Andrew Abolafia -- Static Field Converter

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**Andrew ABOLAFIA**

**Static Field Converter**

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Email: Andrew@InventorOne.com

 
 

Contact Phone: 518-632-9193   
 Contact Fax:
518-632-9192

The Andrew Abolafia  Co.   
 PO Box  291   
 Granville, NY 12832

 
Andrew Abolafia

![](andrewabolafia.jpg)

  


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**<http://www.mmdnewswire.com/source-of-energy-2450.html>**

 

*October 23, 2007 -- Hartford, NY* --
The Andrew Abolafia Company, after more than four years of
research on an intellectual property (Static Field
Converter) in collaboration with the University at Buffalo,
SUNY, produced results that suggest The Andrew Abolafia
Companys Static Field Converter taps a new source of
energy. ANSYS Finite Element Analysis computer simulation
yields the data that support that interpretation. It has
helped enable The Static Field Converter to evolve and be
refined in conjunction with experimentation at the
University at Buffalo.

 

The Static Field Converter (patented and
patents pending) is an invention that converts the energy in
a static magnetic field into usable electrical energy. The
significance of the innovation is that the energy stored in
some permanent magnet materials can be tapped. The magnitude
of the energy is large enough to make a significant impact
in reducing the U.S. addiction to oil as well as mitigate
the destruction of the environment. Large amounts of
electricity generated by the invention can produce large
amounts of hydrogen. Hydrogen can be used as fuel in most
applications that now require fossil fuels. It can also be
used to power fuel cells. The exhaust is water.

 


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[**http://www.inventorone.com/**](http://www.inventorone.com/)

**Publications**

1. A. Puppala, M. Soliman and M. Safiuddin,
State University of New York at Buffalo, Amherst, NY, A.
Abolafia, The Andrew Abolafia Co., Hartford, NY,
"Feasibility Study of Rotating Shield Generator,"
AIAA-2005-5646. 3rd International Conversion Engineering
Conference and Exhibit, San Francisco, California, August
15-18, 2005.

 

2. Puppala A K, Soliman M, Safiuddin M,
Abolafia A, "Feasibility Study of Static Field Converter,"
3rd International Industrial Simulation Conference 2005
ISC'2005, pp 210-13, Berlin, Germany June 9-11, 2005.

 

Background

 

A small business matching grant (March, 2003)
between TCIE (The Center for Industrial Effectiveness-SUNY,
Buffalo) and The Andrew Abolafia Company of Hartford, NY
initiated research on the Abolafia Company's patented
technology (published on this web site) at the University at
Buffalo, SUNY, electrical engineering department. The patent
(and patents pending) are based upon a High Temperature
Superconductor energy conversion device termed a "Static
Field Converter" that uses a hemispherical High Temperature
Superconductor (HTS) element as a rotor. The invention
converts the energy in a static magnetic field into useable
electrical power. That energy can be significant, clean and
abundant. We applied for and received the grant because we
were interested in knowing the feasibility of construction
of the device.

 

More than four years of research later an
electrical engineering graduate student at UB who worked on
the project used the research as the basis of his Master's
and Doctoral dissertations and several scientific papers
were produced. An analysis was done, using a Finite Element
Analysis program, assuming perfect diamagnetic properties
for the HTS superconductor.

 

"Because of the high flux density values of
the Permanent Magnet (PM) used in the simulations, and the
assumption that the superconductor behaves ideally as a
perfect diamagnetic material, the voltage output observed in
the simulation was appreciable.

 

To meet the counter torque when power is
being taken out from the system, there must be power input
from the prime mover, or the Permanent Magnet must
constantly lose its magnetic energy."1

 

Conclusion: The New Source of  Energy

 

The Andrew Abolafia Company's conclusion is
that power is coming from the Permanent Magnet and that the
energy contained in certain permanent magnetic materials is
appreciable enough to be considered as a hitherto untapped,
abundant, clean source of energy that can make fossil fuels
obsolete. The substitution of an electromagnet for the
permanent magnet would produce data that would support
energy being consumed from the magnetic source. The
University at Buffalo, SUNY, does not concur with this
conclusion but concludes the invention is a promising new
type of generator.

Abstract

 

If the wave form of the output power of the
invention is symmetrical (which it is) a perfectly
diamagnetic rotor will be repelled by the same magnitude of
torque when it exits the magnetic fields of the magnet and
output coil as when it enters them (Magnetostatic analysis
is appropriate). No energy input is necessary upon exiting
the magnetic fields (the rotor, a perfect diamagnet, is
always repelled by a magnetic field). A prime mover is only
necessary upon entering the combined magnetic fields
of  the magnet and coil (the rotor, a perfect
diamagnet, is always repelled by a magnetic field). The
torques acting on the rotor are equal and opposite resulting
in zero net torque on the rotor. Therefore a net power of
zero horsepower from the prime mover (minus losses) can
drive the rotor. The energy to generate the electric power
from the Static Field Converter can only come from the
magnet. If there is doubt simply substitute an
electromagnet. An FEA computer simulation of the invention
can corroborate our observations and conclusions at any
company, university or research facility in the world with
the appropriate IT resources.

Summation

 

Some types of Permanent Magnetic materials
can be used as a new source of energy.

 

1A. Puppala, State University of New York at
Buffalo, Amherst, NY "Doctoral Dissertation, Dept. of
Electrical Engineering," pp.2-3, September, 2007.

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http://www.tabexperts.com/AbouttheAuthor.htm

 

Andrew Abolafia is the
founder and CEO of the Andrew Abolafia Company
(InventorOne.com) located in yjr Northeastern USA. He has
and continues to serve as consultant to Fortune 500
clients.. Mr. Abolafia holds a Summa Cum Laude Bachelors
degree from York College. He also holds a diploma in
computer programming from Chubb Institute. He has held
positions of trust and responsibility at Eagle Electric
Manufacturing Company, Inc., Trichem, Inc. and Pepsico, Inc.
He is available to serve as a consultant and expert witness
in computer related fields such as software, software
engineering, software liability, computer languages and
programming, the Internet, Internet related software,
infrastructure and computer security.

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**<http://v3.espacenet.com/publicationDetails/biblio?adjacent=true&KC=A&date=19980120&NR=5710531A&DB=EPODOC&locale=en_EP&CC=US&FT=D>**

**US5710531** **Static field converter**

 1998-01-20

Abstract -- A device for the conversion of a static magnetic
field into electrical energy comprising a permanent or
electromagnet for establishing a stationary (static) magnetic
field, one or more coils responsive to the magnetic field, a
switch to periodically place a load across said responsive
coils, and a hemispherical diamagnetic insulating element to
periodically shield the coils from the magnetic field to produce
electrical energy in the coils. The responsive coil may be
cylindrical and totally surround one pole (half) of a magnetic
dipole. The insulating element is rotatable around the magnet
and is to alternately shield and expose the coil to the field of
the magnet. The switch periodically opens and closes the coil
circuit corresponding of the rotation of the shield.

1. Field of the Invention

The present invention relates to an apparatus for producing
electrical energy and, more particularly, to an electrical
device for efficiently transforming the energy of a stationary
magnetic field into useful electrical energy for use as an
electric generator, a dc/ac converter, dc transformer, or a high
energy density battery through the use of the diamagnetic
properties of superconductive materials.

2. Description of the related Art

Various attempts have been made to use the Meissner effect of
superconductive materials to perform useful work. The Meissner
effect occurs when a superconductive material is cooled to a
temperature below its transition point. In a magnetic field, the
lines of induction are then pushed out as if the superconductor
exhibited perfect diamagnetism. Various devices have been
developed which bring a superconductor in or out of the
diamagnetic state or mechanically move a superconductive element
in relation to a magnetic field and thereby produce or control
mechanical, magnetic or electrical energy.

For example, U.S. Pat. No. 5,339,062 to Donaldson et al.,
issued on Aug. 16, 1994, discloses a system where electrical
energy is transferred or switched to a secondary inductive
element (a coil) through a path which contains a high
temperature superconductive element which is capable of holding
off the field when in its superconductive state. The
superconductive element is driven in and out of the diamagnetic
state by heating with a laser pulse. When in its normal state,
the flux passes through the element and couples the field to the
secondary, which may be connected to a load. When in a
superconductive state, there is no coupling. A primary coil of
superconductive material around the secondary coil can provide
superconductive magnetic energy storage. The primary field is
held off by its superconductive elements in the flux path to
opposite ends of the secondary coil. These elements may be
driven normal by laser pulses to transfer the stored magnetic
energy to a load. A plurality of secondary coils, each with
associated superconductive elements, may be selectively coupled
to the load as programmed inductive elements. Similarly, Soviet
Union Patent No. 1736016-A1 dated May 23, 1992 to Kuroedov Yu D,
discloses a device for storing electromagnetic energy and
generating pulsed currents using a superconductive screen
between the windings.

