 0.16
to a 0.01 m2 condenser reduced the yield from 0.25 to 0.15 L. The
reduction in size on both axes (e.g., from 10 cm by 10 cm to 5 cm
by 5 cm) showed a greater decrease in yield than when one axis was
kept constant (e.g., from 20 cm by 10 cm to 10 cm by 10 cm). This
suggests that there is a border effect that reduces the efficiency
of the condenser surface toward the edges. This issue has not yet
been explored in detail.  
  
**Position**  
  
The position of the dew condenser, in terms of its inclination,
shading and exposure, influences the condensation of water. First,
it was found that an angle of 30A deg with respect to the horizon was
the optimal inclination to minimize the heat exchange effect
caused by wind, increase the water recovery by gravitational force
and not hinder the visibility to the sky that is needed for
radiation cooling. For example, a study in Grenoble, France, found
that when the condenser was inclined at an angle of 30A deg, the yield
of dew water increased by up to 20 % when compared to a nearby
horizontal reference plate (Beysens et al. 2003).  
  
Second, studies of dew condensation showed different results for
condensers in the sunlight and in the shade. For example, an
experiment in Israel showed higher yields in the shaded areas
(Kidron 2000). Furthermore, in north-west India, water
condensation was 35 % higher for a condenser that remained longer
in the shade than for one exposed to sunlight (Sharan et al.
2007).  
  
Finally, studies showed that exposure to the sky also affected
condensation rates by being related to radiative cooling. A site
surrounded by high altitude topography will have the infrared
radiation that the condenser emits reflected back by the hills or
mountains (Beysens et al. 2007). For example, a study comparing an
uphill site with a downhill site showed that the yield from the
latter was 40 % lower than that of the uphill site (Kidron 2000).
In addition, Muselli et al. (2006) showed that a condenser exposed
from the sides had a higher yield (mean dew yield: 0.118 L/day)
than one that was enclosed and closer to the ground (mean dew
yield: 0.111 L/day).  
  
The optimization of radiative condensers allows yield to be
increased by changing the design of the condenser from a flat
plate to more complex shapes and materials. First, an optimal
inclination of 30A deg decreases the heating effect of wind on the
condenser (force convection) and enhances water collection by
gravity. In addition, an inverted hollow structure such as a cone
or pyramid reduces the negative consequences of convection even
further, including free convection. However, producing a hollow
structure is more complicated than producing plane condensers.
Second, the emittance properties of the material can significantly
enhance dew condensation. The standard OPUR sheet has been shown
to increase the cooling of the condensing surfaces; however, since
the sheet is specially manufactured for research purposes, the
cost is quite elevated. Maestre-Valero et al. (2011) studied a
low-cost polyethylene foil that is commonly used in agriculture,
which produced better results than the OPUR sheet. This suggests
that there is further potential to lower the price of the material
used as a surface collector while increasing the efficiency of the
collector. Finally, the scaling up of the condenser from the 1 m2
standard has shown a decrease in efficiency of about 40 % (Sharan
et al. 2007), which does not allow for the collection of high
volumes of dew water.  
  
**Active condensers**  
Given the low yields of radiative condensers and the specific
environmental conditions required for dew formation, active
condensers may be a viable alternative. Although relative humidity
is a significant factor in the efficiency of active condensers
(Peters et al. 2013), active condensers are less affected by
variation in conditions such as sky emissivity, wind speed, and
topographic cover than radiative condensers. Thus, they can
potentially be operational under a wider range of weather
conditions (Peters et al. 2013).  
  
Active condensers can be classified into personal scale devices
that can generate 15a50 L of water per day, or larger industrial
scale machines, which can produce up to 200,000 L/day (Peters et
al. 2013; Khalil et al. 2014). The yield of active condensers is
much higher than of radiative condensers, but active condensers
typically have a high energy demand. Despite this drawback, active
condensers can be useful as a supplementary water source in
circumstances where water supply from other sources is limited,
such as an alternative source of potable water.  
  
Active dew condensers typically use cooling condensation or
regenerative desiccation to bring trapped air to the dew point
temperature, thus causing the water vapor to condense for
collection. Early active condenser technology used simple designs
to maintain collection surfaces at cool temperatures for a longer
period of time than can be achieved in radiative condensers.
Subsequent technological development focused on using regenerative
desiccants, which are subdivided into solar regeneration, heat
exchanger coupled, and dual air pathways, and cooling condensation
technology, which is further divided into ground-coupled,
portable, vehicle compatible and seawater cooling. Each of these
design types has benefits and drawbacks, as discussed below.  
  
**Regenerative desiccant materials**  
Regenerative desiccant technologies use hygroscopic materials
(substances that can attract and hold water molecules through
adsorption or absorption) to increase the volume of dew collected.
Silica gel and zeolite are commonly used in active condensers. The
capacity of hygroscopic materials to hold amounts of water greater
than their own mass theoretically makes the active condensers more
effective at extracting and retaining water than radiative
condensers. Furthermore, low dew points can be achieved without
potential freezing at moderately low operation costs. However,
initial costs of desiccant materials are high and the desiccant
beds must be replaced periodically. Regenerative desiccant
condensers typically include a bed of hygroscopic material that
can be exposed to humid air, and a stimulus source, such as solar
power or heat exchangers, to extract the water content for
collection in built-in or external reservoirs. It should be
emphasized that some apparatuses (e.g., solar regeneration) depend
on solar radiation for heating the desiccant and do not require an
additional source of energy. These apparatuses cannot be
considered as active condensers, but were included in this section
as one of the types of regenerative desiccant condensers.  
  
**Solar regeneration**  
Initial designs of this type consisted of a solid or liquid
desiccant that absorbed water vapor from moist air, which was
subsequently recovered by heating the desiccant and condensing the
evaporated water (Hamed et al. 2010). For example, an apparatus
that used a high surface area of wood exposed to the nighttime air
absorbed moisture of up to 30 % of the dry woodas weight. During
the daytime, the wood was stored in an area with large windows and
glass ceilings to allow the sunas heat to evaporate the moisture
from the wood. The air was then expelled to an area in the shade
where the moisture condensed and was collected in a reservoir. The
air was recirculated back to the wood to carry more moisture and
flow back to repeat the cycle (Altenkrich 1938). Several setups
used different desiccants, such as saw wood (Altenkrich 1938),
silica gel (Dunkak 1949; Ackerman 1968; Hamed et al. 2011), and
recycled newspapers (Krumsvik 1998). For instance, a glass pyramid
shape apparatus with a multi-shelf solar system to extract water
from humid air was explored by Kabeel (2007). Saw wood and cloth
were examined as beds and were saturated with 30 % concentrated
calcium chloride solution. During the night, the pyramid glass
sides were opened to allow the desiccant to absorb moist air and
during the day, the glass sides were closed to extract the
moisture from the bed by solar radiation. Water evaporates and
condenses on the top of the pyramid and is collected through a
middle cone and through the glass inclined sides to an external
reservoir (Fig. 2). The pyramid shape with multi-shelves doubled
the amount of collected water compared with a solar
desiccant/collector system with horizontal and corrugated beds.  
  
**Fig. 2****Glass pyramid with shelves (open during night and closed
during day)**  

![](Fig2.gif)

  
Similar setups have used silica gel contained within a breather,
which is a vented housing that allows air exchange with the
atmosphere due to temperature and pressure differences between the
two. The breather housing was coated with a dull, dark finish to
allow for maximum heat absorption during the day. The heated
silica gel inside was then activated, which allowed release of the
water content, creating warm moist air that flowed out of the
breather and condensed. The gel sat on a slotted bed, which was
sufficient to allow it to collect moisture during the night-time
(Dunkak 1949). Similar mechanisms can be found in different
designs, such as several cone shaped thin sheets of metal stacked
vertically with a desiccant in the middle. During the night, the
ends of the metal sheets were raised so that the desiccant was
exposed to the cool, moist air, and condensed during the day
(Ackerman 1968). Recycled newspapers have also been used as
desiccants housed in glass pyramid chambers (Krumsvik 1998).  
  
Collectors with regenerative desiccant materials have been
designed for use in a wide range of environments, and have been
optimized by altering the desiccant used and the design of the
collector. For example, for humid tropical regions with large
temperature differences, Groth and Hussmann (1979) described a
device comprising a glass sun-ray collecting top layer, followed
by a coarse, granular silica gel absorbent layer, followed by a
layer of non-absorbent materials, such as stones, that was stacked
3a5 m high (Fig. 3). At the bottom, fans supplied and withdrew
air. This device could be 100a200 m in width and up to 15 m in
length. Cool, moist nighttime air was channeled from the bottom up
so that it passed the non-absorbent layer and cooled before
reaching the absorbent layer, where water adsorbed to the silica.
During the day, hot air flowed in the reverse order and reverse
direction. The moisture desorbed from the silica gel flowed
downwards into the stones (heat exchange layer) and condensed on
contact with the cool surface, then flowed into a reservoir. The
air flow in this phase could also be aided by a radiator (Groth
and Hussmann 1979). This structure could collect 10a15 L of water
per square meter of adsorbing surface over 24 h.  
  
**Fig. 3****A simplified illustration of the device proposed by Groth
and Hussmann (1979)**

**![](Fig3.gif)**

  
For application on a larger scale in desert regions, Klemic (2005)
detailed an apparatus containing a frame 1a6 m high, which held a
net of superabsorbent polymer, preferably of a grain size of
50a1000 microns. This polymer was capable of absorbing moisture of
several times its own weight, which was released with the
application of solar power. The condensate water was collected in
a trough located directly below the net. This device can be used
for fog clearance and odor removal in addition to water
generation, and the frame can be built from local, widely
available materials.  
  
**Heat exchanger coupled desiccants**  
  
Regenerating desiccant beds with heat exchangers removed the time
constraints associated with solar power and led to more control
over the amount of energy supplied to regenerate the desiccants.
For example, Michel and Bulang (1981) described an apparatus
containing a sun collector, an adsorbent layer with a desiccant
bed, and an air baffle, followed by a condenser (Fig. 4). A grated
collection reservoir was located below the condenser, as well as
fans below the sun collector to channel air through. Air intake
was in the air baffle zone, which was open during the night to
contain air inside. Upon entry, the air flow was split into two,
with one partial air stream being channeled through the condenser
and heat storage reservoir to cool it. The second stream is
directed into the adsorbent layer, where its moisture was
adsorbed. The two streams connected before exiting through the air
outlet port. In the daytime phase, the water was desorbed and
condensed. The air flaps were closed and mirrors concentrated sun
rays to heat the air inside. Heating the adsorbent released
moisture to two streams of air. One went down to the condenser
layer and relinquished some of the moisture, which condensed as
water droplets and was heated in the process. The warm air was
recycled back through the adsorbent layer and continued to pick up
more moisture. Ito et al. (1981) described similar designs with
multiple desiccant beds.  
  
**Fig. 4****A visual representation the aforementioned apparatus
described by Michel and Bulang (1981). Air stream represents the
first air stream that is directed through the condenser and heat
storage reservoir and Air stream 2 represents the partial air
stream that is directed through the absorbent material**

**![](Fig4.gif)**

**Dual air paths and chambers**  
Newer designs with regenerative desiccants used multiple pathways
and chambers, the purpose of which was to maximize moisture
extraction and increase the efficiency of batch processing. Such
designs included portable sized devices that could be coupled to
mobile energy sources, such as automobiles. For example, Tongueas
(2007) desiccant wheel required a heat source such as that from a
vehicle exhaust to provide heat to an air loop, where a heat
exchanger heated the air within the loop. On one side of the loop
was dry air and on the other was the humid air passage. The moist
air in the second passage flowed to a condenser, from where the
subsequent condensate dripped through a pipe to a reservoir, where
it was filtered further before being dispensed (Call et al. 2009).
An air blower channeled ambient air into a desiccant bed, the air
from which was then released via heat from an energy conversion
device. With the addition of heat, the high temperature, high
humidity air was desorbed, passed over a condenser and collected
as water droplets. The energy conversion device can be excess heat
from a vehicleas motor.  
  
Rodriguez and Khanji (2012) described another dual chambered
device that incorporated a water treatment step. The closed
chamber received air funneled in through fans, which was then
heated to 75a82 A degC and exposed to a desiccant that had been
pre-absorbed with moisture from the ambient air. The hot air was
humidified and then passed over condenser coils, which collected
water condensate that dripped into a collection tank. The computer
control extra heated the desiccant once per day to decontaminate
it, and ambient air from the open air chamber was infused within
it to supply the moisture. The collected water was exposed to UV
light and then pumped through filters containing carbon and zinc
or silver activated zeolite, before being collected in a final
reservoir that rested on Peltier plates to allow the water to cool
before dispensing. Water sensors could shut off or shift the
output of processed water when the reservoirs were full. Ellsworth
(2013) described a desiccant that included porous support material
and hydroscopic absorbent dispersed within the support material.
Materials such as PVA foam with calcium chloride as a chemical
desiccant resulted in increased moisture adsorbing properties.  
  
**Cooling condensation systems**  
  
The second common class of active condensers contain the
components of a refrigeration system to provide a cooled surface
for condensation to occur, such as in a reverse cycle air
conditioner (Graham and Dybvig 1946). These devices often contain
a compressor, condenser, and evaporator connected by conduits that
carry a refrigerant. These, in addition to pressure valves, air
inlets and outlets, and water reservoirs, are generally housed in
a rectangular container. The advantages offered by this approach
include low initial costs, and low operating and maintenance
costs. In addition, the refrigeration mechanism allows for dew
collection even at times when the ambient temperature is greater
than the dew point temperature, potentially making them more
efficient than radiative condensers. The disadvantages include
potential icing of evaporator coils and low cost-effectiveness
during periods of low air flow. However, these problems have been
addressed in newer models by insulation and programmable cycling
compressors, respectively.  
Designs using cooling liquids  
  
Coanda and Coanda (1956) described a housing with orientable entry
and exit points for wind, located near large water bodies, where
warm, moist air is prevalent. Inside the housing was the first
cooling radiator coil, which was connected via conduits to a
second coil located beneath the soil surface that was in contact
with cooler temperatures. A cooling liquid was driven through the
coils by a windmill. The warm air entering the housing was cooled
as it flowed through the coils, such that condensed water droplets
flowed down the coils and were piped via conduits into a
dispensing reservoir.  
  
Portable atmospheric water generators also use cooling liquids to
acquire potable water from ambient air of varying temperature and
humidity conditions, and typically generate between 20 and 50 L of
water per day. They also contain built-in filtration systems that
remove the need for separate water treatment, making them an asset
to regions without such infrastructure. Air is funneled into the
device via fans through an air filter that screens out debris.
Inlet air passes through evaporator and condenser coils aided by a
compressor to remove the water vapor by condensation from the air.
Evaporators induce liquid refrigerant vaporization, allowing the
air to cool the air and the water to condense into a reservoir for
collection. A compressor and condenser allow the refrigerant to
return to its liquid state. The condensate is collected on a
collecting pan and channeled into a reservoir where UV light is
applied to kill 99.9 % of microorganisms (Reidy 1992a, b). Once
sufficient water has collected, it is passed through a water
filter into a second reservoir where secondary UV light exposure
is applied. Processing is halted if either of the UV lights
malfunction or when filters require replacement or cleaning, as
detected by an air pressure sensor. Sensors detect and stop water
output once the external or internal containers are full and the
flow of water can be shifted to secondary containers (Reidy 1992a,
b).  
  
