Abstract:
The invention describes a product and a method for generating electrical power directly from nuclear power. More particularly, the invention describes the use of a liquid semiconductor as a means for efficiently converting nuclear energy, either nuclear fission and/or radiation energy, directly into electrical energy. Direct conversion of nuclear energy to electrical energy is achieved by placing nuclear material in close proximity to a liquid semiconductor. Nuclear energy emitted from the nuclear material, in the form of fission fragments or radiation, enters the liquid semiconductor and creates electron-hole pairs. By using an appropriate electrical circuit an electrical load is applied and electrical energy generated as a result of the creation of the electron-hole pairs.

Description:
CROSS REFERENCE TO RELATED APPLICATION 
     This application is a divisional application of application Ser. No. 10/720,035 filed on Nov. 21, 2003 and titled “Nuclear Voltaic Cell,” which is incorporated herein by reference in its entirety. 
    
    
     FIELD OF THE INVENTION 
     The invention relates primarily to a method of and a device for generating electrical power directly from nuclear power, and more particularly to using liquid semiconductors as a means for efficiently converting nuclear energy, either nuclear fission and/or radiation energy, directly into electrical energy. 
     BACKGROUND OF THE INVENTION 
     Ever since the potential for generating electrical power from nuclear reactions was recognized, scientists have strived to devise the best methods of harnessing nuclear power and putting it to practical use. The main objectives of such research have been to create the most efficient methods of power conversion, power converters that can generate electrical power from nuclear power sources for sustained periods of time without maintenance, and smaller, more manageable power converters that can be used as everyday power sources. The sources of nuclear energy that scientists have sought to harness include nuclear fission (the splitting of atoms), radiation (the emission by radiation of alpha, beta or gamma rays) and nuclear fusion (the fusing of atoms). The present invention is designed to generate electrical power from energy produced from nuclear fission and/or radiation. For the purposes of this document, the following terms shall have, in addition to their generally accepted meaning, the meanings listed below: 
     (a) the term “nuclear material” or “nuclear materials” refers to fissile materials and radioactive isotopes that are non-fissile, but produce radiation—either alpha, beta or gamma type radiation; 
     (b) the term “fissile material” includes uranium, plutonium, thorium, neptunium and mixtures of plutonium and uranium; 
     (c) Uranium refers to the following classifications—depleted uranium (U-235 concentration less than 0.7%), natural uranium (U-235 concentration equal to approximately 0.7%), low enriched uranium (U-235 or U-233 concentration less than 20%), high enriched uranium (U-235 or U-233 greater than 20%); 
     (d) Plutonium refers to reactor grade plutonium where the Pu-240 concentration is nominally 10% to 15%. 
     The best-known method of generating electrical power using nuclear energy is via heat exchange processes, the method used in nuclear power plants to generate electricity for use in the United States national grid. In the nuclear power plant, rods of uranium-235 are positioned in a reactor core where fission, the splitting of the uranium-235 atoms, occurs. When the uranium-235 atom splits apart, large amounts of energy are emitted. Inside the nuclear power plant, the rods of uranium are arranged in a periodic array and submerged in water inside a pressure vessel. The large amount of energy given off by the fission of the uranium-235 atoms heats the water and turns it to steam. The steam is used to drive a steam turbine, which spins a generator to produce electrical power. In some reactors, the superheated water from the reactor goes through a secondary, intermediate heat exchanger to convert water to steam in the secondary loop, which drives the turbine. Apart from the fact that the energy source is uranium-235, the nuclear power plant uses the same power conversion methods found in power plants that burn fossil fuels. 
     Nuclear power plants, in general, have energy conversion rates of between 30 and 40 percent. This efficiency rate is very good considering that several steps are used in such power plants to convert the nuclear energy to electrical energy. Consequently, nuclear power plants are a good source for large-scale generation of electricity. However, apparatus that use heat transfer techniques for generating electricity from nuclear energy are, in general, large and inefficient for small-scale power conversion. 