Japanese Patent No. 1-24474 (A) dated Jan. 26, 1989 to Sharp
Corp., discloses a disk 11 which is driven into rotation by the
repulsion between a permanent magnet 15 and a layer of cooled
superconductive material 13 at the edge of disk 11 thereby
providing rotational force. Similarly, Japanese Patent No
1-273369 (A) dated Nov. 1, 1989 to Fuji electric Co., Ltd., also
uses the Meissner effect to drive a rotating disk. Japanese
Patent No. 5-268736 (A) dated Oct. 15, 1993 to Sanyo Electric
Co., Ltd., discloses a motor driven by a dc source without
energy loss. A disk is floated in position by means of the
diamagnetic properties of superconductors. Thus, the function of
the superconductive element is to suspend the rotor and
eliminate friction.

Japanese Patent No. 1-149409 (A) dated Jun. 12, 1989 to
Mitsubishi Electric Corp., shows a static superconducting
generator where mechanical movement of a superconductive element
in a magnetic field acts to generate power. Japanese Patent No.
1-138703 (A) dated May 31, 1989 to Toshio Takayama, discloses an
electric generator using superconductive elements as a magnetic
shield. German Patent No. DE 708986 dated Mar. 19, 1987 to
Priebe, K.P., shows a field effected induction unit to convert
magnetic to electric energy uses, by use of a superconducting
material to form a screen of the induction coil.

U.S. Pat. No 4,237,391 to Schur and Abolafia, discloses an
electrical generator comprising a stationary permanent magnet
for establishing a magnetic field, one or more sensing coils
responsive to the magnetic field and a diamagnetic blocking
element moveable between the magnet and sensing coil for
periodically interrupting the magnetic field to produce
electrical energy in the coil. In that device, the blocking
element is a rotatable disk interposed between a magnet and a
coil. The rotatable disk has a semicircular portion of
magnetically inert material to alternately block and pass the
magnetic field to the coils upon rotation of the disk. It does
not disclose the use of a hemispherical shielding member which
rotates around the magnetic or electromagnetic element.

Most of these patents require bringing an element in and out of
a superconductive state and as such, require the expenditure of
substantial energy in making this transition. This prior art
does not disclose a system in which a superconductive shielding
element rotates around a magnetic field to alternately expose
and shield a responsive electrical coil from the magnet.

SUMMARY OF THE INVENTION

 

In the present invention, a superconductive
magnetic insulating/blocking device in the form of a
hemisphere, rotates inside a responsive means such as a coil
to periodically shield and unshield the responsive means
from a magnetic field. The invention provides for the
efficient transformation of the energy of the magnetic field
into electrical energy and can thus be used as a dc
transformer, a dc to ac converter, an electric generator or
a very high energy density battery.

 

Faraday's Law states the the induced emf
around a closed mathematical path in a magnetic field is
equal to the rate of change of magnetic flux intercepted by
the area within the path, or

 

emf   =  -dphi/dt

 

emf   =  Electromotive Force   
 phi    =  BA   
 B      =  
Magnetic Field   
 A      =  
Area Bounded By Conductor

Faraday's Law is unconcerned with how the
change in magnetic flux occurs. Inefficient systems can use
large amounts of energy to change the magnetic flux and
produce the electromotive force while more efficient methods
for changing the flux may be used to produce the same
electromotive force for far less energy. Thus, the
efficiency in the production of the emf is a product of the
efficiency in changing the magnetic flux which passes
through the closed circuit.

 

In the present invention, the Meissner effect
of superconductive materials (i.e., the diamagnetic
properties of a superconductive material operating at a
temperature below its transition temperature) are exploited
to provide a device for producing electrical energy from a
fixed magnetic field. A superconductive element maintained
at a temperature immediately below its transition
temperature or colder periodically acts to shield a
responsive means such as a coil from a magnetic field
established by a permanent or electromagnet, to generate
electrical energy.

 

A static field converter of the present
invention comprises a magnetic dipole such as a permanent or
electromagnet for establishing a magnetic field, a
responsive means which generates electric current in
response to the magnetic field established by the magnetic
dipole, a shielding means interposed between the field of
the magnetic dipole and a responsive means, a switching
device to periodically open and close the circuit forming
the responsive means, and a driving means to rotate the
shielding means.

 

The magnetic dipole can be any source of
magnetic field such as a permanent or electromagnet. The
shielding means comprises a magnetic flux shielding device
of diamagnetic material mounted for movement between the
magnetic dipole and the responsive means, thereby
alternately shielding and unshielding the magnet flux from
the magnetic dipole to the responsive means. The shielding
means of the preferred embodiment comprises a hemisphere of
superconductive material mounted such that it rotates around
the field of the magnetic dipole and the magnetic field,
thereby shielding and unshielding the responsive means from
the magnetic field. The shield may form part of a rotatable
sphere composed of two hemispherical elements, the first of
magnetically inert material and the second of
superconductive material. This sphere may be mounted about a
sphere of ferromagnetic material such as transformer steel
or the like which would enclose and confine the field of the
magnetic dipole.

 

The sensing means may comprise an electrical
coil positioned around the shielding means and thus around
the magnetic dipole. The coil forming the responsive means
may be periodically opened and closed during the operating
cycle of the present invention thereby eliminating magnetic
resistance to rotation of the shielding means as it rotates
around the magnetic dipole and in and out of the responsive
means. An electric motor or other means can be used to
rotate the shield.

 

BRIEF DESCRIPTION OF THE DRAWINGS

 

The foregoing and other objects, features and
advantages of the present invention will become more
apparent by the reading of the following description in
connection with the accompanying drawings, in which:

 

FIG. 1 is a
perspective view, with interior elements shown by dotted
lines, of a static field converter constructed in accordance
with the principles of the present invention;

![](571-1.jpg)

FIG. 2 is a cross-sectional view of the
apparatus of FIG.1, taken at 2-2, with lines added to show
magnetic flux and other schematic elements;

![](571-2.jpg)

FIG. 3 is a schematic diagram showing a first
position of the shield member in an operating cycle with a
representation of the corresponding flux pattern shown;

![](571-3.jpg)

FIG. 4 is a schematic diagram showing a
second position for the shielding member in an operating
cycle as it rotates 180 degrees from the first position with
the corresponding flux pattern shown; and

 

FIG. 5 is a schematic
diagram showing the return position of the shield member to
the first position in its operating cycle with the
corresponding flux pattern shown;

 

FIG. 6 is a
perspective view with interior elements shown by dotted
lines of a second embodiment of the static field converter
constructed in accordance with the principles of the present
invention in which there are two sets of coils.

![](571-6.jpg)

Referring to FIGS. 1 and 2, the
superconductive static field converter unit 10 of the
present invention is shown. It is adapted to be immersed in
a low temperature vessel, e.g. a Dewar tank or refrigeration
unit 14 diagrammatically shown in FIG. 2 to maintain the
unit at temperatures below the transition temperature of the
superconductive material. The static field converter 10
includes a circular base 11 provided with four support means
17, 18, 19 and 20 extending upward from the circular base.

 

A magnet 13 is mounted on support means 17
and 19 by rods 15 and 16 by conventional means such as
collars 21 and 22 or alternatively a bonding method such as
adhesives (not shown) may be used. Support means 17-20, rods
15 and 16, collar 21 and 22, and base 1 are made from
non-conducting, non-ferromagnetic material such as plastic
or graphite. Magnet 13 is shown in the diagrams as an
electromagnet having coils 23 around a core 24 of
transformer steel or the like. Alternatively, magnet 13 may
be in the form of a permanent magnet. Rods 15 and 16 and
magnet 13 are in a fixed position and do not rotate.

 

The coil 12 is mounted on supports 18 and 20
by conventional means (not shown). While responsive means 12
is shown as single coil, it may consist of several coils
either on the same or opposite hemispheres. The coil forming
responsive means 12 consists of a plurality of turns of
insulated wire and includes a set of leads 26 electrically
connective  to the responsive means 12 to a switch 25.
Leads 27 for attachment to a load (not shown) are connected
to leads 26 through switch 25.

 

A shielding means 30 is rotatedly mounted on
bearing 31 and 32 of a non-conducting, non-ferromagnetic
material which are rotatively position around rod 15 and 16,
respectively. The shielding means 30 consists of a
hemisphere of superconductive material 35. It may be paired
with a hemisphere 36 of magnetically inert material such as
Teflon to form a complete sphere for easier rotation or may
consist solely of the hemisphere of superconductive
material. The field of magnet 13 is totally contained within
shielding means 30, either by the air gap between the magnet
13 and the shielding means 30 or by a ferromagnetic flux
guide 45. The flux guide 45 of ferromagnetic material, such
as transformer steel, may be positioned immediately inside
the shielding means 30 but not in contact with it. The flux
guide 45 completely encloses the magnet 13.