A programmable microchip set can be used to operate the generator.
In addition to being programmed to display alerts during
compromised operations, such as when the air filters need
replacing, the microchip can be coupled to a thermostat and
humidistat. These can be programmed to process air of a given
temperature and humidity level so as to maximize the water yield
for a given amount of energy needed to operate the generator. For
example, at 24 A degC and 50 % relative humidity, up to a 3.79 L of
water can be produced within 12 min (Reidy 1993). Similar designs
incorporate ionic air filters and activated charcoal water filters
to remove volatile organic compounds, and heat strips to prevent
freezing of water when atmospheric temperatures drop below 0 A degC
(LeBleu 1997, 1998).  
  
Subsequent designs allowed the collected water to be cooled or
heated, as well as to be recirculated to prevent stagnation.
Insulation and heating measures were also added to prevent rusting
and icing of the condensing coils (e.g., Zakryk 2000; Lloyd and
Baier 2002). Design modifications to prevent stagnation included a
spinning reservoir that was cylindrical at the top and conical at
the bottom; the vortex created by the spinning water prevented
stagnation and accumulation of sediment. Additional forms of
filtration included melamine deep filters and charcoal black
filters. The water was chilled or heated and pumped to be
dispensed from a spout located at the top (Dagan 2003). Water
dispensing can be either gravity assisted or accomplished through
the use of small pumps (Faqih 2004). Versatile designs can be a
standalone indoor or outdoor unit, wall-mounted, mobile or
attached to a vehicle (Engel and Clasby 2004; Foss 1973).  
  
**Ground-coupled heat exchangers**  
  
The ground can also be used as a heat sink to naturally induce
condensation. However, one disadvantage of this approach is that
underground tubes are susceptible to contamination and are
difficult to clean. Courneya (1982) described an apparatus that
contained a cold heat exchanger buried beneath the surface of soil
or a body of water that was at or near subsurface temperature. An
above ground, water collecting funnel channeled air into the
system, through the heat exchanger, out through the outlet valve,
and into a reservoir that collected the condensate. The outlet
valve could be regulated to increase residence time of the air
inside the heat exchanger to allow for sufficient condensate to
form. OaHare (1984) described a simpler apparatus that operated by
the same principle with solely a blackbody pipe that extended
beneath the surface (Fig. 5). In addition, Smith (1984) described
a housing with a turbine and evaporator conduit. The turbine was
connected to an electrical generator that powered the
refrigeration system. The unit was mounted on a tower such that it
automatically rotated to point toward the wind. The cooling of the
evaporator caused the air to sink and leave the unit at a lower
position to where it entered, leading to denser air. A similar
design contained a chamber located 6' below the surface, which
contained fans that helped circulate air within several conduits.
When air temperature is higher or lower than ground temperature, a
gradient is established and water is trapped and condensed (Rogers
and Midgett 1980).  
  
**Fig. 5****An illustration of OaHareas (1984) ground-coupled heat
exchanger apparatus with the rotatable turbine tower introduced
by Smith**

**![](Fig5.gif)**

**Seawater cooling**  
  
Cravenas (2008) invention generated fresh water from deep cold
ocean water at altitudes above sea level (Fig. 6). It included a
first stage with a siphon, collecting tank and supporting
structure. The irrigation piping in the siphon transported the
deep ocean water high up the insulated irrigation pipe condenser,
which retained the coolness of the water, and allowed the air
outside to condense onto it. The layered irrigation pipes were
made of materials with properties that allow them to function as a
heat exchanger.  
  
**Fig. 6****Cravenas seawater cooling system (Craven 2008). The top
figure represents an aerial view, while the bottom figure
illustrates a profile view of the system**

**![](Fig6.gif)**

**Cooling using dual airflows**  
  
Bulang (1980) described a device that took moist nighttime air and
divided it into two partial air flows. The first partial air flow
passed through a water-absorbing material, such as silica gel. 75
g of water could be absorbed for 100 g of the silica gel. The
second partial gas flow passed through a heat accumulator where
heat was transferred to it. The accumulator was deheated and the
second partial gas flow was discharged. In the second stage during
the daytime, a flow of moist gas that had been heated by a
solar-energy collector was passed through the moisture laden water
absorber from step 1. This gas flow absorbed the moisture from the
absorber, creating a second warmer and more humid gas flow. This
gas was passed over the deheated heat accumulator, where heat was
transferred to the accumulator and moisture condensed on its
surface. The flow of gas was discharged and the condensate was
collected. Hussmannas (1982a, b) similar device used four stages.
In the first stage cool humid atmospheric air was used to cool the
first heat condenser and moisten an adsorbent medium. In the
second stage, warm solar heated air was used to expel moisture
from the adsorbent and carry the moisture into the first heat
storage condenser, where the moisture condensed and released its
heat. In the third stage, a second stream of cool humid air was
used to cool the second heat condenser and moisten the first
adsorbent. In the fourth phase, a second stream of warm solar
heated air was used to harness moisture from the adsorbent and
condense it over the second heat storage condenser. The stream of
air in the second phase was preheated by the second heat storage
condenser from the fourth phase. The stream of hot air in the
fourth phase was preheated by the first heat storage condenser, in
addition to solar radiation, and this heat was also used to expel
all moisture from the adsorbent.  
  
**Other methods**  
Ockert (1978) proposed the aTornooka device, which was a tall
stack with an extended base (Fig. 7). Air intake was through the
base, which contained inlets that imparted a rotational velocity
to the air. The resulting air had a reduced pressure and the
density difference aided in continuing the flow. This also led to
rapid moisture loss from the air, which was precipitated due to
the centrifugal force in the vortex. The remaining air was heated
to be released from the top of the stack, and the resulting
pressure differential allowed for new air to enter from the base.
High humidity resulted in a stronger vortex.  
  
**Fig. 7****A conceptual profile view of the Tornook device Ockert
(1978)**

**![](Fig7.gif)**

  
Peltier systems, which consist of a unit that transfers heat from
one side to the other powered by electricity, have been used to
provide water directly to plants for irrigation. Biancardi (1982)
described a Peltier system that contained a housing, a
condensation member and a pair of electrical probes. The probes
were stuck in the soil such that the condensation member resided
above the soil. In addition, a thermocouple such as a Peltier
crystal, which contains a hot and cold side when electricity is
conducted, was included. The hot side contained a heat sink and
the cold side contained a conductor that removed heat from the
conduction member, making it cooler. The cooled conduction member
allowed condensation of moisture from the atmosphere; this
condensation was then channeled into a small collection reservoir
and subsequently into the soil (MuA+/-oz-GarcA-a et al. 2013). The
electricity source for the system could be a battery or an AC
current source. Similarly, Tircotas (1985) apparatus utilized the
Peltier effect and had a hot end that was in contact with a heat
dissipater and a cold end in contact with a thermally insulated
condenser powered by an AC current (Fig. 8). Air entered the
chamber and induced the condensation of water into droplets that
were collected in an external reservoir. A fan and thermometer can
also be used to force air and detect temperatures inside the
chamber to ensure adequate processing.  
  
**Fig. 8****Conceptual representation of Tircotas Peltier system**

**![](Fig8.gif)**

**Large-scale designs**  
Faqih (2005) offered several prototypes for collecting water for
human, animal and irrigation purposes using flat, vertical or
conical condensation surfaces. Evaporator coils were installed
behind the condenser surfaces, where humid air lost moisture on
contact with the surface; the condensation collected on these
surfaces dripped down into a collection pan. The water could then
be filtered and appropriated for use. These devices used
thermo-acoustic engines, which use high intensity sound waves to
generate superhot gas molecules that transfer their energy to
coils and then expand and cool, rather than standard refrigeration
systems.  
  
**Implications for optimization and use of active condensers**  
  
Regions where low technology systems are more appropriate tend to
use passive radiative condensers or solar-energy based
regenerative desiccant condensers. However, active condensers may
prove useful in regions and situations where conventional sources
of water are not available and a higher yield is required, such as
for providing potable water for isolated communities in arid
regions or insular areas. The usefulness of active condensers
depends on their design and intended application. For instance,
active condensers using cooling condensation technology generally
provide the benefit of being more portable than regenerative
desiccation systems. Traditionally, desiccants allowed for
function of condensers at lower dew point temperatures because
there was no concern that the condenser coils would freeze.
However, insulation and programmable chipsets have allowed for the
design of condensers that can remain functional at lower
temperatures as well as perform within certain temperature ranges,
so as to be more efficient depending on the local climate. The
trend in regenerative desiccants has been to couple them with heat
exchangers to improve their regeneration capabilities and enhance
the yield.  
  
Milani et al. (2011) estimated that 95 % of the water costs of
such technology can be attributed to energy consumption rather
than the capital costs of the active condenser technology.
However, this is difficult to quantify, as energy consumption
varies with the design of the condenser. For example, a life-cycle
assessment of active condensers in comparison to refrigerators has
shown that active condensers powered by conventional,
non-renewable energy sources consume more electricity for
operation than refrigerators. In addition, active condensers
powered by conventional sources of energy require 4a8 L of virtual
water to produce one liter of potable water, excluding condensed
vapor, based on the source of power (99 % of this water is a
consequence of coal washing and power station cooling operations
used to provide electrical power) (Peters et al. 2013). The high
energy consumption also raises environmental concerns related to
emission of greenhouse gases. For example, active condensers
produce nearly three orders of magnitude more greenhouse gases
than seawater desalination plants (Peters et al. 2013). It should
be emphasized that these analyses were based on active condensers
that were powered by conventional electricity sources.  
  
Given that 99 % of the water use and greenhouse gas emissions of
active condensers are associated with the power supply, the
obvious way to improve these generators is to utilize renewable
sources of energy, such as wind or solar. With such a power
supply, the active condensers would significantly outperform sea
water desalination plants on greenhouse emissions. Overall, it is
likely to be environmentally safer and more cost-effective to
utilize active condensers powered by renewable energy sources.
Although including a solar power unit to provide the power
required for active condensers will increase the capital cost, the
operation costs as well as the cost per liter will be reduced
significantly.  
  
Khalil et al. (2014) suggested an independent dew water irrigation
system (IDWIS), which consists of four main components: a solar
power unit, active condenser(s), water reservoir, and a drip
irrigation system. The design of the IDWIS consists of four steps.
First, the irrigation demand is computed based on the area
cultivated and the crop type. Second, the reservoir is designed to
store the amount of water required for the maximum irrigation
event. Third, the number of condensers is identified based on the
amount of water required for the maximum irrigation event and the
productivity of a single condenser. Fourth, the solar power unit
is designed based on the energy required for the number of
condensers identified in the third step.  
  
Other designs utilize seawater to enhance cooling and to reduce
the energy demands of cooling condensation condensers. The
seawater greenhouse prototype may be a useful tool to better
understand the enhanced cooling by means of seawater (Wahlgren
2000). This prototype uses cool seawater that is pumped into a
greenhouse and channeled between a condenser and evaporators to
enhance the cool and humid conditions in the greenhouse that are
required for plant growth, as well as to produce fresh water
condensate. There are certain constraints to this technology,
including that the location must be coastal, capital costs are
high, and water is relatively expensive at the rate of
$0.005a0.012/L (Wahlgren 2000). However, these costs can be
attenuated by selling the products grown inside the greenhouse for
a profit.  
  
Overall, although water production from active condensers remains
relatively costly at present, active condensers are still
beneficial in appropriate situations and there are several
promising developments in their design that overcome key
shortcomings of earlier models. However, while technological
development has been extensive, little research has been conducted
into design optimization for particular conditions to maximize
yield. The reliability of coupled renewable energy sources and
other alternative cooling mechanisms has also not been evaluated.
These issues must be explored further for active dew condensers to
be a reliable source of water in regions where supply and quality
of water from other conventional sources are poor.  
  
**Conclusion**  
  
Dew forms on surfaces when the surface temperature is lower than
the dew point temperature. For water condensation to occur; there
are several environmental conditions that must be met. A high
relative humidity, high sky visibility to infrared radiation, and
low wind speed are required, which therefore means that the
volumes of dew formed are highly variable. Radiative dew
condensers rely solely on the physical processes that induce dew
formation naturally. To maximize water condensation without any
external source of energy, radiative condensers can be optimized
in terms of their shape, size, material (hydrophilic properties,
mass, infrared emittance), and position (inclination, shading, sky
exposure, and orientation). Such condensers are an interesting
source of alternative water because they do not require any
additional energy input, and the highest yields collectedaup to
0.6 mm/day/m2aare predominantly in regions of water scarcity (arid
and semi-arid regions). Despite optimization, radiative condensers
are still highly dependent on the weather conditions, making this
a relatively unreliable source of water. In addition, yields will
remain low, since the scaling up the condenser size from 1 m2 has
been found to decrease efficiency.  
  
Compared to radiative condensers, active condensers are more
efficient, with daily yields proven to be considerably higher
(e.g., 15a50 L/day for a small portable drinking water unit).
Active condenser technology takes two main forms: regenerative
desiccant materials and cooling condensation systems. The first of
the two uses hygroscopic substances that can attract and hold
water molecules, from which water is subsequently extracted using
a specific stimulus such as solar regeneration, heat exchange, or
air paths and chambers. With this type of system, higher volumes
of water can be extracted from the air than can be extracted using
radiative condensers. Cooling condensation systems contain the
components of a refrigeration system to provide a cooled surface
for condensation to occur. Similar to radiative condensers, they
are optimized to lower the temperature of a specific surface to
below the dew point temperature. However, the cooling condensation
systems are able to create a larger temperature difference between
the air temperature and the surface temperature than radiative
condensers.  
  
Thus, active condensers hold promise as an alternative or
supplemental source of water in regions where conventional water
supplies are limited or unavailable, due to the higher yields
produced than those of radiative condensers. Nevertheless, they
are more expensive and tend to have high energy demands. Several
recent innovations offer solutions for reducing the energy
requirements, such as coupling condensers with ground heat
exchangers or vehicles, and using seawater for cooling. In
addition, the majority of activity in relation to active
condensers has been in technological innovation, with research
into their efficiency being relatively limited compared to
radiative condensers. If active condensers are to achieve their
potential, research is needed to evaluate the existing
technologies in terms of yield under different conditions, to
optimize their design and reduce their energy requirements.  
  
**Acknowledgments**  
Financial support provided by Sustainable Project Funds of McGill
University, as well as an NSERC Discovery Grant held by Jan
Adamowski, is acknowledged.  
  