     Research has been performed into ways of reducing the size of the equipment necessary for an effective heat transfer system for generating electrical power from nuclear materials. Some success has been achieved, and since the 1950s small nuclear power plants have powered a great number of military submarines and surface ships. However, because of the associated risks, heat transfer systems have not been used for other small-scale energy sources and are no longer used on United States space vehicles. The use of nuclear energy to power nuclear submarines highlights the advantages that nuclear materials have as a power source; for example, a nuclear submarine can travel 400,000 miles before needing to be refueled. 
     Because of the potential of nuclear materials as a source for providing energy over a long period of time, a great deal of research has been performed to develop a small, self-contained power source utilizing nuclear materials that does not have the associated risks inherent in a heat transfer system. This research has led to the development of several methods of converting nuclear energy into electrical energy. 
     Theoretically, the best methods for converting nuclear energy into electrical energy should be direct methods where the nuclear energy is directly changed into electrical energy. The nuclear power plant discussed above involves an indirect, two-step process in which the nuclear energy is transferred into thermal energy that causes water to turn to steam that is used to drive turbines and create electrical energy. Direct conversion methods are potentially the most efficient conversion methods because they would avoid the inherent energy loss during each conversion process. The following are examples of direct conversion techniques that have been proposed up until the present date. 
     Conversion of nuclear energy to electrical energy using solid semiconductors. In this process, radiation energy from the radioactive isotope is directly converted to electrical energy by irradiating a semiconductor material with radioactive decay products to produce a number of electron-hole pairs in the material. To accomplish this, nuclear material, such as a radioactive isotope, is placed in close proximity to a solid semiconductor. As it decays, the radioactive isotope produces radiation. Because it is in close proximity with the solid semiconductor, some of this radiation enters the solid semiconductor and causes electron-hole pairs to be generated. Generally, the solid semiconductor is configured so as to incorporate a p-n junction that contains a built-in electric field within a region called the depletion region. This electrical field applies a force that drives electrons and holes generated in the depletion region in opposite directions. This causes electrons to drift toward the p type neutral region and holes toward the n type neutral region. As a result, when radiation enters the solid semiconductor, an electrical current is produced. Current can also be generated from electron-hole pairs produced within a few diffusion lengths of the depletion region by a mechanism involving both diffusion and drift. A Schottky barrier junction formed on either an n-type or p-type semiconductor can also be used in lieu of the p-n junction. In that case, an analogous process occurs when the metal on the n-type (p-type) semiconductor collects drifting holes, as did the p-type (n-type) neutral region in the p-n junction. 
     The potential conversion efficiency of the solid semiconductor system is high. However, the solid semiconductor method of converting nuclear power cannot be used to produce large power outputs for extended periods of time because the high energy radiation that enters the solid semiconductor also causes damage to the semiconductor lattice. Furthermore, if the energy source is fissile material, some of the fragments of fissile material that enter the solid semiconductor remain in the solid semiconductor. The introduction of trace amounts of defects, including native and impurity point defects and extended defects, can significantly reduce semiconductor device performance. Over time the solid semiconductor is degraded and efficiency decreases until it is no longer useful for power conversion. Consequently, even though systems using solid semiconductors as direct converters of nuclear energy to electrical energy are potentially very efficient, they are often impractical for high power, long duration applications. 
     Conversion of nuclear energy to electrical energy using Compton scattering. Compton scattering occurs when high-energy gamma radiation interacts with matter causing electrons to be ejected from the matter. A method for direct conversion of nuclear energy to electrical energy has been proposed in which a gamma radiation source is surrounded by an insulating material. As a result of Compton scattering, the gamma rays interact with the insulating material and cause electrons to be produced. These electrons can be collected to produce an electric current. Experiments to date have not been able to demonstrate that this method can generate sufficiently large amounts of electricity with the required efficiency and reliability at a sufficiently low cost to be useful for widespread use in practical applications. 