 

The shield is so mounted that it is freely
rotated on bearings 31 and 32 around rods 15 and 16 so that
the hemisphere of superconductive material can be
periodically placed between the magnet 13,  its field
and the responsive means 12, thereby shielding the
responsive means 12. An electric motor 40 is attached to
bearing 32 through gears 41 and 42. The electric motor, when
activated, rotates the shielding means around magnet 13,
alternately coming between and outside of the responsive
means 12. While an electric motor 40 is shown, other means
can be used to rotate the shielding means.

 

In starting the apparatus, the static field
converter 10 is inserted in the refrigeration tank 14. The
temperature is then reduced to below the transition
temperature of the superconductive material 35. Rotation of
the shielding means 30 is initiated by motor 40. When the
switch 25 is in the open position, such that responsive
means 12 does not form a complete circuit, there is nothing
to resist the rotation of the shielding means 30 other than
a normal friction encountered at bearings 31 and 32 and,
accordingly, shielding means 30 freely rotates around rods
15 and 16 as it is driven by motor 40.

 

As seen in FIG. 3, at the beginning of a cycle, the superconducting
hemisphere is totally outside the coils forming responsive
means 12 and switch 25 is open circuited. Since switch 25 is
open circuited, the hemisphere 35 freely rotates up into
coil 12 when driven by motor 40. Accordingly, it can freely
rotate to the position diagrammatically shown in FIG. 4 where the
superconductive shielding material is positioned totally
within the coil from the responsive means 12. At this point
the responsive means 12 is completely shielded from the
magnetic field and magnetic dipole 13, as diagrammatically
shown in FIG. 4. At this point, switch means 25 is automatically
closed and puts a load across responsive means 12. As the
shielding means 30 continues rotation, the magnetic field
generated by magnet 13 is exposed to the responsive means
12. This produces a current in the responsive means 12 and a
corresponding magnetic field. This acts to further drive the
superconductive portion of the shielding means 35 around
rods 15 and 16 driving it to the position shown in FIG. 5 which corresponds to
the initiating position of FIG. 3. Once it is in the  position shown in FIG. 5, switch means 25
automatically opens the circuit once again so that the flux
does not generate a magnetic field in coil 12 that would
repel shielding means 30.

 

While the invention has been disclosed with
the superconductive material being in the form of a
hemisphere, it may equally be any other shape having a
cavity in which the magnet 13 can be at least partially
mounted.

 

While the invention has been described as
having a preferred design, it is understood that it is
capable of further modification, uses and/or adaptations of
the invention following in general the principal of the
invention and including such departures from the present
disclosure as come with known or customary practice in the
art to which the invention pertains, as may be applied to
the central figures hereinabove set forth and fall within
the scope of the invention of the limits of the appended
claims.

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http://v3.espacenet.com/publicationDetails/biblio?adjacent=true&KC=A&date=19830524&NR=4385246A&DB=EPODOC&locale=en\_EP&CC=US&FT=D

**US4385246** **Apparatus for producing electrical
energy**

( Andrew Abolafia & Paul SCHUR )   
EC:   H02K55/02  IPC:   H02K55/02;
H02K55/00; (IPC1-7): H02K11/00   
1983-05-24

 

Abstract -- An
electrical generator comprises a stationary permanent magnet
for establishing a magnetic field, one or more sensing coils
responsive to the magnetic field, and a diamagnetic blocking
element movable between the magnet and the sensing coils for
periodically interrupting the magnetic field to produce
electrical energy in the coils. A preferred embodiment
includes a pair of semi-circular coils arranged side-by-side
in the magnetic field and a rotatable blocking disc
interposed between the magnet and the coils. The disc
includes a semi-circular portion of superconductive material
rendered impermeable to the magnetic field at temperatures
near absolute zero and a semi-circular portion of
magnetically inert material to alternately block and pass
the magnetic field to the coils upon rotation of the disc.

Abstract

 

An electrical generator comprises a
stationary permanent magnet for establishing a magnetic
field, one or more sensing coils responsive to the magnetic
field, and a diamagnetic blocking element movable between
the magnet and the sensing coils for periodically
interrupting the magnetic field to produce electrical energy
in the coils. A preferred embodiment includes a pair of
semi-circular coils arranged side-by-side in the magnetic
field and a rotatable blocking disc interposed between the
magnet and the coils. The disc includes a semi-circular
portion of superconductive material rendered impermeable to
the magnetic field at temperatures near absolute zero and a
semi-circular portion of magnetically inert material to
alternately block and pass the magnetic field to the coils
upon rotation of the disc.

 

Current U.S. Class:  310/10 ; 310/68R; 322/49   
Current International Class:  H02K 55/00 (20060101); H02K 55/02
(20060101); H02K 011/00 ()   
Field of Search: 
310/10,40,52,168,169,170,171,191,209,154,157,113,68 322/49

 

References Cited
[Referenced By]

 

U.S. Patent Documents --  3336489 August
1967 Volger // 3393332 July 1968 Fakan //  3402307
September 1968 Pearl //  3427482 February 1969 Massar
//  3443128 May 1969 Fakan //  3467481 September
1969 Migot //  3469121 September 1969 Smith // 3478232
November 1969 Eder // 3560773 February 1971 McFarlane
//  3564307 February 1971 Kawabe //  3673444 June
1972 Kawabe

 

Other References

 

Buchold "Applications of Superconductivity",
Scientific American, vol. 202, No. 3, 1969, pp. 74-82. .   
 Volger "Dynamo for Generating Persistent
Current in a Superconducting Circuit", P.T.R., vol. 25,
1963-1964, No. 1, pp. 16-19. .   
 Appleton "Motors, Generators and Flux Pumps",
Cryogenics, 6/1969, pp. 147-157..

 

Primary Examiner: Skudy; R.   
 Attorney, Agent or Firm: Finnegan, Henderson,
Farabow, Garrett & Dunner

 

Parent Case Text

 

This is a continuation, of application Ser.
No. 719,978, filed Sept. 2, 1976, now U.S. Pat. No.
4,237,391.

 

Description

 

The present invention relates to an apparatus
for producing electrical energy and, more particularly, to
an electrical generator for transforming a stationary
magnetic field into useful electrical energy.

 

It has become increasingly important in
recent years to develop sources of electrical energy which
operate with increased efficiency. The rapidly inflating
cost of fuel, e.g., oil and gasoline, has made the operation
of generators utilizing these fuels increasingly expensive.
In addition, energy consumers have become more conscious of
the finite limits of our world-wide supply of energy. As a
result, it has become imperative to find more efficient
alternatives to the conventional sources of electrical
energy previously used.

 

The present invention contemplates the use of
a magnetic blocking device, e.g., an element which exhibits
the property of diamagnetism, to periodically interrupt a
magnetic field to generate electrical energy in a sensing
device responsive to changes in the magnetic field. Blocking
devices, such as superconductive material or plasma (ionized
gas), both of which exhibit diamagnetism, are contemplated
as suitable mechanisms for control of the magnetic field.
The invention provides for efficient transformation of the
energy of the magnetic field into an electrical output which
can be used in place of conventional sources of electrical
energy.

 

A preferred embodiment of the present
invention relies on principles of magnetism and cryogenics
to achieve an electrical generator of enhanced efficiency in
comparison with prior art devices. It is well known that, at
temperatures near absolute zero (0.degree. K.), certain
materials, e.g., niobium, become superconductive and offer
little or no resistance to the flow of electrical current.
Two (2) types of superconductive materials have been
recognized to exist. Type I or soft superconductors, usually
very pure metals, e.g., niobium, mercury, lead, aluminum,
vanadium, lanthanum and technetium, when maintained near
absolute zero, have the property of perfect diamagnetism or
negative susceptibility. This condition is represented by
the following equation:

 

where X represents susceptibility, M is the
magnetic moment per unit volume (dynes-cm/cm.sup.3), and B
is the macroscopic field intensity (gauss or flux/cm.sup.2).
In addition, Type I superconductive materials exhibit the
Meissner effect, i.e., the tendency of magnetic flux lines
to bounce off rather than penetrate the material. Further,
Type I superconductors generally exhibit a low critical
field. Type II or hard superconductors are alloys which
exhibit superconductivity at temperatures near absolute zero
but do not exhibit perfect diamagnetism or the Meissner
effect. In addition, the Type II superconductive materials
have a higher critical field than Type I superconductors.