**References**  
  
Ackerman E (1968) Production of water from the atmosphere. US
Patent No. 3400515  
  
Agam N, Berliner PR (2006) Dew formation and water vapor
adsorption in semi-arid environmentsaa review. J Arid Environ
65:572a590  
  
Alnaser WE, Barakat A (2000) Use of condensed water vapour from
the atmosphere for irrigation in Bahrain. Appl Energy 65:3a18  
  
Altenkrich E (1938) Method of gaining water from the atmosphere.
US Patent No. 2138689  
  
Beysens D (1995) The formation of dew. Atmos Res 39:215a237  
  
Beysens D, Milimouk I, Nikolayev V, Muselli M, Marcillat J (2003)
Using radiative cooling to condense atmospheric vapour: a study to
improve water yield. J Hydrol 276:1a11  
  
Beysens D, Ohayon C, Muselli M, Clus O (2006) Chemical and
biological characteristics of dew and rain water in an urban
coastal area (Bordeaux, France). Atmos Environ 40:3710a3723  
  
Beysens D, Clus O, Mileta M, Muselli M, Milimouk I, Nikolayev VS
(2007) Collecting dew as a water source on small islands: the Dew
Equipment for Water Project in Biseva (Croatia). Energy
32:1032a1037  
  
Beysens D, Broggini F, Milimouk-Melnytchouk I, Ouazzani J, and
Tixier N (2012) Dew architectures: dew announces the good weather.
materiality in its contemporary forms: architectural perception,
fabrication and conception, pp 283a292  
  
Biancardi RP (1982) Apparatus and method for automatically
watering vegetation. US Patent No. 4315599  
  
Bulang W (1980) Process and plant for recovering water from moist
gas. US Patent No. 4185969  
  
Bundschuh J, Hoinkins J (2012) Renewable energy applications for
freshwater production. CRC Press, FloridaGoogle   
  
Call CJ, Beckius RC, Merrill EL, Hong SH, Powell M (2009) Method
and apparatus for generating water using an energy conversion
device. US Patent No. 7601206  
  
Clus O, Ortega P, Muselli M, Milimouk I, Beysens D (2008) Study of
dew water collection in humid tropical islands. J Hydrol
361:159a171  
  
Clus O, Ouazzani J, Muselli M, Nikolayev VS, Sharan G, Beysens D
(2009) Comparison of various radiation-cooled dew condensers using
computational fluid dynamics. Desalination 249:707a7012  
  
Coanda H, Coanda MH (1956) Device for obtaining fresh drinkable
water. US Patent No. 2761292  
  
Courneya CG (1982) Apparatus for extracting potable water. US
Patent No. 4351651  
  
Craven JP (2008) Fresh water extraction device. US Patent 7328584,
US Patent and Trademark Office, Washington  
  
Dagan A (2003) Apparatus for extracting potable water from the
environment air. US Patent 6644060  
  
Dunkak EB (1949) Solar activated dehumidifier. US Patent No.
2462952, US Patent and Trademark Office, Washington  
  
Ellsworth J (2013) Composite desiccant and air-to-water system and
method. US Patent No. 8506675  
  
Engel DR, Clasby ME (2004) Apparatus and method for extracting
potable water from atmosphere. US Patent 6755037  
  
Faqih AAM (2004) Apparatus for the production of freshwater from
extremely hot and humid air. US Patent 6684648  
  
Faqih AAM (2005) Production of potable water and freshwater needs
for human, animal and plants from hot and humid air. US Patent
6868690  
  
Foss FD (1973) Humidifier-dehumidifier device. US Patent No.
3740959  
  
Gandhidasan P, Abualhamayel HI (2005) Modeling and testing of a
dew collection system. Desalination 180:47a51  
  
Gindel I (1965) Irrigation of plants with atmospheric water within
the desert. Nature 207:1173a1175  
  
GlAcurrencyser HJ, Ulrich S (2013) Condensation on the outdoor surface of
window glazingacalculation methods, key parameters and prevention
with low emissivity coatings. Thin Solid Films 532:127a131  
  
Graham CD, Dybvig ES (1946) Refrigerating apparatus. US Patent
2401560   
  
Groth W, Hussmann P (1979) Process and system for recovering water
from the atmosphere. US Patent No. 4146372  
  
Hamed AM, Kabeel AE, Zeidan EB, Aly AA (2010) A technical review
on the extraction of water from atmospheric air in arid zones. JP
J Heat Mass Transfer 4(3):213a228Google   
  
Hamed AM, Aly AA, Zeidan EB (2011) Application of solar energy for
recovery of water from atmospheric air in climatic zones of Saudi
Arabia. Nat Resour 2(1):8a17Google   
  
Hussmann P (1982a) Method and apparatus for abstracting water from
air. US Patent No. 4342569  
  
Hussmann P (1982b) Method and apparatus for recovery of water from
the atmosphere. US Patent No. 4345917  
  
Ito T, H Matsuoka, Azuma K, Y Hirayama, N Takahashi (1981) Water
producing apparatus. US Patent No. 4304577  
  
Jacobs AFG, Heusinkveld BG, Lucassen DC (1998) Temperature
variation in a class A evaporation pan. J Hydrol 206:75a83  
  
Jacobs AFG, Heusinkveld BG, Berkowicz SM (2008) Passive dew
collection in a grassland area, The Netherlands. Atmos Res
87:377a385  
  
Kabeel AE (2007) Water production from air using multi-shelves
solar glass pyramid system. Renew Energy 32(1):157a172  
  
Khalil B, Adamowski J, Rojas M, Reilly K (2014) Towards an
independent dew water irrigation system for arid or insular areas.
Proceedings of the ASABE international annual meeting, Montreal  
  
Khalil B, Adamowski J, Ezzeldine M (2015) Dew water collection as
non-conventional source of water. Proceedings of the 22nd Canadian
hydrotechnical conference, Montreal, 29 Apra2 May 2015  
  
Kidron GJ (2000) Analysis of dew precipitation in three habitats
within a small arid drainage basin, Negev Highlands, Israel. Atmos
Res 55:257a270  
  
Kidron GJ (2010) The effect of substrate properties, size,
position, sheltering and shading on dew: an experimental approach
in the Negev Desert. Atmos Res 98:378a386  
  
Klemic J (2005) Atmospheric water absorption and retrieve device.
US Patent No. 6869464  
  
Krumsvik PK (1998) Method and device for recovering water from a
humid atmosphere. US Patent No. 5846296  
  
LeBleu TL (1997) Portable, Potable water recovery and dispensing
apparatus. US Patent 5669221  
  
LeBleu TL (1998) Portable/potable water recovery and dispensing
apparatus. US Patent 5845504  
  
Lekouch I, Lekouch K, Muselli M, Mongruel A, Kabbachi B (2012)
Rooftop dew, fog and rain collection in southwest Morocco and
predictive dew modeling using neural networks. J Hydrol
448a449:60a72  
  
Lloyd DJ, Baier SE (2002) Water generating machine. US Patent
6490879  
  
Maestre-Valero JF, Martinez-Alvarez V, Baille V, Martin-Gorriz B,
Gallego-Elvira B (2011) Comparative analysis of two polyethylene
foil materials for dew harvesting in a semi-arid climate. J Hydrol
410:84a91  
  
Maestre-Valero JF, Ragab R, Martinez-Alvarez V, Bailie A (2012)
Estimation of dew yield from radiative condensers by means of an
energy balance model. J Hydrol 460:103a109  
  
McCabe WI, Smith JC, Hariott P (1993) Unit operation of chemical
engineering, 5th edn. McGraw Hill Chemical Engineering Series  
  
Michel H, Bulang W (1981) Method and apparatus for the recovery of
water from the atmospheric air. US Patent No. 4285702  
  
Milani D, Abbas A, Vassallo A, Chiesa M, Al Bakri D (2011)
Evaluation of using thermoelectric coolers in a dehumidification
system to generate freshwater from ambient air. Chemical Eng Sci
66:2491a2501  
  
Monteith JL, Unsworth MH (1990) Principles of environmental
physics, 2nd edn. Routledge Chapman & Hall Inc., New
YorkGoogle   
  
MuA+/-oz-GarcA-a MA, Moreda GP, Raga-Arroyo MP, MarA-n-GonzA!lez O
(2013) Water harvesting for young trees using Peltier modules
powered by photovoltaic solar energy. Comput Electron Agric
93:60a67  
  
Muselli M, Beyesens D, Milimouk I (2006) A comparative study of
two large radiative dew water condensers. J Arid Environ 64:54a76  
  
Muselli M, Beysens D, Mileta M, Milimouk I (2009) Dew and rain
water collection in the Dalmatian Coast, Croatia. Atmos Res
92:455a463  
  
Nikolayev VS, Beysens D, Gioda A, Milimouk I, Katiushin E, Morel
JP (1996) Water recovery from dew. J Hydrol 182:19a35  
  
OaHare LR (1984) Ground moisture transfer system. US Patent No.
4459177  
  
Ockert CE (1978) Device for extracting energy, fresh water and
pollution from moist air. US Patent No. 4080186  
  
Peters GM, Blackburn NJ, Armedion M (2013) Environmental
assessment of air to water machinesatriangulation to manage scope
uncertainty. Int J Life Cycle Assess 18:1149a1157  
  
Reidy JJ (1992a) Potable air-water generator. US Patent 5106512  
  
Reidy JJ (1992b) Potable water generator. US Patent 5149446  
  
Reidy JJ (1993) Potable air-water generator. US Patent 5203989  
  
Rodriguez F, Khanji NK (2012) Low power atmospheric water
generator. US Patent No. 8118912  
  
Rogers W, Midgett P (1980) Underground heating and cooling system.
US Patent No. 4234037  
  
Shank DB (2006) Dew point temperature prediction using artificial
neural networks. MS thesis, Department of Biological and
Agricultural Engineering, University of Georgia, Athens  
  
Sharan G, Beysens D, Milimouk-Melnytchouk I (2007) A study of dew
water yields on galvanized iron roofs in Kothara (North-West
India). J Arid Environ 69:259a269  
  
Smith RH (1984) Apparatus and method for recovering atmospheric
moisture. US Patent No. 4433552  
  
Tircot M (1985) Apparatus for continuously metering vapours
contained in the atmosphere. US Patent No. 4506510  
  
Tongue S (2007) Water-from-air system using desiccant wheel and
exhaust. US Patent 7251945  
  
Wahlgren RV (2000) Atmospheric water vapour processor designs for
potable water production: a review. Water Resour 35(1):1a22Google
  
  
Xu Y, Yan B, Zhu H, Guan J (2013) Dew condensation monitoring in a
wetland ecosystem in the sanjiang plain. Fresenius Environ Bull
22(5):1351a1356Google   
  
Zakryk JM (2000) Water collection and dispensing. US Patent
6029461, US Patent and Trademark Office, Washington  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0043135400002475**](http://www.sciencedirect.com/science/article/pii/S0043135400002475)[**http://dx.doi.org/10.1016/S0043-1354(00)00247-5**](http://dx.doi.org/10.1016/S0043-1354%2800%2900247-5)**Water Research, Volume 35, Issue 1, January 2001, Pages
1a22**

**Atmospheric water vapour processor designs
for potable water production: a review**  
  
**Roland V. Wahlgren**

**Abstract**  
Atmospheric water vapour processing (AWVP) technology is reviewed.
These processors are machines which extract water molecules from
the atmosphere, ultimately causing a phase change from vapour to
liquid. Three classes of machines have been proposed. The machines
either cool a surface below the dewpoint of the ambient air,
concentrate water vapour through use of solid or liquid
desiccants, or induce and control convection in a tower structure.
Patented devices vary in scale and potable water output from small
units suitable for one personas daily needs to structures as large
as multi-story office buildings capable of supplying drinking
water to an urban neighbourhood.  
  
Energy and mass cascades (flowcharts) are presented for the three
types of water vapour processors. The flowcharts assist in
classifying designs and discussing their strengths and
limitations. Practicality and appropriateness of the various
designs for contributing to water supplies are considered along
with water cost estimates. Prototypes that have been tested
successfully are highlighted.  
  
Absolute humidity (meteorological normals) ranges from 4.0 g of
water vapour per cubic metre of surface air in the atmosphere (Las
Vegas, Nevada, USA) to 21.2 g m-3 (Djibouti, Republic of
Djibouti). Antofagasta, Chile has a normal absolute humidity of
10.9 g m-3. A 40% efficient machine in the vicinity of Antofagasta
requires an airflow of 10 m3 s-1 to produce 3767 l of water per
day. At a consumption of 50 l per person per day, 75 people could
have basic water requirements for drinking, sanitation, bathing,
and cooking met by a decentralized and simplified water supply
infrastructure with attendant economic and societal benefits.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/0022169495029397**](http://www.sciencedirect.com/science/article/pii/0022169495029397)**Journal of Hydrology,Volume 182, Issues 1a4, July 1996,
Pages 19-35**

**Water recovery from dew**  
  
**V.S. Nikolayev, D. Beysens, A. Gioda, I. Milimouk, E.
Katiushin, J.-P. Morel**

**Abstract**  
  
The recovery of clean water from dew has remained a longstanding
challenge in many places all around the world. It is currently
believed that the ancient Greeks succeeded in recovering
atmospheric water vapour on a scale large enough to supply water
to the city of Theodosia (presently Feodosia, Crimea, Ukraine).
Several attempts were made in the early 20th century to build
artificial dew-catching constructions which were subsequently
abandoned because of their low yield. The idea of dew collection
is revised in the fight of recent investigations of the basic
physical phenomena involved in the formation of dew. A model for
calculating condensation rates on real dew condensers is proposed.
Some suggestions for the aideala condenser are formulated.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0169809509000209**](http://www.sciencedirect.com/science/article/pii/S0169809509000209)[**http://dx.doi.org/10.1016/j.atmosres.2009.01.004**](http://dx.doi.org/10.1016/j.atmosres.2009.01.004)**Atmospheric Research, Volume 92, Issue 4, June 2009, Pages
455a463**

**Dew and rain water collection in the
Dalmatian Coast, Croatia**  
  
**M. Muselli, D. Beysens, M. Miletac, I. Milimouk**

**Abstract**  
Passive dew harvesting and rainwater collection requires a very
small financial investment but can exploit a free, clean (outside
urban/industrial zones) and inexhaustible source of water. This
study investigates the relative contributions of dew and rain
water in the Mediterranean Dalmatian coast and islands of Croatia,
with emphasis on the dry summer season. In addition, we evaluate
the utility of transforming abandoned roof rain collectors
(aimpluviumsa) to collect dew water too. Two sites were chosen, an
exposed open site on the coast favourable to dew formation (Zadar)
and a less favourable site in a cirque of mountains in KomiA3/4a (Vis
Island). Between July 1, 2003 and October 31, 2006, dew was
collected two or three times per day on a 1 m2 inclined (30A deg) test
dew condenser, together with standard meteorological data (air
temperature and relative humidity, cloud cover, windspeed and
direction). Maximum yields were 0.41 mm in Zadar and 0.6 mm in
KomiA3/4a. The mean yearly cumulative dew yields were found to be 20
mm (Zadar) and 9.3 mm (KomiA3/4a). Because of its physical setting,
KomiA3/4a represents a poor location for dew collection. However,
during the dry season (May to October), monthly cumulative dew
water yield can represent up to 38% of water collected by
rainfall. In both July 2003 and 2006, dew water represented about
120% of the monthly cumulative rain water. Refurbishing the
abandoned impluviums to permit dew collection could then provide
useful supplementary water, especially during the dry season. As
an example, the 1300 m2 impluvium at PodA!pilje near KomiA3/4a could
provide, in addition to rain water, 14,000 L dew water per year  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0140196305001096**](http://www.sciencedirect.com/science/article/pii/S0140196305001096)[**http://dx.doi.org/10.1016/j.jaridenv.2005.04.007**](http://dx.doi.org/10.1016/j.jaridenv.2005.04.007)**Journal of Arid Environments, Volume 64, Issue 1, January
2006, Pages 54a76**