     Conversion of nuclear energy to electrical energy using an induction process. The use of induction to convert nuclear energy to electrical energy involves apparatus that provides electrical power by modulating the density of a cloud of charged particles confined within an enclosed space by a magnetic field. A radioactive material is positioned at the center of an enclosing hollow sphere having its inner surface coated with a metal, such as silver. The sphere is centrally positioned between the poles of a permanent magnet. As the radioactive material decays it emits radiation that in turn causes the cloud of charged particles to move. The movement of the charged particles results in a variation in the density of the cloud of charged particles and a variation in the magnetic field created by the cloud. This variation in the magnetic field induces an electric current in a conductive wire. Once again, the conversion efficiency of the system is very low and the amount of electrical power provided is too small for most applications. 
     Conversion of nuclear energy to electrical energy using thermoelectric systems. Thermoelectric conversion systems rely on direct conversion of thermal energy to electricity by means of the Seebeck effect. The Seebeck effect describes the phenomenon that when a thermal gradient occurs in a system containing two adjacent dissimilar materials, a voltage can be generated. Therefore, if radioactive material is placed in proximity to the system, the radiation produced by the radioactive material will heat the material causing a thermal gradient and as a result of the Seebeck effect, a voltage difference can be generated. A load can be inserted into the system, allowing electrical power to be removed from the system. Thermoelectric converters are used in radioisotope thermoelectric generators for deep space probes and can provide up to a kilowatt of power. However, theoretical conversion efficiencies for commonly used materials are only 15-20 percent and in practice, conversion efficiencies are much lower. 
     Conversion of nuclear energy to electrical energy using thermionic systems. Thermionic systems make use of the physical principle that certain materials when heated will emit electrons. Thermionic systems use nuclear matter, radioisotopes or fissile material, as an energy source to heat an emitter cathode that emits electrons which can be collected on an anode surface, delivering electrical power to an external load. Conversion efficiencies for thermionic systems increase with emitter temperature, with theoretical efficiencies ranging from 5% at 900 K to over 18% at 1,750 K. The drawbacks of the thermionic conversion system are poor efficiencies, high operating temperatures, and intense radiation environments. 
     Conversion of nuclear energy to electrical energy using fluorescent materials. In this system, a mixture of a radioactive substance and a fluorescent material is positioned between a pair of photovoltaic cells. The radioactive substance produces radioactive rays that excite the atoms of the fluorescent material and cause it to emit photons. The photovoltaic cells use this radiation to generate electricity. In general, this system requires a very complex structure but nevertheless provides poor conversion efficiency on the order of less than 0.01%. 
     SUMMARY OF THE INVENTION 
     As described above, ever since nuclear power was recognized as a viable energy source in the 1950s, considerable research has been performed to find better methods for converting nuclear power into electrical power. However, no direct conversion method has been created that is efficient and practical. In view of the foregoing, an objective of the present invention is to improve upon the prior art by providing a method and apparatus for the efficient, direct conversion of nuclear energy, either radioactive decay energy or fission energy, into electrical energy. More specifically, it is an object of the present invention to provide a self-contained method and apparatus for converting nuclear power to electrical power that can generate large amounts of electrical power for long periods of time without the need for frequent refueling and require little or no maintenance. Another object of the present invention is to provide a method and apparatus that meets the long felt need for a method of converting nuclear energy to electrical energy that is small in size, reliable and can generate large amounts of electrical energy for use in submarines, surface ships, and as a battery to power a whole range of products—including, for example, military equipment, satellites and space vehicles. 
     Each embodiment of the current invention relates to the use of a liquid semiconductor in conjunction with a radiation source: either fissile material such as uranium-235 or plutonium, or a radioactive isotope. Use of a liquid semiconductor minimizes the effects of radiation damage, because liquid semiconductors rapidly self-heal, and can be purified or “scrubbed” of fission fragments left from fission events. The current invention comprises different embodiments, several of which are described below. 