 

With respect to the critical field property
of superconductive materials, a Type I or soft
superconductor generally has a critical field H.sub.c
(transition panel) at which the material abruptly becomes a
normal conductor. At field strengths below H.sub.c, the
material exhibits the Meissner effect, which is essentially
perfect diamagnetism, and exhibits no hysteresis. Type II or
hard superconductors have a number of transition points,
i.e., H.sub.1, H.sub.c, H.sub.2 and H.sub.3. Transition
points H.sub.c and H.sub.3 are relatively unimportant for
purposes of the present invention. At H.sub.1, which is very
low (usually much lower than H.sub.c for niobium), the Type
II material behaves as a soft superconductor. Between
H.sub.1 and H.sub.2, the Type II material is in its vortex
state. Although the Type II material is still
superconductive, it is threaded by areas of normal
conductivity. The Type II material exhibits a large amount
of hysteresis and is not perfectly diamagnetic.

 

In the preferred embodiment of the present
invention, the diamagnetic property and Meissner effect of
soft (Type I) superconductive material are exploited to
provide a generator for producing electrical energy from a
magnetic field. A soft superconductive element maintained as
a temperature near absolute zero is employed to periodically
interrupt the magnetic field, e.g., a uniform field
established by a stationary permanent magnet, to generate
electrical energy in a device, e.g., a coil, responsive to
changes in the magnetic field. The superconductive element
is located at position in the magnetic field slightly below
its critical field strength H.sub.c. Since, in contrast to a
conventional conductor, no work is required to move the soft
superconductive material across a uniform magnetic field
less than the critical field H.sub.c due to the absence of
hysteresis, the apparatus operates at a high level of
efficiency.

 

In accordance with the principles of the
invention, an apparatus for producing electrical energy
comprises a permanent magnet for establishing a magnetic
field, sensing means responsive to the magnetic field
established by the permanent magnet for producing electrical
energy in response to changes in the magnetic field, and
blocking means interposed between the permanent magnet and
the sensing means for periodically interrupting the magnetic
field from the permanent magnet. For example, the blocking
means comprises a magnetic flux blocking device of
diamagnetic material mounted for movement between the
permanent magnet and sensing means for alternately blocking
and passing the magnetic flux from the permanent magnet to
the sensing means. In a preferred embodiment, the sensing
means comprises a coil located within the magnetic field
established by the permanent magnet. The blocking means of
the preferred embodiment comprises a rotatable blocking
element of soft superconductive material rendered
impermeable to the magnetic field at temperatures near
absolute zero and adapted to alternately block and pass the
magnetic field from the permanent magnet upon rotation of
the blocking element to produce electrical energy in the
coil.

 

The invention is specifically embodied in a
generator unit adapted to be immersed in liquid helium or
other low temperature medium. The generator unit includes a
magnet and a pair of sensing coils mounted side-by-side
within the magnetic flux of the magnet. A magnetic field
control device in the form of a rotatable disc including a
semi-circular portion of soft superconductive material
rendered impermeable to the magnetic flux at temperatures
near absolute zero and a semi-circular portion of
magnetically inert material is interposed between the magnet
and sensing coils. Upon rotation of the disc and
superconductive blocking element, each coil is alternately
shielded from and exposed to the magnetic flux to produce
electrical signals in the coils.

 

The accompanying drawings illustrate a
preferred embodiment of the invention and, together with the
description, serve to explain the principles of the
invention.

 

Of the drawing:

 

FIG. 1 is a
perspective view, partially in section, of a superconductive
electrical generator constructed in accordance with the
principles of the present invention;

![](4385-1.jpg)

FIG. 2 is a vertical section of the apparatus
of FIG. 1 illustrating the arrangement of a permanent
magnet, a pair of sensing coils, and a rotatable,
superconductive blocking element for interrupting the
magnetic field from the magnet to the coils and a motor
control arrangement to rotate the blocking element;

 
 

![](4385-2.jpg)

FIG. 3 is an enlarged side view, in section,
of the superconductive blocking element;

![](4385-3.jpg)

FIG. 4 is a plan view taken along line 4--4
of FIG. 2 illustrating the relationship of the sensing coils
and superconductive blocking element; and

 

FIG. 5 illustrates an
oscilloscope circuit used to measure the electrical power
produced by the apparatus.

 

Referring to FIG. 1, the present invention is
embodied as a superconductive electrical generator unit,
generally 20, adapted to be immersed in a low temperature
vessel, e.g., a Dewar tank 22, to maintain the generator
unit at temperatures near absolute zero (0.degree. K.).
Generator unit 20 includes a circular plate or cover 24
provided with a plurality of support rods 26 extending
downwardly from the circular plate. Preferably, a set of
three (3) equidistantly spaced support rods 26 is provided
adjacent to the periphery of plate 24. Each support rod
includes a threaded portion 28 at its lower end for
receiving a pair of nuts 30 (FIG. 2). A platform 32,
consisting of a circular base, is secured to support rod 26
by nuts 30. In the preferred embodiment, the base is
provided with spaced holes (not shown) to reduce its mass.
Circular plate 24 supports a rigid tube 34 located at the
center of the plate and extending axially downward.

 

In the apparatus of the present invention, a
permanent magnet is provided for generating a magnetic
field. Referring to FIGS. 1 and 2, generator unit 20
includes a permanent magnet 36 mounted on platform 32
beneath the lower end of tube 34. The magnet preferably
consists of a solid cylindrical piece of permanently
magnetized material. Alternatively a magnet assembly
consisting of a plurality of smaller permanent magnets is
arranged in a circular configuration on platform 32. The
purpose of the permanent magnet is to establish a
stationary, uniform magnetic field for the generator.

 

In accordance with the present invention, the
apparatus is provided with sensing means responsive to the
magnetic field established by the permanent magnet for
producing electrical energy in response to changes in the
magnetic field. Preferably, the sensing means comprises one
or more coils located within the magnetic field established
by the permanent magnet. Referring to FIG. 1, a pair of
coils 38 is mounted at the lower end of tube 34, e.g., by
conventional bonding technique or other adhesive. Each coil
consists of a plurality of turns of insulated wire and
includes a set of leads 40 for electrical connection to an
output circuit. The coils are arranged in a side-by-side
configuration to respond to different portions of the
magnetic flux from permanent magnet 36.

Further, in accordance with the invention,
blocking means is interposed between the permanent magnet
and the sensing means for periodically interrupting the
magnetic field from the permanent magnet. Preferably, a
magnetic field control device mounted for movement between
the permanent magnet and sensing coil includes an element of
diamagnetic material for shielding the sensing coil from the
magnetic field upon interposition of the element between the
magnet and the coil. In the preferred embodiment, the
magnetic field control device comprises a rotatable blocking
element of soft superconductive material rendered
impermeable to the magnetic field at temperatures near
absolute zero and adapted to alternately block and pass the
magnetic field from the permanent magnet upon rotation of
the blocking element to produce electrical energy in the
coil.

 

Referring to FIGS. 1 and 2, a disc, generally
42, is rotatably mounted between permanent magnet 36 and
sensing coils 38. The disc is attached at the lower end of a
shaft 44 rotatably mounted within tube 34 by a plurality of
sleeve bearings 45 provided at spaced locations in the tube.
A magnetic control element 46, e.g., a piece of magnetized
material such as alnico 8, is mounted on tube 34 to permit
the demagnetizing effects of temperature and other
conditions to be determined. The upper end of shaft 44 is
connected through a coupling 47 to a motor 48 mounted on a
circular platform 50 supported by a plurality of rods 52
extending upward from circular plate 24. Each rod 52 is
provided with a threaded portion 54 at its upper end for
receiving a pair of nuts 56 which are employed to clamp
platform 50 to the rods.

 

Since tube 34 and shaft 44 provide a heat
conductive path from the interior to the exterior of the low
temperature vessel, it is contemplated that these components
can be constructed to minimize the amount of heat transfer
from the vessel. For example, the tube and shaft can be
constructed of insulating material, e.g., a rigid plastic
such as teflon, to minimize heat conduction. Further, it is
contemplated that alternative pressure or magnetic coupling
arrangements, which do not require mechanical connection
between the motor and the disc, can be provided to eliminate
the requirement of a continuous shaft extending from the
interior to the exterior of the vessel.

 

Referring to FIGS. 3 and 4, the magnetic
field control device consists of a thin, semi-circular
element 58 of niobium placed between a pair of circular
elements 60 of magnetically inert material. Alternatively,
other soft superconductive material, e.g., mercury, lead,
aluminum, vanadium, lanthanum, or technetium may be used in
place of niobium, if desired. In addition, it is possible to
employ hard superconductive materials with an appropriate
adjustment in the magnetic field strength. Niobium element
58 and magnetically permeable elements 60 are held together
by any suitable arrangement, e.g., bonding or adhesive tape.
The resulting disc comprises a semi-circular portion of soft
superconductive material (niobium) rendered impermeable to
the magnetic flux at temperatures near absolute zero and a
semi-circular portion of magnetically inert material. Disc
42 is located in a position relative to permanent magnet 36
to place superconductive element 58 at a magnetic field
strength slightly below its critical field.