**A comparative study of two large radiative
dew water condensers**  
  
**M. Muselli, D. Beysens, I. Milimouk**

**Abstract**  
  
In order to improve the yield of dew condensation from atmospheric
vapor, two large (30 m2 in area) insulated plane radiative
condensers, inclined at 30A deg, were installed in Ajaccio (Corsica
island, France; latitude 41A deg55'N, longitude 8A deg48'E). Prototype P1
was elevated such that the underside was open and exposed.
Prototype P2, however, was enclosed on all sides and closer to the
ground. Both used a special radiative foil that enhances dew
formation. The period of observation for P1 was July 22,
2000aNovember 11, 2001, and for P2 was December 10, 2001aDecember
10, 2003. All data were compared with respect to the same
horizontal calibration plate of polymethylmethacrylate (Plexiglas)
placed at 1 m above the ground on a sensitive recording balance.
Water yield of both prototypes were compared and correlated
against meteorological data (cloud cover, relative humidity, wind
speed, condenser temperature and air temperature). Both prototypes
exhibit improved performances when compared with the calibration
plate: more dew days (+16% and +15% for P1 and P2, respectively);
decrease of the humidity threshold (-3% and -4.4% for P1 and P2);
increase of dew yields for wind speeds up to 3 m s-1. A model of
the mass and thermal exchanges with the ambient air was used. Two
adjustable parameters (heat and mass transfer coefficients) are
used in the model. The values of these parameters were found
larger than the values obtained in continental sites where dew
forms with weak wind, thus emphasizing the peculiarities of dew
formation in windy islands. When data are reduced with the
calibration PMMA data, prototype P1 provided average water yields
slightly larger than the enclosed prototype P2, a result that can
be attributed to the influence of surface thermal radiation.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0168169913000306**](http://www.sciencedirect.com/science/article/pii/S0168169913000306)[**http://dx.doi.org/10.1016/j.compag.2013.01.014**](http://dx.doi.org/10.1016/j.compag.2013.01.014)**Computers and Electronics in Agriculture, Volume 93, April
2013, Pages 60a67**

**Water harvesting for young trees using
Peltier modules powered by photovoltaic solar energy**  
  
**M.A. MuA+/-oz-GarcA-a, G.P. Moreda, M.P. Raga-Arroyo, O.
MarA-n-GonzA!lez**

  
**Abstract**  
  
Young trees transplanted from nursery into open field require a
minimum amount of soil moisture to successfully root in their new
location, especially in dry-climate areas. One possibility is to
obtain the required water from air moisture. This can be achieved
by reducing the temperature of a surface below the air dew point
temperature, inducing water vapor condensation on the surface. The
temperature of a surface can be reduced by applying the
thermoelectric effect, with Peltier modules powered by
electricity. Here, we present a system that generates electricity
with a solar photovoltaic module, stores it in a battery, and
finally, uses the electricity at the moment in which air humidity
and temperature are optimal to maximize water condensation while
minimizing energy consumption. Also, a method to reduce the
evaporation of the condensed water is proposed. The objective of
the system is to sustain young plants in drier periods, rather
than exclusively irrigating young plants to boost their growth.  
  
**Highlights**  
  
Water can be obtained from the moisture of the air using Peltier
modules... The water obtained by electronic devices can be enough
to save young trees... A computer based controller can optimize
the energy consumption of a water condenser... A photovoltaic
power source supplies more energy when the necessity is higher.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0009250911001059**](http://www.sciencedirect.com/science/article/pii/S0009250911001059)[**http://dx.doi.org/10.1016/j.ces.2011.02.018**](http://dx.doi.org/10.1016/j.ces.2011.02.018)**Chemical Engineering Science, Volume 66, Issue 12, 15 June
2011, Pages 2491a2501**

**Evaluation of using thermoelectric coolers
in a dehumidification system to generate freshwater from
ambient air**  
  
**Dia Milani, Ali Abbas, Anthony Vassalloa, Matteo Chiesa, Dhia
Al Bakri**

**Abstract**  
  
The feasibility of using thermoelectric coolers (TECs) in a
dehumidification system to condense atmospheric moisture and
generate renewable freshwater was investigated. An algorithm was
developed to correlate psychrometric variables at the entrance and
exit of the TEC dehumidification system, determining the amount of
condensable water, required energy and total cost per kL of
generated water. The driving force of condensation is set to be
dynamic to imitate wet-bulb variation at a pre-determined margin.
The influence of relative humidity variation on saturation
temperature, energy consumption, water productivity and the price
of generated water in maximal thermal conditions was also
determined. It found that more than 95% of the water cost was
attributed to energy consumption rather than capital cost of the
dehumidification system. The price of generated water is estimated
to start from $82 per kL and can be integrated and programmed to
top-up rainwater harvesting tanks (RHTs) productivity to entirely
secure end-users freshwater demands. The main attractions of this
approach include compact, safe and noiseless technology that can
provide independent and clean water supply to end-users and
alleviate the stress on freshwater resources and their aquatic
ecosystems.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0022169412005471**](http://www.sciencedirect.com/science/article/pii/S0022169412005471)[**http://dx.doi.org/10.1016/j.jhydrol.2012.06.046**](http://dx.doi.org/10.1016/j.jhydrol.2012.06.046)**Journal of Hydrology, Volumes 460a461, 16 August 2012,
Pages 103a109**

**Estimation of dew yield from radiative
condensers by means of an energy balance model**  
  
**J.F. Maestre-Valeroa, R. Ragabb, V. MartA-nez-Alvareza, A.
Baillea**

**Summary**  
  
This paper presents an energy balance modelling approach to
predict the nightly water yield and the surface temperature (Tf)
of two passive radiative dew condensers (RDCs) tilted 30A deg from
horizontal. One was fitted with a white hydrophilic polyethylene
foil recommended for dew harvest and the other with a black
polyethylene foil widely used in horticulture. The model was
validated in south-eastern Spain by comparing the simulation
outputs with field measurements of Tf and dew yield. The results
indicate that the model is robust and accurate in reproducing the
behaviour of the two RDCs, especially in what refers to Tf, whose
estimates were very close to the observations. The results were
somewhat less precise for dew yield, with a larger scatter around
the 1:1 relationship. A sensitivity analysis showed that the
simulated dew yield was highly sensitive to changes in relative
humidity and downward longwave radiation. The proposed approach
provides a useful tool to water managers for quantifying the
amount of dew that could be harvested as a valuable water resource
in arid, semiarid and water stressed regions.  
  
**Highlights**  
  
Surface temperature and dew yield of RDCs are estimated from the
energy balance... Surface emissivity and emitted radiance are two
key parameters when modelling dew... The applied filter was an
appropriate strategy for a good performance of the model... Dew
yield is very sensitivity to the meteorological input
variables/parameters... Our energy balance model explained about
70% of the total variance of dew.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0022169411006470**](http://www.sciencedirect.com/science/article/pii/S0022169411006470)**http://dx.doi.org/10.1016/j.jhydrol.2011.09.012****Journal of Hydrology, Volume 410, Issues 1a2, 15 November
2011, Pages 84a91**

**Comparative analysis of two polyethylene
foil materials for dew harvesting in a semi-arid climate**  
  
**J.F. Maestre-Valero,  V. MartA-nez-Alvarez, A. Baille, B.
MartA-n-GA3rriz, B. Gallego-Elvira**

**Summary**  
This paper analyses the dew collection performance of two
polyethylene (PE) foils in a semi-arid region (Southern Spain).
The dew collecting devices consisted of two commercial passive
radiative dew condensers (RDCs) of 1 m2 tilted to 30A deg. They were
fitted with two different high-emissivity PE foils: a white
hydrophilic foil (WSF) recommended as standard for dew recovery
comparisons by the International Organization for Dew Utilization
(OPUR), and a low-cost black PE foil (BF) widely used for mulching
in horticulture. Dew yield, foil surface temperature and
meteorological variables (air temperature, relative humidity,
downward long wave radiation and wind speed) were recorded hourly
during a 1-year period from May-2009 to May-2010. The spectral
emissivity of the foils was determined in laboratory in the range
2.5a25 Aum and the radiance-weighed values were calculated over
different intervals, indicating that BF emitted more than WSF,
especially in the range 2.5a7 Aum. Dew yield was well correlated
with the air relative humidity and foil net radiation in both
foils and was hardly detected when the relative humidity was lower
than 75% or the wind speed higher than 1.5 m s-1. WSF was more
sensitive to dew formation due to its hydrophilic properties,
registering more dewy nights (175) than BF (163) while the annual
cumulative dew yield for BF was higher (20.76 mm) than for WSF
(17.36 mm) due to the higher emissivity and emitted radiance of
BF. These results suggested that increasing the surface emissivity
over the whole IR spectrum could be more effective for improving
RDC yield performances than increasing the surface hydrophilic
properties. On a practical point of view, BF could be considered
as a suitable material for large scale RDCs, as in our study it
presented several advantages over the reference material, such as
higher dew collection performance, longer lifespan and much lower
cost.  
  
**Highlights**  
We compare the performance of two polyethylene foil materials for
dew harvesting... Dew was well correlated with the air relative
humidity and foil net radiation... Black foil (BF) was more
productive...Surface emissivity and hydrophylic properties are two
key parameters... Our empirical relationship explained about
two-thirds of the total variance of dew.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0022169412002673**](http://www.sciencedirect.com/science/article/pii/S0022169412002673)[**http://dx.doi.org/10.1016/j.jhydrol.2012.04.004**](http://dx.doi.org/10.1016/j.jhydrol.2012.04.004)**Journal of Hydrology, Volumes 448a449, 2 July 2012, Pages
60a72**

**Rooftop dew, fog and rain collection in
southwest Morocco and predictive dew modeling using neural
networks**  
  
**Imad Lekoucha,  Khalid Lekouch, Marc Musellic, Anne
Mongruel, Belkacem Kabbachi, Daniel Beysens**

**Summary**  
  
Two coastal sites were investigated in an arid region of southwest
Morocco to determine the amount of dew, fog and rain that could be
collected from rooftops for household use. Systematic measurements
were performed in Mirleft (43 m asl, 200 m from the coast) for 1
year (May 1, 2007 to April 30, 2008) and in Id Ouasskssou (240 m
asl, 8 km from the coast) for three summer months (July 1, 2007 to
September 30, 2007). Dew water was collected using standard
passive dew condensers and fog water by utilizing planar fog
collectors. The wind flow was simulated on the rooftop to
establish the location of the fog collector. At both sites, dew
yields and, to a lesser extent, fog water yields, were found to be
significant in comparison to rain events. Mirleft had 178 dew
events (48.6% of the year, 18 A+/- 2 L m-2 cumulated amount) and 20
fog episodes (5.5% of the year, 1.4 L m-2 with uncertainty
-0.2/+0.4 L m-2 cumulated amount), corresponding to almost 40% of
the yearly rain contribution (31 rain events, 8.5% of the year, 49
A+/- 7 mm cumulated amount). At Id Ouasskssou there were 50 dew
events (7.1 A+/- 0.3 L m-2, 54.3% frequency), 16 fog events (6.5 L
m-2 with uncertainty -0.1/+1.8 L m-2, 17.4% frequency) and six
rain events (16 A+/- 2 mm, 6.5% frequency).  
  
Meteorological data (air and dew point temperature and/or relative
humidity, wind speed and wind direction, cloud cover) were
recorded continuously at Mirleft to assess the influence of local
meteorological conditions on dew and fog formation. Using the set
of collected data, a new model for dew yield prediction based on
artificial neural networks was developed and tested for the
Mirleft site. This model was then extrapolated to 15 major cities
in Morocco to assess their potential for dew water collection. It
was found that the location of the cities with respect to the
Atlas mountain chain, which controls the circulation of the humid
marine air, is the main factor that influences dew production.  
  
**Highlights**  
Dew, fog and rain data collected over 1 year in two sites of
south-west Morocco... Dew yield is important and amounts to about
40% of rain water... Good correlation of dew data found with only
a very few meteorological data... Artificial neural network (ANN)
predictive model for dew is developed and tested... ANN model to
predict dew in 15 Morocco cities; RH at night controls dew
production.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0960148106000462**](http://www.sciencedirect.com/science/article/pii/S0960148106000462)[**http://dx.doi.org/10.1016/j.renene.2006.01.015**](http://dx.doi.org/10.1016/j.renene.2006.01.015)**Renewable Energy. Volume 32, Issue 1, January 2007, Pages
157a172**

**Water production from air using
multi-shelves solar glass pyramid system**  
  
**A.E. Kabeel**

**Abstract**  
  
The capability of the glass pyramid shape with a multi-shelf solar
system to extract water from humid air is explored. Two pyramids
were used with different types of beds on the shelves. The beds
are saturated with 30% concentrated Calcium Chloride solution. The
pyramid sides were opened at night to allow the bed saturated with
moist air and closed during the day to extract the moisture from
the bed by solar radiation. The bed in the first pyramid was made
of saw wood while it is made of only cloth in the second pyramid
with the same dimensions. The system was experimentally
investigated at different climatic conditions to study the effect
of pyramid shape on the absorption and regeneration processes.
Preliminary results have shown that the cloths bed absorbs more
solution (9 kg) as compared to the saw wood bed (8 kg). Adopting
this approach produces 2.5 L/day m2. The use of the pyramid shape
with four glass surfaces and multi-shelves enhances the produced
water by 90a95% compared with solar desiccant/collector system
with horizontal and corrugated beds. Results also show that the
clothes bed has higher productivity than that of saw wood bed by
about 5%. This is due mainly to the greater carrying solution at
the onset of the experimental work. The obtained results may help
in designing more efficient system.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0169809507001950**](http://www.sciencedirect.com/science/article/pii/S0169809507001950)[**http://dx.doi.org/10.1016/j.atmosres.2007.06.007**](http://dx.doi.org/10.1016/j.atmosres.2007.06.007)**Atmospheric Research, Volume 87, Issues 3a4, March 2008,
Pages 377a385****Third International Conference on Fog, Fog Collection and
Dew a Fog and Dew**

**Passive dew collection in a grassland area,
The Netherlands**  
  
**A.F.G. Jacobs, B.G. Heusinkveld, S.M. Berkowicz**

**Abstract**  
  
Passive dew collection experiments were initiated in late 2003 in
the centre of The Netherlands within a grassland area. A specially
designed 1 m2 insulated planar dew collector, set at a 30A deg angle
from horizontal, was covered with a thin (0.39 mm) polyethylene
foil and subsequently replaced with 4 mm polyvinyl chloride. A
second dew collector, in the shape of an inverted pyramid, was
constructed to reduce the view angle to only the nighttime sky. A
simple surface energy-budget model and an aerodynamic model were
used to simulate the dew collected by both collectors. The planar
collector collected about 90% of the dew at the grass cover while
the pyramid collector collected about 1.20% of the grass cover.
The aerodynamic model was able to predict the amount of collector
data to within 50% for the planar collector and 60% for the
inverted pyramid collector. The pyramid collector design was able
to collect about 20% more dew than the inclined planar collector.  
  