     Embodiments utilizing fissile materials:
         Embodiment 1: A nuclear voltaic cell with fissile material applied in a solid layer, and the layers of the nuclear voltaic cell axially opposed to each other and wound around a mandrel.   Embodiment 2: A nuclear voltaic cell with fissile material applied in a solid layer, and the layers of the nuclear voltaic cell axially opposed to each other and stacked on top of each other.   Embodiment 3: A nuclear voltaic cell with fissile material in solution in a liquid semiconductor, and the layers of the nuclear voltaic cell axially opposed and wound around a mandrel.   Embodiment 4: A nuclear voltaic cell with fissile material in solution in a liquid semiconductor, and the layers of the nuclear voltaic cell axially opposed to each other and stacked on top of each other.   Embodiment 5: An array of nuclear voltaic cells according to Embodiments 1, 2, 3, or 4.   Embodiment 6: A nuclear voltaic cell reactor core, with one closed loop in two sections for quiet continuous removal of waste heat. One liquid semiconductor is used for both energy conversion and cooling. The heat extractor on one section is also used for scrubbing the liquid semiconductor of unwanted fission fragments, while the opposing heat extractor may be used for replacing burned-up fissile material (if necessary).   Embodiment 7: A nuclear voltaic cell reactor core with separate loops, one for fission fragment scrubbing, one for cooling. Liquid semiconductor used for energy conversion, another substance (inert gas, water, etc.) used for cooling.       

     Embodiments utilizing radioactive isotopes:
         Embodiment 8: A nuclear voltaic cell with a radioactive isotope in solution with the liquid semiconductor, and the layers of the nuclear voltaic cell axially opposed to each other and wound around a mandrel.   Embodiment 9: A nuclear voltaic cell with a radioactive isotope in solution with the liquid semiconductor, and the layers of the nuclear voltaic cell axially opposed to each other and stacked on top of each other.   Embodiment 10: An array of nuclear voltaic cells according to Embodiments 8 or 9.       

     In accordance with one embodiment of the invention, there is provided a compact cell for supplying large amounts of electrical energy for a long duration. The cell includes nuclear material for providing nuclear energy, either radiation or fission energy. 
     In embodiment 1, a solid layer of the nuclear material is placed in close proximity to a liquid semiconductor. Nuclear energy in the form of fission fragments enters the liquid semiconductor and creates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode when placed in contact with the n-type or p-type liquid semiconductor. The structure contains both a Schottky contact and a low resistance or an Ohmic contact. As a consequence of this Schottky diode arrangement, a potential difference is produced across the liquid semiconductor that causes the electron-hole pairs, created by interactions with the nuclear radiation or energetic particles, to migrate to the metallic contacts. By placing an electrical load on the contacts of the present invention electrical power is generated. In a preferred embodiment, the nuclear voltaic cell comprising of nuclear material and a liquid semiconductor is constructed by wrapping the layers of materials around a mandrel in a spiral fashion. 
     In embodiment 2, a solid layer of the nuclear material is placed in close proximity to a liquid semiconductor. As in embodiment 1, nuclear energy in the form of fission fragments enters the liquid semiconductor and creates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode and a low resistance or Ohmic contact when placed in contact with the n-type or p-type liquid semiconductor. As a consequence of this Schottky diode arrangement, a built-in field is produced in the depletion region within the liquid semiconductor that causes electron-hole pairs to drift in different directions. By exposing the material to radiation and placing an electrical load on the contacts of the present invention, electrical power is generated. In a preferred embodiment of embodiment 2, a nuclear voltaic cell is constructed by stacking the layers of materials. 
     In a preferred embodiment of the current invention, described as embodiment 3 above, nuclear material providing fission energy is dissolved in the liquid semiconductor. Again, nuclear energy in the form of fission fragments is released within the liquid semiconductor that generates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode and a low resistance or Ohmic contact when placed in contact with the n-type or p-type liquid semiconductor. A built-in field is produced within the depletion region of the liquid semiconductor that causes electrons and holes generated either in the depletion width or within a few diffusion lengths of it to move in opposite directions. This results in the generation of a current. By placing an electrical load on the contacts of the present invention, electrical power is generated. In a preferred embodiment, a nuclear voltaic cell is constructed by wrapping the layers of materials around a mandrel in a spiral fashion. 