 

Alternatively, it is contemplated that
mechanisms other than a superconductive blocking element can
be used to provide a suitable magnetic field blocking
device. For example, in the field of plasma physics, it is
recognized that ionized gases known as plasmas exhibit the
property of diamagnetism. Such materials, if confined in a
suitable container, would be appropriate, in place of the
soft superconductive material of the preferred embodiment,
to provide a unit in which the magnetic field applied to the
sensing coils is periodically interrupted. Of course, such a
modified device would not require the low temperature medium
of the preferred embodiment.

As shown in FIG. 2, a voltage supply circuit
including a variable power supply 62 for converting
conventional AC voltage to DC voltage provides a suitable DC
voltage input for operating motor 48. A common current
wattmeter 64 is connected across the AC input lines to the
variable power supply to indicate the power consumption of
the motor.

 

The circuit of FIG. 5 is used to determine
the output power produced by the generator. This circuit
includes a variable resistor 66 and an ammeter 68 which can
be connected in series across either coil 38 of the
generator. The resistance serves as a load and the ammeter
measures the load current. In addition, an oscilloscope 70
is connected across the coil to measure the output voltage.
The product of the load current and output voltage equals
the output power.

 

In the operation of the apparatus, generator
unit 20 is inserted into Dewar tank 22 with circular plate
24 resting on the upper edge of the tank. Liquid helium is
applied to the interior of the tank up to the dashed line
shown in FIG. 2 to cool the niobium element to a temperature
near absolute zero. The position of disc 42 is set relative
to magnet 36 by adjustment of platform 50 on rods 52 to
locate niobium element 58 slightly above the position at
which the flux density of the magnetic field renders the
niobium element a normal conductor. At temperatures near
absolute zero, niobium exhibits diamagnetism and the
Meissner effect. Thus, when interposed between magnet 36 and
either of the coils, niobium element 58 blocks the magnetic
flux from the magnet to the coil.

 

When motor 48 is energized to rotate disc 42,
niobium element 58 operates to alternately block and pass
the magnetic flux from magnet 36 to coils 38. When niobium
element 58 is located entirely below either coil, the coil
is completely shielded from the magnetic flux. At the same
time, the other coil is completely exposed to the magnetic
flux. At all other times, each coil is partially shielded
and partially exposed to the magnetic flux.

 

As a result of rotation of disc 42 and
niobium element 58, each coil 38 is subjected to a
continuously changing magnetic field. A voltage is induced
in each coil which is proportional to the rate of change of
the magnetic flux through the coil. When the coil is
connected to an output circuit, such as the circuit of FIG.
5, the output power produced by the generator can be
determined by measuring its output voltage and load current.

 

Example

 

In a specific example of a generator unit
constructed according to the principles of the present
invention, circular plate or cover 24 is made of aluminum
six and three-quarter inches (63/4") in diameter and one
inch (1") in thickness. It serves as a cover for Dewar tank
22 which has an inner diameter of five and three-quarter
inches (53/4"). Support rods 26 comprise hollow stainless
steel tubes with a wall thickness of 0.03 inch and an outer
diameter of one-half inch (1/2"). Platform 32 is made of
steel one-eight inch (1/8") in thickness and is provided
with spaced holes (not shown) approximately one-half inch
(1/2") in diameter to reduce its mass.

Tube 34 is made of stainless steel with an
outer diameter of one and one-half inches (11/2") and an
inner diameter of 1.435 inches. Magnet 36 comprises a
substantially circular assembly of bar magnets of alnico 8
material. The magnet has a maximum field strength of
approximately 4800 gauss.

 

Each coil 38 consists of AWG #18 wire and
includes approximately one hundred (100) turns. Each coil is
substantially semi-circular in configuration with a radius
of 2.25 inches, a height of 0.7 inch, and a depth of 0.2
inch.

 

Shaft 44 is made of stainless steel
one-eighth inch (1/8") in diameter. Disc 42 attached to the
lower end of shaft 44 includes semi-circular element 58 of
niobium, approximately 0.001 inch in thickness and 99.84%
pure, and two (2) circular elements 60 composed of
cardboard. The disc is approximately four and one-half
inches (41/2") in diameter.

 

In a representative operation, the position
of disc 42 was set by adjustment of the level of platform 50
to place the disc slightly above the flux density
(approximately 2000 gauss) at which niobium element 58
behaves as a normal conductor. The disc was rotated at one
thousand (1000) revolutions per minute and readings on each
coil 38 were taken. The value of resistance 66 (FIG. 5) was
varied. The wattage consumed by motor 48 was roughly 7 watt
plus or minus 2.5 watts. The wattage output measured by the
circuit of FIG. 5 was approximately 11.4 watts maximum. The
V.sub.RMS of each coil was 1.14 volts plus or minus 0.5
volts. V.sub.MAX was 1.612 volts and I.sub.RMS was about 10
amps. Wattmeter readings were divided by the product of the
oscilloscope and ammeter readings to determine the power
factor which was very close to unity.

 

The generator unit of the present invention
provides a highly efficient device for producing electrical
energy from a magnetic field. It produces an enhanced
electrical output in comparison with the input energy
required to drive the unit. It is anticipated that a portion
of the enhanced electrical output can be used for operation
of the cooling apparatus to provide liquid helium and
another portion of the electrical output can be used to
provide input energy to drive the motor of the generator
unit.

The invention in its broader aspects is not
limited to the specific details shown and described, and
modifications may be made in the details of the generator
unit without departing from the principles of the present
invention.

---

**http://v3.espacenet.com/publicationDetails/biblio?adjacent=true&KC=A&date=19801202&NR=4237391A&DB=EPODOC&locale=en\_EP&CC=US&FT=D**



**US4237391** **Apparatus for producing electrical
energy**

  
1980-12-02

Abstract -- An electrical generator comprises a stationary
permanent magnet for establishing a magnetic field, one or
more sensing coils responsive to the magnetic field, and a
diamagnetic blocking element movable between the magnet and
the sensing coils for periodically interrupting the magnetic
field to produce electrical energy in the coils. A preferred
embodiment includes a pair of semi-circular coils arranged
side-by-side in the magnetic field and a rotatable blocking
disc interposed between the magnet and the coils. The disc
includes a semi-circular portion of superconductive material
rendered impermeable to the magnetic field at temeperatures
near absolute zero and a semi-circular portion of magnetically
inert material to alternately block and pass the magnetic
field to the coils upon rotation of the disc.

---

http://appft1.uspto.gov/netacgi/nph-Parser?Sect1=PTO2&Sect2=HITOFF&p=1&u=%2Fnetahtml%2FPTO%2Fsearch-bool.html&r=1&f=G&l=50&co1=AND&d=PG01&s1=Abolafia.IN.&OS=IN/Abolafia&RS=IN/Abolafia
  
http://v3.espacenet.com/publicationDetails/biblio?adjacent=true&KC=A1&date=20090326&NR=2009082208A1&DB=EPODOC&locale=en\_EP&CC=US&FT=D

USP App 20090082208   
SUPERCONDUCTING GENERATOR

  
2009-03-26   
Also published as:  WO2009038939

Abstract -- A generator that comprises at least one
ferromagnetic core including a gap, a magnet capable of
producing a normal magnetic field within said gap and at least
one coil positioned within the normal magnetic field on the
core. At least one diamagnet that is positioned to pass
through said gap on said core, wherein the diamagnet
momentarily blocks the normal magnetic field causing a voltage
to be induced within said coil.

BACKGROUND OF THE INVENTION

[0001] The invention relates to generators.

BRIEF SUMMARY OF THE INVENTION

[0002] A first embodiment of the invention is a generator
comprising at least one ferromagnetic core including a gap; a
magnet positioned on said at least one ferromagnetic core
producing a normal magnetic field within said gap; at least
one coil positioned within the normal magnetic field on said
at least one ferromagnetic core; at least one diamagnet
rotatably positioned to pass through said gap on said at least
one ferromagnetic core, wherein rotation of said at least one
diamagnet that momentarily blocks the normal magnetic field
causing a voltage to be produced withing said at least one
coil.

[0003] A second embodiment of the invention is a
superconducting generator comprising: at least one rotatable
ferromagnetic core including a gap; a magnet positioned on
said at least one ferromagnetic core producing a normal
magnetic field; a coil positioned within the field on said at
least one ferromagnetic core; and at least one fixed
superconducting diamagnet positioned to pass through said gap
on said at least one ferromagnetic core when said core is
rotated.

[0004] A third embodiment of the invention is
a superconducting generator comprising: a plurality of
ferromagnetic cores arranged in a circle, wherein each core
includes a gap; a magnet positioned on each of said
plurality of ferromagnetic cores producing a normal magnetic
field within each said core and said gap; at least one coil
positioned within the normal magnetic field on each said
plurality of ferromagnetic cores; a plurality of
superconducting diamagnet positioned and configured to pass
through each said gap on said plurality of ferromagnetic
cores, wherein rotation of either said plurality of
superconducting diamagnets or plurality of ferromagnetic
cores with respect to each other momentarily blocks the
normal magnetic field causing a voltage to be produced
withing said at least one coil.