---

  
[**http://file.scirp.org/Html/4124.html**](http://file.scirp.org/Html/4124.html)**Natural Resources, 2011, 2, 8-17** **doi:10.4236/nr.2011.21002**

**Application of Solar Energy for Recovery of
Water from Atmospheric Air in Climatic Zones of Saudi Arabia**   
  
**Ahmed M. Hamed, Ayman A. Aly, El-Shafei B. Zeidan**

**Abstract**  
  
In the present work, an investigation on the application of solar
energy to heat a sandy bed impregnated with calcium chloride for
recovery of water from atmospheric air is presented. The study
also aimed at evaluating the effects of different parameters on
the productivity of the system during regeneration. These
parameters include system design characteristics and the climatic
conditions. An experimental unit has been designed and installed
for this purpose in climatic conditions of Ta if area, Saudi
Arabia. The experimental unit which has a surface area of 0.5 m2,
comprises a solar/desiccant collector unit containing sandy bed
impregnated with calcium chloride. The sandy layer impregnated
with desiccant is subjected to ambient atmosphere to absorb water
vapor in the night. During the sunshine period, the layer is
covered with glass layer where desiccant is regenerated and water
vapor is condensed on the glass surface. Ambient temperature, bed
temperature and temperature of glass surface are recorded. Also,
the productivity of the system has been evaluated. Desiccant
concentration at start of regeneration is selected on the basis of
the climatic data of Al-Hada region, which is located at Taif
area, Saudi Arabia. Experimental measurements show that about 1.0
liter per m2 of pure water can be regenerated from the desiccant
bed at the climatic conditions of Taif. Liquid desiccant with
initial concentration of 30% can be regenerated to a final
concentration of about 44%. Desiccant concentration at start of
regeneration is selected on the basis of the climatic data of
Al-Hada region. The climate of Taif city is dry compared with that
for Al-Hada region. This method for extracting water from
atmospheric air is more suitable for Al-Hada region especially
in  the fall and winter.   
   
**1. Introduction**  
Shortage of drinking water is chronic, severe, and widespread in
the regions of Northern Africa, Middle East, and Central and
Southern Asia. The problem of providing arid areas with fresh
water can be solved by the following methods [1]:     
  
transportation of water from other locations;   
  
desalination of saline water (ground and under-   
ground);   
  
extraction of water from atmospheric air.   
  
Transportation of water through these regions is usually very
expensive, and desalination depends on the presence of saline
water resources, which are usually rare in arid regions.
Atmospheric air is a huge and renewable  reservoir of water.
This endless source of water is available everywhere on the earth
surface. The amount of water in atmospheric air is evaluated as
14000 km3, whereas the amount of fresh water in rivers and lakes
on the earth surface is only about 1200 km3 [2]. The extraction of
water from atmospheric air has several advantages compared with
the other methods. The extraction of water from atmospheric air
can be accomplished by different methods, the most common of these
methods are cooling moist air to a temperature lower than the air
dew point, and absorbing water vapor from moist air using a solid
or a liquid desiccant, with subsequent recovery of the extracted
water by heating the desiccant and condensing the evaporated
water....     
  


---

  
[**https://www.researchgate.net/profile/Ahmed\_Hamed11/publication/285533435\_A\_technical\_review\_on\_the\_extraction\_of\_water\_from\_atmospheric\_air\_in\_arid\_zones/links/5664970908ae192bbf90a853.pdf**](https://www.researchgate.net/profile/Ahmed_Hamed11/publication/285533435_A_technical_review_on_the_extraction_of_water_from_atmospheric_air_in_arid_zones/links/5664970908ae192bbf90a853.pdf)**JP J Heat Mass Transfer 4(3):213a228**

**A technical review on the extraction of
water from atmospheric air in arid zones.**  
  
**Hamed AM, Kabeel AE, Zeidan EB, Aly AA (2010)**

**[ [PDF](AresEXTRACTIONWATER.pdf)
]**

  


---

  
[**http://www.nature.com/nature/journal/v207/n5002/abs/2071173a0.html**](http://www.nature.com/nature/journal/v207/n5002/abs/2071173a0.html)**Nature 207, 1173 - 1175 (11 September 1965);
doi:10.1038/2071173a0**

**Irrigation of Plants with Atmospheric Water
within the Desert**  
  
**I. Gindel**

  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0011916409008686**](http://www.sciencedirect.com/science/article/pii/S0011916409008686)**Desalination, Volume 249, Issue 2, 15 December 2009, Pages
707a712**

**Comparison of various radiation-cooled dew
condensers using computational fluid dynamics**  
  
**O. Clus, J. Ouazzani, M. Muselli, V.S. Nikolayev, G. Sharan,
D. Beysens**

**Abstract**  
Radiation-cooled dew water condensers can serve as a complementary
potable water source. In order to enhance passive dew collection
water yield, a Computational Fluid Dynamics (CFD) software,
PHOENICS, was used to simulate several innovative condenser
structures. The sky radiation is calculated for each of the
geometries. Several types of condensers under typical
meteorological conditions were investigated using their average
radiating surface temperature. The simulations were compared with
dew yield measurements from a 1 m2 30A deg-inclined planar condenser
used as a reference. A robust correlation between the condenser
cooling ability and the corresponding dew yield was found. The
following four shapes were studied: (1) a 7.3 m2 funnel shape,
whose best performance is for a cone half-angle of 60A deg. Compared
to the reference condenser, the cooling efficiency improved by
40%, (2) 0.16 m2 flat planar condenser (another dew standard),
giving a 35% lower efficiency than the 30A deg 1 m2 inclined reference
condenser, (3) a 30 m2 30A deg-inclined planar condenser (representing
one side of a dew condensing roof), whose yield is the same as the
reference collector, and (4) a 255 m2 multi-ridge condenser at the
ground surface provided results similar to the reference collector
at wind speeds below 1.5 m s- 1 but about 40% higher yields at
wind speeds above 1.5 m s- 1.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0022169408003879**](http://www.sciencedirect.com/science/article/pii/S0022169408003879)[**http://dx.doi.org/10.1016/j.jhydrol.2008.07.038**](http://dx.doi.org/10.1016/j.jhydrol.2008.07.038)**Journal of Hydrology, Volume 361, Issues 1a2, 30 October
2008, Pages 159a171**

**Study of dew water collection in humid
tropical islands**  
  
**O. Clus, P. Ortega, M. Muselli, I. Milimouk, D. Beysens**

**Summary**  
An assessment of the potential for dew water to serve as a potable
water source during a rainless season in a humid tropical climate
was carried out in the Pacific islands of French Polynesia. The
climate of these islands, in terms of diurnal and seasonal
variations, wind and energy balance, is representative of the
climate of the tropical Atlantic and Pacific oceans. Measurements
were obtained at two characteristic sites of this region; a
mountainous island (Punaauia, Tahiti Island) and an atoll
(Tikehau, Tuamotu Archipelago). Dew was measured daily on a 30A deg
tilted, 1 m2 plane collector equipped with a thermally insulated
radiative foil. In addition, an electronic balance placed at 1 m
above the ground with a horizontal 0.16 m2 condensing plate made
of PolyTetraFluoroEthylene (Teflon) was used in Tahiti. Dew volume
data, taken during the dry season from 16/5/2005 to 14/10/2005,
were correlated with air temperature and relative humidity, wind
speed, cloud cover and visible plus infrared radiometer
measurements. The data were also fitted to a model.  
  
Dew formation in such a tropical climate is characterized by high
absolute humidity, weak nocturnal temperature drop and strong
Trade winds. These winds prevent dew from forming unless protected
e.g. by natural vegetal windbreaks. In protected areas, dew can
then form with winds as large as 7 m/s. Such strong winds also
hamper at night the formation near the ground of a calm and cold
air layer with high relative humidity. As the cooling power is
lower than in the Mediterranean islands because of the high
absolute humidity of the atmosphere, both effects combine to
generate modest dew yields. However, dew events are frequent and
provide accumulated amounts of water attractive for dew water
harvesting. Slight modifications of existing rain collection
devices on roofs can enhance dew formation and collection. Dew
harvesting thus appears as an attractive possibility to provide
the local population with a complementary a but on occasion,
essential a water resource.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0360544206002684**](http://www.sciencedirect.com/science/article/pii/S0360544206002684)[**http://dx.doi.org/10.1016/j.energy.2006.09.021**](http://dx.doi.org/10.1016/j.energy.2006.09.021)**Energy, Volume 32, Issue 6, June 2007, Pages 1032a1037**

**Collecting dew as a water source on small
islands: the dew equipment for water project in Bis?evo
(Croatia)**  
  
**D. Beysens, O. Clus, M. Mileta, I. Milimouk, M. Muselli, V.S.
Nikolayev**

**Abstract**  
  
In many regions and geographical settings, dew water collection
can serve as a water source, supplementing rain and fog water
collection. This is particularly useful when precipitation is low
or lacking, especially in remote areas and islands in the dry
season. A project called Dew Equipment for Water (DEW) was
initiated for a 15.1 m2 roof in the island of BiA!evo (Croatia),
equipped with commercial plastic cover selected for its superior
dew collection properties. Measurements of both rain and dew water
will be performed over several years and data will be correlated
with meteorological data collected in situ. Preliminary
measurements during the period 21 Aprila21 October 2005 showed
that dew water contributed significantly, 26% of the total
collected water.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S1352231006002688**](http://www.sciencedirect.com/science/article/pii/S1352231006002688)[**http://dx.doi.org/10.1016/j.atmosenv.2006.03.007**](http://dx.doi.org/10.1016/j.atmosenv.2006.03.007)**Atmospheric Environment, Volume 40, Issue 20, June 2006,
Pages 3710a3723**

**Chemical and biological characteristics of
dew and rain water in an urban coastal area (Bordeaux, France)**  
  
**D. Beysens, C. Ohayon, M. Muselli, O. Clus**

**Abstract**  
  
We report on a 1-year investigation (15 January 2002a14 January
2003) in Bordeaux, France, comparing the quality of dew water with
respect to rain water. The following physico-chemical and
bacteriological properties of dew and rain water were measured:
pH, electric conductivity, cations (Na+, K+, Ca2+, Mg++, Zn++,
Cu++), anions (Cl-, SO42-, NO3-, NO2-), hardness (TH, calcical,
magnesial, permanent), complete alkalimetric title, dry residue
and number of colony-forming unities (CFU) at 22 and 36 A degC. The
CO32-, HCO3-, HPO42- concentrations were found negligible. The
ionic concentrations are in general lower in dew than in rain with
NO2- as a noticeable exception. The mean rain pH (5.4) is lower
than dew pH (6.3). The major ions are from the nearby Atlantic
Ocean (within 50 km). Average ion concentrations are found below
the World Health Organization (WHO) limit requirements for potable
water; dew composition is close to low mineralized commercial
spring waters for the analyzed ions. The biological analyses are
concerned with CFU at 22 and 36 A degC. Dew is seen to exceed on
various occasions the WHO limits.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0022169403000258**](http://www.sciencedirect.com/science/article/pii/S0022169403000258)[**http://dx.doi.org/10.1016/S0022-1694(03)00025-8**](http://dx.doi.org/10.1016/S0022-1694%2803%2900025-8)**Journal of Hydrology, Volume 276, Issues 1a4, 15 May 2003,
Pages 1a11**

**Using radiative cooling to condense
atmospheric vapor: a study to improve water yield**  
  
**Daniel Beysens, Irina Milimouk, Vadim Nikolayev, Marc
Muselli, Jacques Marcillat**

  
**Abstract**  
An inexpensive radiative condenser for collecting atmospheric
vapor (dew) was tested in Grenoble (France). The surface
temperature measurements are correlated with meteorological data
(wind velocity, air temperature) and compared to the corresponding
surface temperature of a horizontal Polymethylmethacrylate
(Plexiglas) reference plate located nearby. The condenser surface
is a rectangular foil (1A0.3 m2) made of TiO2 and BaSO4
microspheres embedded in polyethylene. The foil has an angle ?
with respect to horizontal. The under-side of the device,
thermally isolated, faces the direction of the dominant nocturnal
wind. Both a 2D numerical simulation of the air circulation around
the foil and experimental measurements shows that the angle ?=30A deg
is a good compromise between weak wind influence, large
light-emission solid angle and easy drop collection. The study was
conducted from November 25, 1999 to January 23, 2001. In
comparison to the reference plate, it is found that water yield
can be increased by up to 20% and water collection greatly
facilitated.  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0306261999000549**](http://www.sciencedirect.com/science/article/pii/S0306261999000549)[**http://dx.doi.org/10.1016/S0306-2619(99)00054-9**](http://dx.doi.org/10.1016/S0306-2619%2899%2900054-9)**Applied Energy, Volume 65, Issues 1a4, April 2000, Pages
3a18**

**Use of condensed water vapour from the
atmosphere for irrigation in Bahrain**  
  
**W.E. Alnaser, A. Barakat**

**Abstract**  
  
Atmospheric moisture can be condensed as dew and used for
small-scale irrigation. In Bahrain, we found that the most
favourable conditions for dew condensation persist at dawn. The
maximum amount of dew water can be collected in January and the
least in August. Three condensation surfaces have been tested;
aluminum, glass and polyethylene foils. The average quantity of
dew collected on these surfaces was 1.3, 0.8 and 0.3 kg/m2 per h,
respectively. The condensation rate, water vapour content of the
air, and the dew points of Bahrain's climate have been reported.  
  


---

  
[**http://www.appropedia.org/Dew\_collection\_roof\_retrofit**](http://www.appropedia.org/Dew_collection_roof_retrofit)

**Dew collection roof retrofit**

**Daniel Beysens**

**Abstract**  
  
The problem of obtaining clean drinking water is very widespread
among developing nations. The atmosphere contains an abundant
amount of water in the form of vapor; however it can be difficult
and costly to harvest. Atmospheric water vapor processing (AWVP)
is a new field of research that is developing ways to obtain that
vapor. One such method is known as radiative cooling. A surface
radiates heat away until it drops below the dew point, causing
moisture to condense on the surface. This is a process that occurs
naturally, producing dew. The proposal is to harvest the dew that
naturally forms on rooftops as a source of potable water. Rooftops
made out of galvanized iron, plastic, or glass, in regions that
experience the right weather conditions will naturally produce a
significant amount of dew. Simply by collecting this dew, a family
can gather up to 2L of dew water per dew night. This work offers a
primer to the topic of AWVPs, and a description of how to build a
dew collection rig. Unfortunately, dewfall is not currently
recorded in most standard meteorological archives; so the next
step for this project is to offer a reliable means of regional
assessment that is accessible to a layman.  
  