     In Embodiment 4, nuclear material providing fission energy is dissolved in the liquid semiconductor. Nuclear energy in the form of energetic fission fragments interacts with the liquid semiconductor and creates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode and a low resistance or Ohmic contact when placed in contact with the n-type or p-type liquid semiconductor. A built-in field is produced within the depletion region of the liquid semiconductor that causes electrons and holes generated either in the depletion width or within a few diffusion lengths of it to move in opposite directions. This results in the generation of a current. By placing an electrical load on the contacts of the present invention electrical power is generated. In a preferred embodiment, a nuclear voltaic cell is constructed by stacking the layers of materials. 
     Unlike previous methods for converting nuclear energy to electrical energy using solid semiconductors, the present invention can use fission or high-energy radiation to generate large amounts of electrical power without rapid deterioration of the collection efficiency. This is because, unlike the lattice of a solid semiconductor, the short-range order of a liquid semiconductor is not permanently degraded by the interaction with fission fragments or high-energy radiation. Therefore, in a preferred embodiment of the present invention, the liquid semiconductor is made to flow through the active region of the nuclear voltaic cell (something that is not possible with solid semiconductors), and is purified or scrubbed of unwanted fission fragments and neutron activation products so that its purity and semiconductive properties are not degraded over time, making the conversion device capable of continuous optimum energy conversion. In addition, burned-up fissile material may be replaced while the reactor is operating, avoiding down time for refueling. Because of these advantages, the present invention provides for efficient conversion and the generation of large amounts of electrical power, features that are not possible with solid semiconductor devices. 
     The present invention is very adaptable because multiple nuclear voltaic cells—comprising any of the embodiments described above, i.e., embodiments 1, 2, 3, or 4—may be linked together to form a critical array, described as embodiment 5 above, to provide power up to and exceeding the megawatt range. For small power needs a single or small number of cells may be used. In a preferred embodiment of the present invention, described as embodiment 6 above, the array thus formed constitutes a nuclear voltaic reactor core surrounded by appropriate shielding and cooling materials. In a preferred embodiment, the nuclear voltaic reactor core uses the same liquid semiconductor employed in energy conversion for cooling. In a preferred embodiment, the coolant loop is divided into two sections, each with a heat extractor. The loop sections are separated by oscillating valves and an oscillating pneumatic piston and chilled coolant from one heat extractor is quietly forced by high inert gas pressure through the core, while coolant warmed by waste heat in the core flows into the other heat extractor at low inert gas pressure. When the first heat extractor is empty and the second extractor is filled, the oscillating valves change positions and the piston reverses direction to provide continuous quiet cooling of the core. One heat extractor also is used to scrub unwanted fission fragments and neutron activation products while the other may be used to replace burned-up fissile material. 
     In a preferred embodiment of the current invention, the nuclear voltaic reactor core, described in Embodiment 7 above, has two separate loops, one for energy conversion and fission fragment/activation product scrubbing and the other for cooling, but the coolant can be something other than a liquid semiconductor. In this way, the present invention is adaptable and can meet many different needs, including generating power for the electricity grid and providing electrical energy for a wide range of such diverse applications including space vehicles, submarines and military equipment. 
     In another preferred embodiment, the present invention may also be used to construct a nuclear voltaic battery. In Embodiment 8, described above, the nuclear material in the form of a radioactive isotope is dissolved in a liquid semiconductor. Dissolving the radioactive isotope in the liquid semiconductor is a preferred embodiment of the invention, however, in another embodiment the radioactive isotope may instead be positioned in close proximity to the liquid semiconductor. Nuclear energy in the form of alpha, beta, and/or gamma radiation enters the liquid semiconductor and creates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode and a low resistance or Ohmic contact when placed in contact with the n-type or p-type liquid semiconductor. A built-in field is produced within the depletion region of the liquid semiconductor that causes electrons and holes generated either in the depletion width or within a few diffusion lengths of it to move in opposite directions. This results in the generation of a current. By placing a load on the contacts of the present invention electrical power is generated. In a preferred embodiment, the nuclear voltaic cell is constructed by wrapping the layers of materials around a mandrel in a spiral fashion. 