 

BRIEF DESCRIPTION OF THE DRAWINGS

 

[0005] Some of the embodiments of this
invention will be described in detail, with reference to the
following figures, wherein like designations denote like
members, wherein:

 

[0006] FIG. 1 depicts a side view of the core;

 


![](uspa1.jpg)

 

[0007] FIG. 2 depicts a side view of a second embodiment of the
core;

 


![](uspa2.jpg)

 

[0008] FIG. 3 depicts a diamagnetic superconductor that is
optionally encased with a dewar;

 


![](uspa3.jpg)

 

[0009] FIG. 4 depicts a plurality of cores with a centrally
facing gap and a plurality rotated superconductor;

 


![](uspa4.jpg)

 

[0010] FIG. 5 depicts a plurality of rotating cores with an
externally facing gap and a plurality of externally mounted
fixed diamagnets;

 


![](uspa5.jpg)

 

[0011] FIG. 6 depicts a top view of a plurality of cores
arranged in a circular pattern that are rotated to move
fixed diamagnets within that gap;

 


![](uspa6.jpg)

 

[0012] FIG. 7 depicts a top view of a plurality of diamagnets
rotated within a circular formation of inwardly facing
cores; and

 


![](uspa7.jpg)

 

[0013] FIG. 8 depicts a side view of a stacked circular
arrangement of cores and diamagnets.

![](uspa8.jpg)

DETAILED DESCRIPTION OF THE INVENTION

 

[0014] Although certain preferred embodiments
of the present invention will be shown and described in
detail, it should be understood that various changes and
modifications may be made without departing from the scope
of the appended claims. The scope of the present invention
will in no way be limited to the number of constituting
components, the materials thereof, the shapes thereof, the
relative arrangement thereof, etc., and are disclosed simply
as an example of an embodiment. The features and advantages
of the present invention are illustrated in detail in the
accompanying drawings, wherein like reference numerals refer
to like elements throughout the drawings.

 

[0015] As a preface to the detailed
description, it should be noted that, as used in this
specification and the appended claims, the singular forms
"a", "an" and "the" include plural referents, unless the
context clearly dictates otherwise. In the invention a
diamagnet 200, which may be from a superconducting material,
acts as a blocking device that moves with respect to a gap
115 in a core 110 having a magnetic field 130 that includes
a coil 140, wherein the diamagnet 200 periodically shields
and unshields the magnetic field 130 inducing an EMF
(Electro Motive Force) generating a voltage or current 195
from the coil 140. The invention provides for the efficient
transformation of the energy of the magnetic field 130 into
electrical energy from movement of the diamagnet 200 with
respect to the gap 115 in the core 110.

 

[0016] Faraday's Law states that the induced
emf around a closed mathematical path in a magnetic field is
equal to the rate of change of magnetic flux intercepted by
the area within the path. Inefficient systems can use large
amounts of energy to change the magnetic flux and produce
the electromotive force while more efficient methods for
changing the flux may be used to produce the same
electromotive force for far less energy. Thus, the
efficiency in the production of the emf is a product of the
efficiency in changing the magnetic flux which passes
through the closed circuit.

 

[0017] The blocking of the magnetic field 130
in the core 110 occurs when a diamagnetic object passes
through the gap 115, where the diamagnetism is caused by the
Meissner effect of superconductive materials (i.e., the
diamagnetic properties of a superconductive material 200 may
occur in specific materials when operating at a temperature
below its transition temperature) that are exploited to
provide a device 100 for producing electrical energy from a
magnetic field 130. A superconductive element 200, either a
high temperature or low temperature type, is maintained at a
temperature immediately below its transition temperature or
colder and periodically it acts to shield a coil 140 from a
magnetic field established by a permanent or electromagnet
120 causing a changing flux within the coil 140 to induce
and EMF.

 

[0018] A ferromagnetic core 110 is used that
has suitable properties to establish a magnetic field 130
within its body with a magnet 20. The core 110 may be a
circular or closed geometric shape, such as a square to
allow a continuous magnetic field to be guided. The core 110
can also be made of electrical steel, also called lamination
steel, silicon electrical steel, silicon steel or
transformer steel, all of which are specialty steels
tailored to produce certain magnetic properties, such as a
small hysteresis area (small energy dissipation per cycle,
or low core loss) and high permeability. The core material
110 may be manufactured in the form of cold-rolled strips
less than 2 nm thick called laminations that may form a core
110 when stacked together. Laminations may be cut to their
finished shape by a punch and die, or in smaller quantities
may be cut by a laser. The core 110 of the instant invention
may be shaped in any manner that allows a magnetic loop 130
to be formed within and across the gap 115.

 

[0019] A coil 140 induces an EMF in response
to the magnetic field 130 that passes through a gap 115
within the core 110 that is temporarily blocked or disrupted
when a diamagnet 200 is interposed between the field of the
magnet 120 and the coil 140 by passing within the gap 115 of
the core 110. The magnetic field 130 within the core 110 can
be from either a permanent or electromagnet 120. The
diamagnet 200 is a magnetic flux shielding device that moves
with respect to the gap 115 in the core 110 to alternately
shield and unshield the magnetic flux from the coil 140. The
core 110 as discussed above may be made of a ferro-magnetic
material such as transformer steel or the like which would
enclose and confine the field of the magnet dipole 120 to
ensure that it passes through the gap 115. The invention is
not effected by the position of the coil 140 and magnet 120,
which may be placed anywhere upon the core 110.

 

[0020] A superconducting generator 100 of the
invention comprises at least one ferromagnetic core 110
including a gap 115 having a magnet 120 positioned on the
ferromagnetic core 110 producing a normal magnetic field 130
within said gap 115 and at least one coil 140 positioned
within the normal magnetic field 130 on said at least one
ferromagnetic core 110 as shown in FIGS. 1 and 2. The
superconductor generator 100 includes at least one
superconducting diamagnet 200 that is rotatably positioned
adjacent to said core 110 to allow the diamagnet 200 to pass
through said gap 115 as shown in FIG. 4. An EMF is induced
in the coil 140 on the ferromagnetic core 110 when rotation
of said at least one superconducting diamagnet 200
momentarily blocks the normal magnetic field 130 causing a
changing magnetic flux within at least one coil 140.

 

[0021] The blocking device 200 must be kept
below the transition temperature of the specific
superconducting material used, either type I or type II or
the Meisner effect is temporarily destroyed removing the
properties of diamagnetism and therefore preventing blocking
of the magnetic field 130 passing through the gap 115. One
solution to maintain diamagnetism properties of the
superconductor is to cool the whole superconducting
apparatus 100 including the core 110, magnet 120 and coil
140 along with the diamagnet 200 and all attached assemblies
below the superconducting material's critical temperature
used in the application. Another option is by having the
superconducting generator 100 further comprise, as shown in
FIG. 3, a dewar 225 surrounding said superconducting
diamagnet 200, said dewar 225 is dimensioned to pass through
the gap 115 on the core 110. The use of a dewar 225
dimensioned to pass within the gap 115 of the core 110
allows for cooling only of the diamagnetic material 200 and
the remaining constituents of the generator 100 remain at a
more economically desirable temperature above the critical
temperature of the superconductor 200 that is desirable from
the standpoint of cooling costs and storage requirements.

 

[0022] A superconductor placed in a weak
external magnetic field H 130 permits the field 130 to
penetrate the superconductor a short distance called the
London penetration depth before it decays rapidly to zero
(blocked), which is called the Meissner effect, and is a
defining characteristic of superconductivity. The Meissner
effect is different than the diamagnetism in a perfect
electrical conductor that according to Lenz's law, when a
changing magnetic field is applied to a conductor, it will
induce an electrical current in the conductor that creates
an opposing magnetic field. In a perfect conductor, an
arbitrarily large current can be induced, and the resulting
magnetic field exactly cancels the applied field.

 

[0023] The Meissner effect is distinct from
this because a superconductor expels all magnetic fields,
not just those that are changing. Suppose we have a material
in its normal state, containing a constant internal magnetic
field that when the material is cooled below the critical
temperature (Tc), we would observe the abrupt expulsion of
the internal magnetic field, which we would not expect based
on Lenz's law.