**Introduction**  
As the worldas population increases, fresh water supplies are
being tapped out. Desalination has become a necessary means of
acquiring water; however current methods are usually quite costly
and use fossil fuels. This is inappropriate for the developing
world, where there is a serious need for increased fresh water
availability. Atmospheric water vapor processing (AWVP) is a new
and emerging technology in which the atmospheric water vapor is
condensed and collected.[1][2][3]  
  
**Operating Principle**  
There is approximately 4 g of water vapor per cubic meter of air
in the earthas atmosphere. This source of potable water is
available virtually worldwide. AWVPs harvest this water, by
condensing it from vapor to liquid.[4][5]  
  
**Advantages**  
  
It is at an early stage in development, but has the potential to
provide environmentally acceptable alternatives to standard water
supplies.[4][5]  
  
Many AWVP designs favor decentralization of water distribution and
avoidance of huge capital costs for infrastructure.[5]  
  
AWVP can be made appropriate, community-managed and
community-maintained for developing countries.[5]  
  
AWVP methods are competitive with desalination plants and simpler
and less expensive to operate and maintain.[5]  
  
The amount of water produced would vary according to installation
size, and be suitable to provide potable water to individuals or
even thousands of people.[5]  
  
AWVP production can take place in a wide variety of locations.
Thus, expensive water distribution infrastructure can be reduced
or avoided.[5]  
  
Chemically, water vapor in the atmosphere is as clean as the air
around it. Naturally occurring dew is a potable source of soft
water, generally low on any mineral content.[6]...  
  


---

  
[**http://www.sciencedirect.com/science/article/pii/S0360544206000168**](http://www.sciencedirect.com/science/article/pii/S0360544206000168)**Energy, Volume 31, Issue 13, October 2006, Pages 2303a2315**

**Application of passive radiative cooling
for dew condensation**  
  
**Daniel Beysens, et al.**

**Abstract**  
  
Dew water was collected from several passive foil-based radiative
condensers established in a variety of geographic settings:
continental (Grenoble, in an alpine valley, and
Brive-la-Gaillarde, in the Central Massif volcanic area, both in
France), French Atlantic coast (Bordeaux), eastern Mediterranean
(Jerusalem, Israel), and the island of Corsica (Ajaccio, France)
in the Mediterranean Sea. In Ajaccio two large 30 m2 condensers
have been operating since 2000. Additional semi-quantitative dew
measurements were also carried out for KomiA3/4a, island of Vis
(Croatia) in the Adriatic Sea, and in Mediterranean Zadar and
Dubrovnik (both in Croatia). Dew potential was calculated for the
Pacific Ocean island of Tahiti (French Polynesia). The data show
that significant amounts of dew water can be collected. Selected
chemical and biological analyses established that dew is, in
general, potable. Continued research is required for new and
inexpensive materials that can enhance dew condensation.  
  


---

  
[**http://www.nrcresearchpress.com/doi/abs/10.1139/er-2015-0035?af=R&#.WCvg-bkoFdg**](http://www.nrcresearchpress.com/doi/abs/10.1139/er-2015-0035?af=R&#.WCvg-bkoFdg)**Environmental Reviews, 2015, 23(4): 425-442,
10.1139/er-2015-0035**

**Dew as a sustainable non-conventional water
resource: a critical review**  
  
**Marlene Tomaszkiewicz, Majdi Abou Najm, Daniel Beysens,
Ibrahim Alameddine, Mutasem El-Fadela**

**Abstract**  
  
Over the last 20 years, dew harvesting has evolved to fruition
because of a better understanding of its physics, thermodynamics,
and the radiative cooling process of condensing substrates.
Although resultant yields are relatively small, dew positions
itself as a viable water resources supplement because it occurs
naturally and frequently in many locations globally, particularly
in the absence of precipitation or when more traditional water
sources are subject to depletion. Moreover, dew water is generally
potable, especially in rural locations, where it is most
beneficial. This review summarizes dew harvesting research
achievements to date including formation processes, collection in
various environments, prediction models, water quality, and
applications. The paper concludes with outlining existing gaps and
future research needs to improve the understanding and performance
of dew harvesting in the context of adaptation to climate change.  
  


---

  

**FR2917417**  
**Use of a composition comprising a polymeric matrix and a
charge containing kaolin, e.g. for radiative cooling of the
coated surface and vapor condensation of the atmospheric
water, and in paints**

  
Inventor(s):     BEYSENS DANIEL; CLUS OWEN; MUSELLI
MARC +  
  
The present invention relates to the general field of materials
used to promote the natural infrared radiative cooling, including
employees in the construction of buildings, or in the automotive
industry. More particularly, the present invention relates to
materials used to achieve evacuation of calories by radiative
cooling or to allow an atmospheric water vapor condensation in the
form of clean liquid water for consumption. We know the importance
should be attached to the energy management to develop means able
to reduce energy costs and increase water resources, including
drinking water in some areas. For this purpose, it is possible to
use natural infrared radiative cooling of certain materials to
evacuate day calories contained within a closed space, and to
condense the night atmospheric moisture in the form of liquid
water .  
  
This is particularly advantageous in relatively arid regions. Such
natural radiative cooling is particularly effective in a spectral
window wavelength of between 8 and 14 m, commonly known in English
sky window, within which the atmosphere emits only low radiation.
The overall radiative received power at day ground level is broken
down into ultraviolet radiation (between 0 and 0.3 m), visible
(between 0.3 m and 0.7 m), near infrared (between 0.7 m and 3 m)
mid-infrared (between 3 and 25 m) and far infrared (over 25 m).  
By day, the atmospheric radiation at long wavelengths (infrared
and far infrared means) represents 22.9% of the aggregate
radiative power. At night, this radiation is 100% of the energy
received. Atmospheric radiation at long wavelengths is the result
of absorption by the atmosphere, especially by water vapor H2O,
carbon dioxide CO2 and ozone 03, extraterrestrial or infrared
radiation emitted by the ground and oceans. The gas then each
re-emit an infrared spectrum according to their chemical
constitution. Ozone, which broadcasts mainly in the spectral
window ranging from 8 to 14 m, emits a weak infrared radiation.
Most of the sky emissivity deficit is therefore observed in this
window. However, at room temperature, the emission spectrum of a
black body has a maximum in the same window or spectral range. It
is therefore conceivable that a material having a high emissivity
on the spectral window ranging from 8 to 14 m can dissipate large
amounts of energy by radiative transfer to the sky which has a
lower temperature due to its low emissivity this beach.  
Day, a material may limit its heating if it has a high emissivity
in the mid-infrared radiation, and in particular on the spectral
window ranging from 8 to 14 m, combined with reflectance of the
relatively large solar energy, for the ultraviolet, visible and
near infrared. The radiative dissipation is especially important
as it is proportional to the temperature of the surface
considered. The natural radiative cooling is therefore involved in
an air conditioning energy savings.  
  
At night, only the atmospheric radiation at long wavelengths
(infrared and far infrared means) is present. It is therefore
possible to cool the materials by several degrees below the
ambient temperature by radiative dissipation of energy. Such
cooling can cause atmospheric water vapor condensation in the form
of liquid water can be recovered. In this field of materials
provided to the radiative cooling and atmospheric water vapor
condensation, known by the scientific article Light scattering
coatings: Theory and application of solar W. E. Vargas et al.
journal Solar Energy Materials & Solar Cells, 54, (1998)
343-350, a white opaque thermoplastic film with high emissivity on
a spectral band ranging from 8 to 13 m which is obtained from a
low density polyethylene ( LDPE) respectively, which is 5% and 2%
by volume of titanium dioxide (TiO2) and by volume of barium
sulfate (BaSO4) relative to the total volume of the polyethylene.
Such a thermoplastic film including major disadvantages include a
main charge based on titanium dioxide which is relatively
expensive, and require a relatively large thickness for its opaque
character and its high infrared emissivity.  
  
This is especially bad for the cost of such a film, and may be
incompatible with mass production. Furthermore, expenses of the
thermoplastic film does not provide a satisfactory resistance to
ultraviolet radiation, which is particularly problematic for a
film to be used outdoors. In another technical field, by US Patent
US 4,075,784 discloses a thermoplastic film obtained from a high
density polyethylene (HDPE) charge of 1 to 15% by weight of
calcined kaolin (Al2O3.2SiO2) by weight total polyethylene,
calcined kaolinite comprising between 51 and 57% by weight silica,
between 40 and 46% by weight of alumina and less than 3% by weight
impurities. 5 The composition of the thermoplastic film for
agricultural use allows an increase of the emissivity of the
infrared radiation of the materials used in manufacturing
greenhouses while retaining significant transmittance of visible
light in order to increase the crop yield by retention heat and
reduction in the quantity of heat to be supplied to heat
greenhouses.  
  
In the field of agricultural greenhouses are also known from
document US 6441059, a thermoplastic film comprising a high
density polyethylene matrix (HDPE) and a plurality of suitable
mineral fillers to increase the reflectance to the near infrared
radiation while retaining significant transmittance of visible
light to avoid getting daily high temperatures inside the
greenhouse, and also limit heat loss during the night. In the
above two agricultural applications, recommended thermoplastic
films are intended only to limit the harmful temperature
differences for crops due to radiative heat transfer ground / sky
while ensuring, at visible wavelengths, the external energy supply
necessary for their development.  
  
To reduce the energy required to provide for cooling a home, known
from US 6,521,038, a mixture of pigments for paint adapted to
allow the increase of the reflectance of the surface coated with
the paint to radiation near infrared.  
  
Such a mixture has the drawback of being relatively expensive in
so far as it requires a specific formulation for obtaining certain
pigments of the mixture.  
  
In addition, the effectiveness of this solution is low to the
extent that it only limits the introduction of light radiation,
and this on a few extended spectral range. The present invention
therefore aims to remedy the aforementioned drawbacks by enabling
a significant cooling a particularly economically surface.  
  
More particularly, the present invention aims to obtain a
substantial cooling of a surface by natural radiative dissipation,
especially at night. The present invention may also be designed to
ensure a water recovery, and in particular of drinking water by
condensation of atmospheric water vapor during the cooling of the
surface considered. The present invention also aims to achieve
such radiative cooling of a surface, and possibly atmospheric
water vapor condensation, stable over time. According to a first
aspect, the invention relates to a use of a composition high
emissivity on a spectral band ranging from 4 to 50 m, comprising a
polymer matrix and at least one kaolin-based filler for radiative
cooling a surface coated with said composition, and optionally the
atmospheric water vapor condensation.  
  
According to a second aspect, the invention also relates to a
paint composition comprising this composition. Finally, the
invention relates to a plastic film comprising this composition.  
  
Other objects, features, aspects and advantages of the invention
appear more clearly on reading the description and the various
examples that follow.  
  
Kaolin has the advantage of possessing a very high emissivity in
the infrared radiation, and in particular in the range from 7.5 to
25 m. Thus, with a surface coated with the composition provided
with such a burden to low optical density giving a transparent to
the composition, one can obtain an important day and night cooling
by radiative transfer, limiting the supply of external energy
required to cool a confined space. It is easily understood that
this composition is intended to be used primarily in environments
where temperatures are relatively high. The composition is
obtained from components available in low-cost trading. In
addition, the kaolin has been recognized as safe for food contact
use if the polymer matrix is aain contact with food. I1 is
possible to collect drinking water on the surface. Thus, the
drinking water recovery on a surface coated with the composition
according to the invention generates no toxicity.  
Kaolin clay is a white, friable and refractory, of lamellar
structure composed mainly of hydrated aluminum silicate. Alumina
silicate may originate from ore in the forms kaolinite, dickite
and nacrite of empirical formula Al2Si2O5 (OH) 4 or A14Si4O10 (OH)
8, the hydrated halloysite Al2O3.2SiO2.4H2O form of formula or in
its form anauxite the same composition but containing a proportion
of silica slightly higher than kaolinite. In its hydrated form
natural marketed, its water content is generally less than 7% of
the total mass and exceptionally up to 12%.  
  
The natural form is particularly suitable for applications in
water based paints.  
  
After a calcining treatment, the water content is generally less
than 1%. This form is adapted to be incorporated into plastics and
paints in solvent base.  
  
Preferably, the composition comprises from 1 to 15%, and
preferably of from 3.82 to 7.83% by volume of kaolin based on the
total volume of the initial polymer. Particularly interesting
formulations comprise from 5.7% to 7.83% of kaolin volume relative
to the total volume of the initial polymer.  
  
Preferably, the composition comprises a pigment volume
concentration from 1 to 30%, and preferably 5.90 to 12.1% by
volume of kaolin based on the total volume of other non-volatile
materials (mineral fillers, polymers and additives non-volatile).
The pigment volume concentration (PVC) is the ratio of the pigment
volume (or inorganic filler) and the total volume of non-volatile
(i.e., pigments, mineral fillers and binder) present in a paint.
This figure is generally expressed as a percentage. The binder
volume corresponds to the volume solids content of the paint used
as a basis to the mix.  
  
The average diameter of kaolin particles may range preferably
between 0.2 and 2.3 m. However, an average diameter of kaolin
particles less than 0.2 m or greater than 3 m is not harmful to
the radiative properties to thermal infrared wavelengths.  
  
Such a mean diameter of kaolin particles between 0.2 m and 2.3
provides an increase in reflectance in the near infrared
radiation. Indeed, the particles of inorganic fillers diffract the
incident radiation wavelength close to their diameter when
dispersed in a medium optical density lower than the optical
density of the mineral component.  
  
Thus, kaolin is reflective for the wavelength range between 0.2
and 2 to 3 m. Furthermore, the inhomogeneous distribution of the
particle size further increases the reflectance of the composition
to near infrared radiation. For use of the composition in the form
of thermoplastic film include for example kaolin sold under the
name GlomaxLL by Imerys with an average diameter of 1.5 m.  
For use of the composition in the form of painting, there may be
mentioned calcined kaolin sold under the name Blankalite 78 by the
Soka society, with a median diameter of 2.0 m for a solvent-based
paint, and natural kaolin atomized Blankalite 90C or 90P marketed
by the company Gakkai, respectively median diameters 0.8 m and 0.2
m respectively for lower water contents at 5 to 6%.   
  
Advantageously, the composition comprises a matrix polymer
selected from polyolefins, polyvinyls, polyvinylidene,
polystyrenics, acrylic and methacrylic polymers, polyamides,
polyesters, polyethers, polyfluorinated; polyurethane resins,
alkyd resins, epoxy resins, and phenolic resins. For example, the
polymer matrix of the composition may be selected from low or high
density polyethylene, polypropylene, polyvinyl chloride,
polystyrene, poly (ethylene / vinyl acetate), acrylic resins,
glyptal resins, and polyurethane resins.  
Preferably, polyethylene is used. Include an indication
polyethylenes used pursuant blowing sold under brand Lacqtene 1020
FN 24 of Atofina, or Lacqtene FE 8000 with an average density of
0.924.  
  