     In Embodiment 9, described above, the nuclear material in the form of a radioactive isotope is dissolved in a liquid semiconductor. As in Embodiment 8, nuclear energy in the form of alpha, beta, and/or gamma radiation enters the liquid semiconductor and creates electron-hole pairs. The liquid semiconductor is an n-type or p-type semiconductor that is sandwiched between two metal contacts that are selected so as to create a Schottky diode and a low resistance or Ohmic contact when placed in contact with the n-type or p-type liquid semiconductor. A built-in field is produced within the depletion region of the liquid semiconductor that causes electrons and holes generated either in the depletion width or within a few diffusion lengths of it to move in opposite directions. This results in the generation of a current. By placing an electrical load on the contacts of the present invention electrical power is generated. In a preferred embodiment, a nuclear voltaic cell is constructed by stacking the layers of material. 
     In a preferred embodiment of the of the present invention, the liquid semiconductor is made to flow through the active region of the nuclear voltaic cell (something that is not possible with solid semiconductors), and is purified or scrubbed of unwanted decay products so that its semiconductive properties are not impaired over time, making the conversion device capable of continuous optimum energy conversion. Because of these advantages, the present invention provides for efficient conversion and the generation of large amounts of electrical power for long periods of time, things that were not possible with solid semiconductors. 
     The present invention is very adaptable because multiple nuclear voltaic cells may be linked together in an array to form a nuclear voltaic battery, described in Embodiment 10 above, to provide power ranges from fractions of a watt to greater than Megawatts. For small power needs a single or small number of cells may be used. 
    
    
     
       BRIEF DESCRIPTION OF THE FIGURES 
         FIG. 1  shows a schematic cross section through one embodiment of the nuclear voltaic cell, wherein the nuclear material is coated on a substrate. 
         FIG. 2  shows a potential energy diagram for the junction between the Schottky contact and an n-type liquid semiconductor. 
         FIG. 3  shows a fission event occurring in the nuclear voltaic cell. 
         FIG. 4  shows a schematic cross section of a preferred embodiment of the present invention wherein the nuclear material is in solution in the liquid semiconductor. 
         FIG. 5  shows a fission event occurring from fissile material dissolved in the liquid semiconductor in the nuclear voltaic cell in one embodiment of the present invention. 
         FIG. 6  shows the emission of alpha, beta, or gamma rays from a radioactive isotope dissolved in the liquid semiconductor in the nuclear voltaic cell in one embodiment of the present invention. 
         FIG. 7  shows preferred embodiments of the present invention wherein the axially opposed layers of the present invention are wound around a mandrel. 
         FIG. 8  shows how in a preferred embodiment of the present invention multiple nuclear voltaic cells are connected to create an array. 
         FIG. 9  shows how in a preferred embodiment of the present invention multiple nuclear voltaic cells are combined to create a nuclear voltaic reactor. 
         FIG. 10  shows a preferred embodiment of the present invention wherein the coolant and the liquid semiconductor are circulated through the nuclear voltaic cell reactor. 
         FIG. 11  shows how, in a preferred embodiment of the present invention, the coolant loop and energy conversion/fission fragment scrubber loop are separated from each other. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       FIG. 1  shows a cross section through one embodiment of the Nuclear Voltaic Cell  5 . In this embodiment, the Liquid Semiconductor  20  is sandwiched between two metal contacts; the Ohmic Contact  10  and the Schottky Contact  30 . The device will also function if a low resistance contact is used in lieu of the Ohmic Contact  10 . This may be necessary in the case that an ideal Ohmic Contact  10  is not readily available as a result of fundamental or practical reasons. 
     As shown in  FIG. 1 , the Liquid Semiconductor  20  is sandwiched between the two metal contacts, the Ohmic Contact  10  and the Schottky Contact  30 . Furthermore, as shown in  FIG. 1 , the two metal contacts, the Ohmic Contact  10  and the Schottky Contact  30 , form a channel through which the Liquid Semiconductor  20  may flow. In a preferred embodiment of the present invention, the Liquid Semiconductor  20  flows in the direction of the Arrow  15  into the channel between the Ohmic Contact  10  and the Schottky Contact  30  and then flows out of the channel between the Ohmic Contact  10  and the Schottky Contact  30  in the direction of the Arrow  25 . In a preferred embodiment of the present invention, the two ends of the channel between the Ohmic Contact  10  and the Schottky Contact  30  are connected by a closed loop and a pump is used to circulate the Liquid Semiconductor  20  through the channel between the Ohmic Contact  10  and the Schottky Contact  30  and around the closed loop. 