[0024] The Meissner effect breaks down when
the applied magnetic field 130 is too large and thus ceases
to be able to function as a diamagnet. Type I
superconductors may be abruptly destroyed
(superconductivity) when the strength of the applied field
rises above a critical value Hc. Depending on the defects
and flux pinning of the sample, one may obtain an
intermediate state consisting of regions of normal material
carrying a magnetic field mixed with regions of
superconducting material containing no field. In Type II
superconductors, raising the applied field past a critical
value H.sub.c1 leads to a mixed state in which an increasing
amount of magnetic flux penetrates the material, but there
remains no resistance to the flow of electrical current as
long as the current is not too large. At a second critical
field strength Hc2, superconductivity is destroyed because
the mixed state is actually caused by vortices in the
electronic superfluid, sometimes called fluxons because the
flux carried by these vortices is quantized. Therefore, the
magnetic field 130 in the core 110 of the generator 100 must
use a magnetic source 120 weaker than Hc with Type 1
superconductors and weaker than H.sub.c1 for Type 2
superconductors.

 

[0025] The diamagnet of the invention may be
a type 1 superconductors that may require the coldest
temperatures to become superconductive and are elemental and
very pure in nature. The type 1 superconductors listed below
exhibit a very sharp transition to a superconducting state
and a "perfect" diamagnetism the ability to repel a magnetic
field completely. The instant invention may use the Type 1
superconductor Niobium (Nb) that below a temperature of 8K
has an Hc of about 2,000 gauss, which has the highest Hc of
the currently known type 1 and type 2 superconductors.

 

[0026] Below is a list of other known Type 1
superconductors along with their critical transition
temperature (known as Tc) below which each superconducts.
Lead (Pb) 7.196 K; Lanthanum (La) 4.88 K; Tantalum (Ta) 4.47
K; Mercury (Hg) 4.15 K; Tin (Sn) 3.72 K; Indium (In) 3.41 K;
Palladium (Pd)\* 3.3 K; Chromium (Cr)\* 3 K; Thallium (Tl)
2.38 K; Rhenium (Re) 1.697 K; Protactinium (Pa) 1.40 K;
Thorium (Th) 1.38 K; Aluminum (Al) 1.175 K; Gallium
(Ga)1.083 K; Molybdenum (Mo) 0.915 K; Zinc (Zn) 0.85 K;
Osmium (Os)0.66 K; Zirconium (Zr)0.61 K; Americium (Am) 0.60
K; Cadmium (Cd) 0.517 K; Ruthenium (Ru) 0.49 K; Titanium
(Ti) 0.40 K; Uranium (U)0.20 K; Hafnium (Hf)0.128 K; Iridium
(Ir) 0.1125 K; Beryllium (Be)0.023 K (SRM 768); Tungsten
(W)0.0154 K; Platinum (Pt)\* 0.0019 K; Lithium (Li)0.0004 K;
Rhodium (Rh) 0.000325K

 

[0027] The next superconducter possible to
use is a Type 2 category of superconductors that includes
metallic compounds and alloys. The highest Tc attained at
ambient pressure for a material that will form
stoichiometrically (by formula) has been 138 K and a patent
has been applied for a 150K material which does not form
stoichiometrically (see below list). Type 2 superconductors
differ from Type 1 in that their transition from a normal to
a superconducting state is gradual across a region of "mixed
state" behavior. A Type 2 will allow some penetration by an
external magnetic field into its surface. While there are
far too many known to one skilled in the art to list in
totality, some of the more interesting Type 2
superconductors are listed below by similarity and with
descending Tc's

 

[0028] One skilled in the art would naturally
substitute a later discovered type 2 superconductor having
superior properties and higher Tc and should be considered
as an equivalent. While type 2 superconductors known
currently have a much higher Tc than type 1 superconductors
the critical magnetic field is an order of magnitude smaller
at about 200 gauss than Niobium (Nb) having 2,000 gauss,
which directly impacts the amount of current generated by
each coil 140 on each core 110.

 

[0029] A partial list of suitable type 2
superconductors than may be used is as follows:
InSnBa.sub.4Tm.sub.4Cu.sub.6O.sub.18+.about.150 K;
(Hg.sub.0.8Tl.sub.0.2)Ba.sub.2Ca.sub.2Cu.sub.38.33138K;
HgBa.sub.2Ca.sub.2Cu.sub.3O.sub.8 133-135K;
HgBa.sub.2Ca.sub.3Cu.sub.4O.sub.10+ 125-126K;
HgBa.sub.2(Ca.sub.1-xSr.sub.x)Cu.sub.2O.sub.6+ 123-125K;
HgBa.sub.2CuO.sub.4+ 94-98K;
Tl.sub.2Ba.sub.2Ca.sub.2Cu.sub.3O.sub.10 127-128K;
(Tl.sub.1.6Hg.sub.0.4)Ba.sub.2Ca.sub.2Cu.sub.3O.sub.10+123K;
TlBa.sub.2Ca.sub.2Cu.sub.3O.sub.9+ 118-120K;
(Tl.sub.0.5Pb.sub.0.5)Sr.sub.2Ca.sub.2Cu.sub.3O.sub.9 118K;
Tl.sub.2Ba.sub.2CaCu.sub.2O.sub.6 115K;
(Tl.sub.0.5Sn.sub.0.5)Ba.sub.2(Ca.sub.0.5Tm.sub.0.5)Cu.sub.2O.sub.x
112K; TlBa.sub.2Ca.sub.3Cu.sub.4O.sub.11 103K;
TlBa.sub.2CaCu.sub.2O.sub.7+ 95K;
Sn.sub.2Ba.sub.2(Ca.sub.0.5Tm.sub.0.5)Cu.sub.3O.sub.8+ 115K;
SnInBa.sub.4Tm.sub.3Cu.sub.5O.sub.x 113K;
Sn.sub.3Ba.sub.4Tm.sub.3Cu.sub.6O.sub.x 109K;
Sn.sub.3Ba.sub.8Ca.sub.4Cu.sub.11O.sub.x 109K;
SnBa.sub.4Y.sub.2Cu.sub.5O.sub.x 105K;
Sn.sub.4Ba.sub.4Tm.sub.2YCu.sub.7O.sub.x 104K;
Sn.sub.4Ba.sub.4CaTmCu.sub.4O.sub.x 100K;
Sn.sub.4Ba.sub.4Tm.sub.3Cu.sub.7O.sub.x 98K;
Sn.sub.2Ba.sub.2(Y.sub.0.5Tm.sub.0.5)Cu.sub.3O.sub.8+ 96K;
Sn.sub.3Ba.sub.4Y.sub.2Cu.sub.5O.sub.x 91K;
SnInBa.sub.4Tm.sub.4Cu.sub.6O.sub.x 87K;
Sn.sub.2Ba.sub.2(Sr.sub.0.5Y.sub.0.5)Cu.sub.3O.sub.8 80K;
Sn.sub.4Ba.sub.4Y.sub.3Cu.sub.7O.sub.x 80K;
Bi.sub.1.6Pb.sub.0.6Sr.sub.2Ca.sub.2Sb.sub.0.1Cu.sub.3O.sub.y
115K; Bi.sub.2Sr.sub.2Ca.sub.2Cu.sub.3O.sub.10 110K;
Bi.sub.2Sr.sub.2CaCu.sub.2O.sub.9 110K;
Bi.sub.2Sr.sub.2(Ca.sub.0.8Y.sub.0.2)Cu.sub.2O.sub.8 95-96K;
Bi.sub.2Sr.sub.2CaCu.sub.2O.sub.8 91-92K;
(Ca.sub.1-xSr.sub.x)CuO.sub.2 110K;
YSrCa.sub.2Cu.sub.4O.sub.8+ 101K; (Ba,Sr)CuO.sub.2 90K;
BaSr.sub.2CaCu.sub.4O.sub.8+ 90K; (La,Sr)CuO.sub.2 42K;
Pb.sub.3Sr.sub.4Ca.sub.3Cu.sub.6O.sub.x 106K;
Pb.sub.3Sr.sub.4Ca.sub.2Cu.sub.5O.sub.15+ 101K;
(Pb.sub.1.5Sn.sub.1.5)Sr.sub.4Ca.sub.2Cu.sub.5O.sub.15+ 95K;
Pb.sub.2Sr.sub.2(Ca, Y)Cu.sub.3O.sub.8 70K;
AuBa.sub.2Ca.sub.3Cu.sub.4O.sub.11 99K; AuBa.sub.2(Y,
Ca)Cu.sub.2O.sub.7 82K; AuBa.sub.2Ca.sub.2Cu.sub.3O.sub.9
30K; (Y.sub.0.5Lu.sub.0.5)Ba.sub.2Cu.sub.3O.sub.7 107K;
(Y.sub.0.5Tm.sub.0.5)Ba.sub.2Cu.sub.3O.sub.7 105K;
(Y.sub.0.5Gd.sub.0.5)Ba.sub.2Cu.sub.3O.sub.7 97K;
Y.sub.2CaBa.sub.4Cu.sub.7O.sub.16 97K;
Y.sub.3Ba.sub.4Cu.sub.7O.sub.16 96K;
NdBa.sub.2Cu.sub.3O.sub.7 96K; Y.sub.2Ba4Cu.sub.7O.sub.15
95K; GdBa.sub.2Cu.sub.3O.sub.7 94K; YBa.sub.2Cu.sub.3O.sub.7
92K; TmBa.sub.2Cu.sub.307 90K; YbBa.sub.2Cu.sub.307 89K;
YSr.sub.2Cu.sub.307 62K;
GaSr.sub.2(Ca.sub.0.5Tm.sub.0.5)Cu.sub.2O.sub.7 99K;
Ga.sub.2Sr.sub.4Y.sub.2CaCusO, 85K;
Ga.sub.2Sr.sub.4.TM..sub.2CaCusO5 81K;
La.sub.2Ba.sub.2CaCu.sub.5O.sub.9+79K;
(Sr,Ca).sub.5Cu.sub.4Oi.sub.0 70K; GaSr.sub.2(Ca,
Y)Cu.sub.2O.sub.7 70K;
(In.sub.0.3Pb.sub.0.7)Sr.sub.2(Ca.sub.0.8Yo..sub.2)Cu.sub.2Ox
60K; (La,Sr,Ca).sub.3Cu.sub.2O.sub.6 58K;
La.sub.2CaCu.sub.2O.sub.6+45K;
(Eu,Ce).sub.2(Ba,Eu).sub.2Cu.sub.3O.sub.10+43K; (Lal
0.85Sro. .sub.5)CuO.sub.4 40K; SrNdCuO 40K;
(La,Ba).sub.2CuO.sub.4 35-38K; (Nd,Sr,Ce).sub.2CuO.sub.4
35K; Pb.sub.2(Sr,La).sub.2Cu.sub.206 32K;
(Lal..sub.85Ba..sub.15)CuO.sub.4 30K; MgB.sub.2 39K;
Ba.sub.0.6K.sub.04BiO.sub.3 30K; Nb.sub.3Ge 23.2K;
Nb.sub.3Si 19K; Nb.sub.3Sn 18.1K; Nb.sub.3Al 18K;
V.sub.3Si17.1K; Ta.sub.3Pb 17K; V.sub.3Ga 16.8K; Nb.sub.3Ga
14.5K; V.sub.3In 13.9K; PuCoGa.sub.5 18.5K; NbN 16.1K; and
many others.