In the case of low density Lacqtene FE 8000 of a medium density
polyethylene of 0.924 to which is added 7% of additive brand Atmer
7340 0.925 density, percentage by weight of polymer in the final
formulations are respectively 62.1 % (opaque white), 69.9% (white)
and 72.4% (colorless). In another implementation, the composition
may include calcite.  
  
Calcite CaCO3 chemical formulation also having a low optical
density and giving a transparent appearance to the composition,
increases the emissivity thereof over the range from 6.5 to 9.5 m.
Radiative cooling is increased for these wavelengths.  
  
This mineral filler also has a low cost and has been recognized
safe for food contact use. The composition comprises from 0 to 5%,
and preferably from 1.52 to 1.9% calcite volume relative to the
volume of the original polymer. This composition is particularly
suitable for the manufacture of films. For the manufacture of
paints, the composition may comprise 0 to 15%, preferably 2.2 to
3.2% of pigment volume concentration of calcite. Preferably, the
average diameter of calcite particles is between 0.2 and 3 m. This
range for the average diameter of the mineral calcite fillers can
increase the reflectance of the composition for visible light and
near infrared radiation, and specifically on the wavelength
between 0.2 and 3 m.  
  
However, an average diameter smaller or larger particles will not
be harmful to the radiative properties infrared thermal
wavelengths.  
  
For use of the composition as a film or paint, can be cited as
indicative calcite marketed under the name SB Polcarb by Imerys
with a median diameter of 0.8 m. In one embodiment, the
composition further comprises titanium dioxide. TiO2 chemical
formulation of titanium dioxide may be incorporated in the polymer
matrix when it is desired to use the matrix to limit day the
heating of the surface coated with the composition. Indeed, the
introduction of titanium dioxide allows to make white opaque
composition, which allows to obtain on the visible light
reflectance of a relatively high solar energy combined with high
emissivity on the infrared radiation serves to limit daytime
heating of the surface. The use of titanium dioxide is also
eligible for food contact uses, if it is embedded in the material.  
Titanium dioxide, however, a significantly higher price than
kaolin and calcite, which increases the cost of the composition.
The composition may comprise from 1 to 20%, and preferably from
2.4 to 5.4% by volume of titanium dioxide relative to the total
volume of the initial polymer in the manufacture of thermoplastic
films.  
  
For the manufacture of paints, the composition may comprise 0 to
30%, preferably 13.9%, of pigment volume concentration of titanium
dioxide. All in the form of titanium dioxide ranges micronized
suitable for such formulations, the mean diameter being generally
between 0.1 and 0.5 m. Advantageously, the diameter means titanium
dioxide particles is between 0.20 and 0.31 m.  
  
With such an average particle diameter of titanium particles, the
reflectance of the composition is increased mainly for the
ultraviolet and visible radiation. For use of the composition in
the form of thermoplastic film include for example titanium
dioxide marketed under the name TR28 by Huntsman means 0.21 m
diameter. These particles are coated with Al2O3 to present a
stability to ultraviolet radiation. An organic treatment
facilitates their wetting by the polymer for a better dispersion
and a higher mechanical strength of the final material. For use of
the composition in the form of solvent-based paint include an
indication titanium dioxide sold under the brand Ti-Pure R-105 of
the company du Pont de Nemours, with an average diameter of 0.31
m. In one embodiment, the composition comprises at least one
anti-ultraviolet additive (UV). These additives help prevent aging
by photo-degradation of the composition used in film form or in
the form of painting.  
  
The UV stabilizing additives may be selected from the most
widespread in the polymer industry, whether benzophenones type
benzotiazoles, triazines, benzoxazinones, hindered benzoates,
hindered amines, nickel-based, etc. . These stabilizers classes
will be preferentially selected those that are accredited in
temporary contact with foodstuffs. A non-exhaustive list of
products that may be suitable is: Great lakes polymer additive
range, type products Lowilite 94, 62, 22, 26, 27, 28, Q84 and Q21
Lowilite type nickel-based, the products of Ciba Specialty
Chemicals, stabilizers Tinuvin NOR 371; Smartlight RL 1000;
Tinuvin 494; Tinuvin 783.  
  
Range of Cytec, Cyasorb UV the products; Cyasorb THT 4611. Or
products Clariant H Ostavin N 391 and Gran Gran Hostavin ARO 8 and
products from Rhodia brand ranges (paintings) Rhodocoat or
Tolonate. Anti-UV additives are generally selected based on the
polymer base used in said composition. For example, when the
composition is in the form of films and includes low-density
polyethylene, UV light stabilizer is chosen type based hindered
amines or English Hindered Amine Light Stabilizers additive (HALS
). For applying the composition in the form of thermoplastic film
include for example the anti-UV additive sold under the name
Tinuvin 783 by Ciba Specialty Chemicals, which is suitable for
food use. Advantageously, the composition comprises 0.5 to 0.7%
and preferably 0.6% by weight, said anti-UV additive based on the
total weight of the composition.  
  
This aspect of the composition must reflect the product used and
the recommended mass content by the manufacturer. For applying the
composition in the form of painting, proper commercial polymer
matrix for outdoor use already containing such additive is
sufficient. Advantageously, it is possible to impart to the coated
surface from said composition of hydrophilic surface properties to
promote the formation of films of water. Thus, in the case of
films, the composition may comprise at least one additive which
confers to the surface hydrophilic properties.  
  
This additive will favor the condensation of water at the film
surface thereby increasing the amount of water recovered.  
  
Generally, this additive is a surfactant. Moreover, in the case of
a thermoplastic film obtained by extrusion, this type of additive
allows a better distribution of the inorganic fillers within the
polymer matrix. During a cooling phase, this type of additive
migrates to the surface and gives the composition hydrophilic
properties in order to cause condensation in the form of film,
which promotes the flow and the recovery of the condensed water.
For applying the composition in the form of thermoplastic film,
there may be mentioned the surfactant additive sold under the
brand Atmer 7340 by Ciba Specialty Chemicals, which is suitable
for food use.  
  
Preferably, the composition comprises from 6 to 8% and preferably
7% by weight of said water drops anti-forming additive based on
the total weight of the composition. Of course, it is also
possible to provide any other industrial process capable of giving
it hydrophilic properties, for example a corona treatment by
dielectric barrier discharges, or also chemical treatments such as
halogenation, oxidation or that chlorophosphorylation may agree
provided that the legislation allows for the non-permanent contact
with foodstuffs.  
  
For an application of the composition in the form of paint, this
surface hydrophilic property can also be provided by a particular
step in the manufacture of said paint. Thus, the added mineral
fillers, and in particular the kaolin filler, are laid out exposed
by photolysis of the binder on the surface after a period of
exposure to ultraviolet radiation above 30 days.  
  
Painting acquires a highly hydrophilic character preserved over
time and effective in promoting atmospheric water vapor
condensation. This highly hydrophilic character also promotes
gravity flow of condensed water on the surface.  
  
According to a second aspect, the invention also relates to a
paint comprising a composition as defined above. Advantageously,
the paint is water-based or organic solvent. Finally, in a third
aspect, the invention further relates to a plastic film comprising
a composition as defined above. Preferably, the film has a
thickness of between 150 and 250 m. Such a film may be obtained
for example by molding, by blow molding or by extrusion. The
following examples illustrate the present invention and should not
be considered in any way as limiting thereof. Example 1: The
Applicant has made compositions used as films and having the
following formulations: Wire White Colourless low density
polyethylene plastic film (LDPE) Opaque Diffusing Thickness (m)
230 200 150 Titanium dioxide (TiO2) 5 4 2.4 Volume (%) 3.82 5.7
7.83 calcined kaolin (Al203.2SiO2) Volume (%) Calcite (CaCO3) 1.52
1.54 1.9 Volume (%) Total load 37, 9 30.1 27.60 Massic (%) 20  
  
Table 1 The volume percentages are based on the original volume of
polymer introduced.  
  
The first opaque white film formulation comprising a proportion by
volume of kaolin of 3.82% corresponds to a mass percentage of 9.0%
of the polymer mass originally introduced. This formulation is
recommended for applications requiring maximum opacity of the
film.  
  
The film formulations comprising a proportion by volume of kaolin
equal to 5.7% and 7.83% correspond to the respective weight
percentages of 16.1% and 21.9% relative to the polymer mass
originally introduced. The weight percentages are for guidance
from the initial polymer mass for an initial polyethylene
composition Lacqtene FE 8000 with an average density of 0.924 and
7% by mass of additive Atmer 7340 0.925 density).  
  
The mechanical properties obtained for the films of Table No. l
are: Plastic Film White Colourless low density polyethylene (LDPE)
Opaque Diffusing Stress at 10.0 elastic limit 8.1 8.7 (MPa) Strain
at limit 29 74 24 '61 2.75 elastic (%) modulus of elasticity (MPa)
240 340 560 Tensile strength 8.0 10.0 10.2 (MPa) Strain at break
71 53.0 7 30.9 ( %) 17 Table 2 mechanical tests were performed
according to ISO 527-3, ASTM D 882 or. The results, expressed in
MPa are dimensionless since 5 reduced to the section of the test
specimens.  
The optical properties obtained for films comprising formulations
identical to those of Table 1 and having measuring thicknesses of
200, 215 and 155 m are: Plastic film Colorless White low density
polyethylene (LDPE) Opaque Diffusing Br Eur (m) 200 215 155 0.90
0.86 0.62 reflectance of visible radiation (0.38 A1 0.78 m) Table 3
Example 2:  
  
The plaintiff has made compositions used as paints and comprising
the following formulations. Because of 20 the solvent when forming
the paint film, the pigment is expressed in terms pigment volume
concentration (PVC), which is the ratio of the volume of the load
calculated on the total volume of the dry extract of the final
formulation comprising the binder, the pigments and fillers, but
excluding the volume of the solvent. 1015 25 Commercial Base Type
Base Base Colourless Tinted final opaque paint radiative Opaque
Colorless Dye (including white white) CPV TiO2 13.9 CPV kaolin (%)
5.9 12.1 6.8 CPV CaCO3 (%) 2.2 3.0 3.2 22.0 15.1 10.0
Concentration Pigmentosa total added volume (%) Table 4
indication, if a colorless base is used, the volume proportion of
binder in the extract dry the final formulation is 78.0%
respectively (opaque white paint) and 84.9% (colorless paint).  
  
If a tinted base is used, the pigment volume concentration already
incorporated can be variable while the added pigment volume
concentration is 10%. In the latter case, the final proportion of
binder will be determined with knowledge of the total pigment
volume concentration in the mixture. The pigment volume
concentration of each mixture will be the same if it is a
solvent-based paint or water-based.  
  
The optical properties obtained for paints containing formulations
identical to those of Table 4 and having thicknesses of 90 and 94
m are: 20 commercial basis Type brilliant Base Colourless final
painting radiative Opaque white Colorless Thickness (m ) 90 94
Reflectance of visible radiation (0.38> 0.80 0.62 0.78 A1 m) A1
Table 5 the formulations shown in tables 1 and 4 make it possible
to obtain compositions having high emissivity the average
reflectance and infrared radiation of relatively large solar
energy to visible light and near infrared. However, a higher
relative proportion of kaolin is in no way detrimental to the
thermal infrared emissivity (4 A1 100 m) which is the essential
property of these formulations. There is no theoretical upper
limit to the incorporation of kaolin in the formulations. The
materials formulated with a volume proportion of incorporated
kaolin less than the values aagiven in Tables 1 and 4 will be
particularly suitable for passive radiative cooling applications
and atmospheric water vapor condensation.  
  
However, their emissivity medium and far infrared will be less,
reducing their effectiveness for the above applications. The
composition according to the invention is particularly suitable
for use in building construction, or in the automobile industry.
It is for example possible to use this composition in the form of
paints for vehicle bodies automobiles, or to the walls and roofs
of buildings.  
  
Of course, it is also possible to use films comprising the
composition according to the invention to coat the roofs of
buildings. A particularly interesting application of such films
also relates to their use on flat surfaces bearing against the
ground to form condensers and recovering potable liquid water. To
promote a recovery of water, it is possible to incline the
surfaces relative to the ground, for example an angle of a value
of 30 A deg  
  


---

  

**Air Well Patents**

  
US1816592  
Means to Recuperate the Atmospheric Moisture  
Achille Knapen  
  
US2138689  
Method for Gaining Water out of the Atmosphere  
Edmund Altenkirch    
  
US2401560  
Refrigerating apparatus   
Graham CD, Dybvig ES   
  
US2462952  
Solar Activated Dehumidifier  
Elmer Dunkak  
  
US6182453  
Portable, potable water recovery and dispensing apparatus  
FORSBERG FRANCIS  
  
US2761292  
Device for obtaining fresh drinkable water.   
Coanda H  
  
US2779172  
Thermo-electric dehumidifier  
LINDENBLAD NILS E   
  
US2919553  
Combination fluid heater and dehumidifier  
FRITTS ROBERT  
  
US2944404  
Thermoelectric dehumidifying apparatus  
FRITTS ROBERT  
  
US3400515  
Production of water from the atmosphere  
Ackerman E    
  
US3740959  
Humidifier-dehumidifier device.   
Foss FD  
  
US3889532  
Fog Water Collector  
Roland Pilie & Eugene Mack  
  
US4080186   
Device for extracting energy, fresh water and pollution from moist
air.   
Ockert CE   
  
US4146372  
Process and System for Recovering Water from the Atmosphere  
Wilhelm Groth / Peter Hussmann  
  
US4185969  
Process and plant for recovering water from moist gas.   
Bulang W    
  
US4206396  
Charged Aerosol Generator with Uni-Electrode Source  
Alvin Marks  
  
US4219341  
Process and Plant for the Recovery of Water from Humid Air  
Wilhelm Groth / Peter Hussmann  
   
US4234037  
Underground heating and cooling system.   
Rogers W, Midgett   
  
US4242112  
Solar Powered Dehumidifier Apparatus  
Robert Jebens  
  
US4285702   
Method and apparatus for the recovery of water from the
atmospheric air.   
Michel H, Bulang   
  
US4304577  
Water producing apparatus.   
Ito T, H Matsuoka, Azuma K, Y Hirayama, N Takahashi  
  
US4315599  
Apparatus and method for automatically watering vegetation.   
Biancardi RP   
  
US4342569  
Method and apparatus for abstracting water from air.   
Hussmann P   
  
US4345917  
Method and apparatus for recovery of water from the atmosphere.   
Hussmann P  
  
US4351651  
Apparatus for extracting potable water.   
Courneya CG    
  
US4374655  
Humidity Controller  
Philomena Grodzka, et al  
  
US4433552  
Apparatus and method for recovering atmospheric moisture  
Smith RH   
  
US4377398  
Heat Energized Vapor Adsorbent Pump  
Charles Bennett  
  
US4459177   
Ground moisture transfer system.   
OaHare L   
  
US4475927  
Bipolar Fog Abatement System  
Hendricus Loos  
  
US4506510   
Apparatus for continuously metering vapours contained in the
atmosphere.   
Tircot M  
  
US4726817  
Method and Device for Recovering in Liquid Form the Water Present
in the Atmosphere in Vapor Form  
Roger Rippert  
  
US5106512   
Potable air-water generator.   
Reidy J    
  
US5149446   
Potable water generator.   
Reidy JJ   
  
US5203989   
Potable air-water generator.   
Reidy JJ  
  
US5233843  
Atmospheric water extractor  
Clarke / Calif  
  
US5275643  
Fog Water Collecting Device.  
Yoshio Usui  
  
US5284628  
Convection towers  
Melvin Prueitt  
  
US5357865  
Method of Cloud Seeding  
Graeme Mather  
  
US5395598  
Convection towers  
Melvin Prueitt  
  
US5477684  
Convection towers  
Melvin Prueitt  
  
US5626290  
Rain Making System  
Donald Kuntz  
  
US5669221  
Portable, Potable water recovery and dispensing apparatus.   
LeBleu TL   
  
US5729981  
Method and Apparatus for Extracting Water  
Michael Braun, Wolfgang Marcus  
  
US5845504  
Portable/potable water recovery and dispensing apparatus  
LeBleu TL    
  
US5846296  
Method and device for recovering water from a humid atmosphere.   
Krumsvik PK  
  
US6029461   
Water collection and dispensing.   
Zakryk JM  
  
US6156102  
METHOD FOR RECOVERING WATER FROM AIR  
CONRAD, WAYNE ERNEST  
  
US6360557 / US6957543  
Air Cycle Water Producing Machine  
Igor Reznik  
  
US6490879   
Water generating machine.   
Lloyd DJ, Baie    
  
US6511525  
METHOD & APPARATUS FOR EXTRACTING WATER FROM AIR USING A
DESICCANT  
SPLETZER, BARRY / CALLOW, DIANE SCHAFER  
  
US6574979  
Production of Potable Water... from Hot and Humid Air  
Abdul-Rahman Faqih  
  
US6644060  
Apparatus for extracting potable water from the environment air.   
Dagan A    
  
US6684648   
Apparatus for the production of freshwater from extremely hot and
humid air.   
Faqih AAM  
  
US6755037   
Apparatus and method for extracting potable water from atmosphere.
  