 

[0030] The superconducting generator 100 of
FIG. 7 may further comprise a rotatable carrier 300, wherein
said at least one superconducting diamagnet 200 is mounted
thereupon. A coolant 325 may be provided to the
superconducting diamagnets 200 to prevent transition to the
normal state through supports including circulating conduits
330. The superconducting generator 100 further comprises a
rotatable shaft 310 connected to said rotatable carrier 300,
wherein said rotatable shaft contains ducts 320 to circulate
said coolant 325. In addition to the coolant circulation 325
an insulating member 225 may surround said at least one
superconducting diamagnet 200 to maintain a temperature
sufficient to maintain superconductivity through proving
insulation.

 

[0031] The superconducting generator 100
includes a magnet 120 on each core 110 that may either be a
permanent magnet or an electromagnet. The magnet 120 is
selected to produce a field strength below the critical
field strength (saturation point) of the selected
superconductor, which is about 200 gauss for a Type 2
superconductor. The superconducting generator 400 of FIG. 7
shows an embodiment of a device 400 with an arrangement of a
plurality of cores 111 that allows increased electrical
higher output while using a higher temperature Type 2
superconductor 200 having an Hc of 200 gauss or less wherein
a plurality of ferromagnetic cores 111 are arranged in a
circle, wherein said gap 115 faces inwards. A plurality of
rotatable carriers 330 each having at least one
superconducting diamagnet 200 is mounted thereupon in a
circularly spaced fashion to allow rotation. The amount of
diamagnets 200 and cores 111 present are determined by the
rotational force (torque) provided to a rotatable shaft 310
connected to said plurality of rotatable carriers 330. The
plurality of ferromagnetic cores 111 are arranged in a
circle forming a ring of magnetic fields 131, wherein each
of said plurality of rotatable carriers 200 rotates within
said ring of magnetic fields 131 by passing through the gap
115. The number of cores, and diamagnets are determined by
the torque input, desired output, the strength of the
diamagnet that determine individual field strength that
directly correlates to individual coil outputs and required
operating temperature.

 

[0032] Another embodiment of the
superconducting generator 500 as shown in FIG. 6 comprises
at least one rotatable ferromagnetic core 110, 710 including
a gap 115 having a magnet 120 positioned on said
ferromagnetic core 110 producing a normal magnetic field
130. A coil 140 is positioned within the field 130 on each
ferromagnetic core 110, 710. The core 110 is rotated in
relation to at least one fixed superconducting diamagnet 200
that is positioned to pass through said gap 115 on said at
least one ferromagnetic core 110, 710 when said core 110 is
rotated.

 

[0033] The superconducting generator 600 may
further comprising a positioning member 410, wherein a
plurality of superconducting diamagnets 420 are mounted
thereupon in a circularly spaced fashion. A plurality of
ferromagnetic cores 710 arranged in a circle forming a ring
of parallel magnetic fields 720, wherein said ring of
parallel magnetic fields 720 is rotated so that said
plurality of superconducting diamagnets 420 on the
positioning member blocks said ring of parallel magnetic
fields 720 during rotation.

 

[0034] The superconducting generator 600 of
FIG. 6 further comprises a vessel 520 having a wall 525 that
may include insulation 528 and cryogen 530 therein
circulating to cool the plurality of superconducting
diamagnets 200 that are mounted to extend therefrom in a
circularly spaced fashion on said wall 525 of said vessel
520. A rotatable shaft 550 is operably attached to a
plurality of ferromagnetic cores 710 arranged in a circle.
The plurality of cores 710 are not in physical or electrical
contact so as to form a ring of parallel magnetic fields 730
that are mounted to said rotatable shaft 550. The plurality
of ferromagnetic cores 710 have said gap 115 facing outwards
and is positioned within said vessel 520 so that said
diamagnets 200 on said vessel wall 525 momentarily blocks
said fields 730 during rotation when passing within said gap
115. The superconducting generator 600 may include a cryogen
or cryogenic refrigeration 530 within said vessel wall 525
to chill said attached, affixed or partially embedded
superconducting diamagnets 200 to allow the plurality of
ferromagnetic cores 710 to be maintained at a temperature
above a critical superconducting temperature.

 

[0035] The dewar 225 as shown in FIG. 3 may
be made of glass, stainless steel or any other material that
does not have magnetic or electric properties at the low
required temperatures below the Tc of the superconductor
200. The shape of the superconductor 200 within the dewar
225 can be modified to adjust the output waveform of the
coil 140. The diamagnet shape 202 may be changed to a
circular shape, square, rectangular, or rod like to create a
square, triangular or sinusoidal wave pattern from said EMF
output of said coil 140.

 

[0036] A superconducting generator 800 as
shown in FIG. 8 comprises a plurality of ferromagnetic cores
810 arranged in a circle, wherein each core as shown in FIG.
1 includes a gap 115 and a magnet 120 that produces a normal
magnetic field 130 within each core 110 and across the gap
115. There is at least one coil 140 positioned within the
normal magnetic field 130 on each ferromagnetic core. The
plurality of cores arranged in a circle 810 may be stacked
upon each other and share a common rotation shaft 820 that
can be configured to rotate either the plurality of cores
arranged in a circle 810 or a plurality of superconducting
diamagnets 220 positioned and configured to pass through
each said gap 115 on said plurality of ferromagnetic cores
810. The rotation of the shaft 820 depending on the desired
configuration allows movement of either said plurality of
superconducting diamagnets 220 or plurality of ferromagnetic
cores 810 with respect to each other to momentarily block
the normal magnetic field 130 causing a voltage to be
produced within said at least one coil 140.

 

[0037] Various modifications and variations
of the described apparatus and methods of the invention will
be apparent to those skilled in the art without departing
from the scope and spirit of the invention. Although the
invention has been described in connection with specific
embodiments, outlined above, it should be understood that
the invention should not be unduly limited to such specific
embodiments. Various changes may be made without departing
from the spirit and scope of the invention as defined in the
following claims.

  


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FR2422280   
 GENERATEUR ELECTRIQUE POUR
TRANSFORMER UN CHAMP MAGNETIQUE STATIONNAIRE EN ENERGIE
ELECTRIQUE UTILE

 

EC:   H02K55/02 
IPC:   H02K55/02; H02K55/00; (IPC1-7): H02K21/00   
 1979-11-02

  


---

 


DE2813794   
 EINRICHTUNG ZUR ERZEUGUNG VON
ELEKTRISCHER ENERGIE

 

EC:   H02K21/38; H02K55/02 
IPC:   H02K21/38; H02K55/02; H02K21/00; (+2)   
 1979-10-11

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