Engel DR, Clasby ME   
  
US6868690  
Production of potable water and freshwater needs for human, animal
and plants from hot and humid air.   
Faqih AAM   
  
US6869464 / US6869469  
Atmospheric water absorption and retrieve device.   
Klemic J  
  
US6945063  
Apparatus and method for harvesting atmospheric moisture  
  
US6957543 / US6360557  
Air Cycle Water Producing Machine  
Igor Reznik  
  
US7251945  
Water-from-air system using desiccant wheel and exhaust  
Tongue S  
  
US7306654  
METHOD AND APPARATUS FOR PRODUCING POTABLE DRINKING WATER FROM AIR  
HARRISON, NORMAN   
  
US7328584   
Fresh water extraction device.   
Craven JP   
  
US7601206  
Method and apparatus for generating water using an energy
conversion device.   
Call CJ, et al  
  
US7954335  
ATMOSPHERIC WATER HARVESTERS WITH VARIABLE PRE-COOLING  
  
US8118912  
Low power atmospheric water generator.   
Rodriguez F, Khanji N   
  
US8506675  
Composite desiccant and air-to-water system and method  
Ellsworth J   
  
US8627673  
ATMOSPHERIC WATER HARVESTER  
  
US2002011075  
Production of Potable Water... from Hot and Humid Air  
  
US2002029580  
Apparatus and Method for... Production of Fresh Water from Hot
Humid Air  
  
US2003097763  
Combination Dehydrator and Condensed Water Dispenser  
  
US2003150483  
Apparatus and Method for Harvesting Atmospheric Moisture   
  
US2004112055  
Atmospheric Vortex Engine  
Louis Michaud  
  
US2004000165  
Apparatus and Method for Harvesting Atmospheric Moisture  
Michael Max  
  
US2005103615  
Atmospheric Water Collection Device  
Johnathan Ritchy  
  
US2005266287  
Device for Producing Water on Board of an Airplane  
Claus Hoffjann & Hans-Juergen Heinrich  
  
US2005284167  
Combination Dehydrator, Dry Return Air and Condensed Water
Generator/Dispenser  
Michael Morgan  
  
US2005266287  
Device for Producing Water on Board of an Airplane  
Claus Hoffjann & Hans-Juergen Heinrich  
  
US2006032493  
Device for Collecting Atmospheric Water  
Jonathan Ritchey  
  
US2006112709  
Method and Apparatus for Collecting Atmospheric Moisture  
Peter Boyle  
  
US2006130654  
Method and Apparatus for Recovering Water from Atmospheric Air  
Ronald King & Norman Arrison  
  
US2006279167  
SYSTEM & METHOD, FOR RECOVERING WATER FROM AIR  
TURNER, J GLENN  
  
US2007220843  
METHOD FOR EXTRACTING WATER FROM AIR, AND DEVICE THEREFOR  
IKE, H / OKUHATA, N   
  
US2008314058  
Solar Atmospheric Water Harvester  
  
US2010307181  
ATMOSPHERIC MOISTURE HARVESTING  
  
US2011232485  
COMPOSITE DESICCANT AND AIR-TO-WATER SYSTEM AND METHOD  
ELLSWORTH JOSEPH  
  


---

  
CA2478896  
Combination Dehydrator & Condensed Water Dispenser  
Janet Morgan  
  
CA774391  
Method for Precipitating Atmospheric Water Masses  
David Glew & Andrew Watson  
  
CA497523  
APPARATUS FOR EXTRACTING WATER FROM AIR  
SUITER, WILL D  
  
CA2070098  
APPARATUS FOR RECOVERING WATER FROM AIR AND METHOD OF WATER
RECOVERY  
CONRAD, WAYNE E  
  
CH608260  
Process for Obtaining Service Water or Drinking Water...  
Gotthard Frick  
  
DE19734887 / WO9907951  
Device for Obtaining Water from Air  
Heinz-Dieter Buerger & Yourii Aristov  
  
DE3313711  
Process and Apparatus for Obtaining Drinking Water  
Rudolf Gesslauer  
  
EP1142835  
Portable, Potable Water Recovery and Dispensing Apparatus  
Francis Forsberg  
  
EP1629157  
Device for the Extraction of Water from Atmospheric Air  
Frank Thielow  
  
FR2813087  
Unit Recovering Atmospheric Moisture from Vapor or Mist...  
Jacques P. Beauzamy  
  
NL1030069  
Atmospheric Water Collector...  
Ghassan Hanna  
  
CH608260  
Process for Obtaining Service Water or Drinking Water...  
Gotthard Frick  
  
CN2573556 // CN2573555  
Solar adsorption device for obtaining water  
  
CN1403192  
High-hydroscopicity adsorbent and its prepn  
  
UA66218  
A PROCESS FOR PREPARATION OF SWEET WATER FROM AIR  
NEVEDNICHENKO, PETRO SAVOVYCH / HERMAN NATALIIA PETRIVNA  
  
AU3241078  
RECOVERY OF WATER FROM AIR  
  
AU517422B  
OBTAINING WATER FROM AIR  
CLUCK, A  
  
PL257283  
SEPARATOR FOR SEPARATION OF DUST AND WATER FROM AIR  
FRYDEL, WALENTY  
  
GB251689  
Method of and Apparatus for Causing Precipitation of Atmospheric
Moisture and for Kindred Purposes  
William Haight  
  
GB319778  
Improved Means for Collecting Moisture from the Atmosphere  
Achille Knapen  
  
GB1164119  
Device for Modifying Atmospheric Conditions for example, for the
Inhibition or Dispersal of Fog or Mist, or to Induce Rain  
Edmund Updale  
  
GB1214720  
Fog Abatement & Cloud Modification  
  
GB251689  
Method of and Apparatus for Causing Precipitation of Atmospheric
Moisture and for Kindred Purposes  
William Haight  
  
GB319778  
Improved Means for Collecting Moisture from the Atmosphere  
Achille Knapen  
  
GB1164119  
Device for Modifying Atmospheric Conditions for example, for the
Inhibition or Dispersal of Fog or Mist, or to Induce Rain  
Edmund Updale  
  
GB2064358  
EXTRACTING WATER FROM AIR  
  
GB1200221  
PRODUCING FRESH WATER FROM AIR RAISED TO HIGH HUMIDITY BY EXPOSURE
TO WATER VAPOR FROM CONTAMINATED SOURCES OF WATER  
DOBELL, CURZON  
  
GB2376401  
Self-watering Plant Pot  
  
RU2190448  
Independent Complex for Separating Moisture from Air  
O. A. Bernikov  
  
RU2235454  
Method & Apparatus for Producing Acoustic Effect upon
Atmospheric Formations  
E. T. Protasevich & S.A. Ryzhkin  
  
RU2185482  
Apparatus for Receiving Biologically Pure Fresh Water... out of
Atmospheric Air  
  
RU2182562  
Method of Producing Biologically Active Potable Water with Reduced
Content of Deuterium...  
  
RU2146744  
Method for Producing Water from Air  
  
RU2132602  
Method for Accumulating Moisture in Full Fallows  
  
RU2151973  
PROCESS OF WINNING OF WATER FROM AIR ( AIR DRYING ) AND GEAR FOR
ITS REALIZATION  
SIRENKO, V S; GORJACHEV, E A  
  
RU2143530  
DEVICE FOR PRODUCING FRESH WATER FROM AIR  
KOCHETKOV, B F  
  
RU2064036  
DEVICE FOR SEPARATING WATER FROM AIR  
SHAROV, VIKTOR  
  
RU2062838  
DEVICE FOR TAKING DRINKING WATER FROM AIR  
KULIKOV, VIKTOR  
  
RU2000393  
APPARATUS FOR EXTRACTION OF WATER FROM AIR  
SHAROV, VIKTOR V  
  
RU2278790  
Method & Apparatus for... Extraction of Water from
Atmosphere...  
Vladimir Krjukovskij, et al.  
  
RU2278929  
Vortex System for Condensing Moisture from Atmospheric Air  
Vjacheslav Alekseev, et al.  
  
RU2272877  
Method for Obtaining Water from Air  
Jurij Aristov, et al.  
  
RU2190448  
Independent Complex for Separating Moisture from Air  
O. A. Bernikov  
  
RU2235454  
Method & Apparatus for Producing Acoustic Effect upon
Atmospheric Formations  
E. T. Protasevich & S.A. Ryzhkin  
   
SU69751  
Equipment for collecting water from air  
Tygarinov  
  
SU1751608  
DEVICE FOR COLLECTING DRINKING WATER FROM AIR  
DEMIDOV, VALENTIN  
  
WO2007009184  
Gust Water Trap Apparatus  
Maxwell Whisson  
  
WO2006017888  
Apparatus & method for Cooling of Air  
Maxwell Whisson  
  
WO2006040370  
Method of Obtaining Water from an Atmospheric Air Mass...  
Alexander Ermakov  
  
WO2006028287  
Method of Water Extraction... from Atmospheric Air  
Hideya Koshiyama  
  
WO2002086245  
METHOD FOR EXTRACTING WATER FROM AIR AND DEVICE FOR CARRYING OUT
SAID METHOD  
ROMANOVSKY, VLADIMIR FEDOROVICH  
  
WO200184066  
DEVICE FOR COLLECTING WATER FROM AIR  
FAWZI, HISHAM  
  
WO200111152  
METHOD FOR OBTAINING WATER FROM AIR  
LADYGIN, ANATOLY VLADIMIROVICH  
  
WO9907951  
DEVICE FOR OBTAINING WATER FROM AIR  
BUERGER, HEINZ-DIETER  
  
WO9739197  
METHOD OF EXTRACTING WATER FROM AIR AND A DEVICE FOR CARRYING OUT
SAID METHOD  
ROMANOVSKY, VLADIMIR  
  
WO200218859  
METHOD AND APPARATUS FOR EXTRACTING WATER FROM AIR  
SPLETZER, BARRY  
  
WO200218858  
METHOD AND APPARATUS FOR EXTRACTING WATER FROM AIR  
SPLETZER, BARRY  
  
WO200136885  
METHOD AND APPARATUS FOR EXTRACTING WATER FROM AIR  
SPLETZER, BARRY L  
  
WO2004029372  
Method & Apparatus for Collecting Atmospheric Moisture  
Peter H. Boyle  
  
WO2003104571  
Device for Collecting Atmospheric Water  
Jonathan Ritchey  
  
WO9943997  
System for Producing Fresh Water from Atmospheric Air  
  
WO02094725  
Method and Device for Recovery of Water from the Atmospheric Air  
  
WO03078909  
Combination Dehydrator and Condensed Water Dispenser  
  
WO2007051886  
NOVEL PLANT FOR GENERATING WATER FROM AIR  
MARTINEZ, SANTIAGO JOSE ANTONIO  
  
WO2007041804  
METHOD & APPARATUS FOR EXTRACTING WATER FROM AIR CONTAINING
MOISTURE  
CLARKE, PETER  
  
JP52134896  
METHOD OF RECOVERING WATER FROM AIR APPARATUS THEREFORE AND
PROCESS FOR PREPARING SILICAGEL AND APPARATUS THEREFORE  
BUIRUHERUMU, GUROOTO  
  
JP54047354  
METHOD OF OBTAINING WATER FROM AIR IN ATMOSPHERE AND ITS DEVICE  
BUORUFUGANGU, BURANGU  
  
JP2004316183  
Equipment & Method for Producing Fresh Water from Atmospheric
Moisture Content  
Aoki Kazuhiko, et al.  
  
JP2004169321  
METHOD FOR EXTRACTING WATER FROM AIR & APPARATUS THEREFOR  
IKE, HIDETOSHI  
  
JP 2004057890  
ULTRA WATER-REPELLENT SURFACE TYPE WATER EXTRACTION DEVICE FOR
EXTRACTING WATER FROM AIR & NEGATIVE ION PRODUCING DEVICE  
KOSHIYAMA, HIDEYA  
  
JP5203177  
FORCE FEED SYSTEM FOR DRAIN WATER FROM AIR-CONDITIONER  
AWATA, KOJI  
  
JP59150277  
PREVENTIVE DEVICE FOR SCATTERING OF WATER FROM AIR CONDITIONER  
HISATAKA, SATORU  
  
JP54127870  
METHOD AND APPARATUS FOR OBTAINING WATER FROM AIR  
HERUMUUTO, MIHIERU  
  
  
KR20010003009  
EVAPORATOR OF DRAIN WATER FROM AIR CONDITIONER IN ELEVATOR  
HWANG, JONG YUN  
  
KR20000052036  
EVAPORATOR FOR DISCHARGING WATER FROM AIR CONDITIONER OF ELEVATOR  
HWANG, JONG YUN  
  
KR20010077162  
NON-POWERED APPARATUS AND METHOD FOR DRAINAGE OF CONDENSATE WATER
FROM AIR CONDITIONER  
LEE, GWANG SEOP / LEE, MYEONG SEOP  
  
KR20070028377  
METHOD FOR EXTRACTING WATER FROM AIR, AND DEVICE THEREFOR  
IKE, HIDETOSHI /OKUHATA, NAO

---