     As persons familiar with the art will understand, the Ohmic Contact  10  is preferably made from a metal such that no, or a minimal barrier, exists between the Ohmic Contact  10  and the Liquid Semiconductor  20 . Furthermore, as persons familiar with the art will understand, the Schottky Contact  30  is preferably made from a metal such that when placed in contact with the Liquid Semiconductor  20  a substantial electrostatic barrier is created across the Liquid Semiconductor  20 . In the embodiment of the present invention described in  FIG. 1 , a Substrate  40  is plated with Nuclear Material  50  and the metal Schottky Contact  30  is coated on top of the Nuclear Material  50 . In a preferred embodiment of the invention, the Ohmic Contact  10  and the Schottky Contact  30  are connected in a circuit so that a Load  35  may be applied to the circuit and electrical energy removed from the present invention. 
     As shown in  FIG. 1 , in a preferred embodiment of the present invention, the cross section of the strata making up the active parts of the invention is of the order of 1.63×10 −2  cm across. In a preferred embodiment, non-active spacers are placed between the Ohmic Contact  10  and the Schottky Contact  30  to maintain the separation of the two contacts. In an alternative embodiment, the Nuclear Material  50  may be replaced with a non-fissile radioactive isotope that produces either of or a combination of alpha, beta or gamma radiation as it decays. 
     In a preferred embodiment of the invention, the Liquid Semiconductor  20  is a solid at room temperature and is deposited between the Ohmic Contact  10  and the Schottky Contact  30 . In a preferred embodiment of the present invention, the layers of the Nuclear Voltaic Cell  5  are fabricated using thin film technology. In a preferred embodiment of the invention, once the layers of the Nuclear Voltaic Cell  5  have been fabricated, the Nuclear Voltaic Cell  5  is heated so as to melt the Liquid Semiconductor  20 . Optimum operating temperatures will vary depending upon the properties of the Liquid Semiconductor  20  used. In a preferred embodiment, the Liquid Semiconductor is selenium and the operating temperature is 230-250° Celsius. It will be understood by those experienced in the art that liquid semiconductors other than selenium may be employed. Over particular ranges of temperature and composition, liquid semiconductors may be formulated from pure chalcogens (oxygen, sulfur, selenium and tellurium). Among other possibilities, suitable liquid semiconductors include mixtures of chalcogens, and alloys of chalcogens with metals. In a preferred embodiment of the present invention, after initial heating by an external source, the heat generated from the nuclear material maintains the temperature of the Nuclear Voltaic Cell  5 . 
     In a preferred embodiment of the present invention, an external electrical power source is used to heat the Nuclear Voltaic Cell  5  and liquefy the semiconductor. In an alternative embodiment, the Liquid Semiconductor  20  is liquid at room temperature and the present invention does not have to be heated prior to operation. 
       FIG. 2  shows an energy band diagram for the Junction  60  between the Schottky Contact  30  and the Liquid Semiconductor  20 . The metal of the Schottky Contact  30  is chosen so that at equilibrium a potential difference is created across the Liquid Semiconductor  20 . In a preferred embodiment of the present invention, the Liquid Semiconductor  20  is an n-type semiconductor. The point of contact between the Schottky Contact  30  and the Liquid Semiconductor  20  is often referred to in the art as a junction. 
     At thermal equilibrium, with no external voltage applied, there is a region in the Liquid Semiconductor  20  close to the Junction  60 , which is depleted of mobile carriers. This is known in the art as the Depletion Region  70 . The height of the barrier in the Liquid Semiconductor  20  from the Fermi level to the top of the electrostatic barrier is equal to the Built-In Potential φ b    80 . Electrons  90  or Holes  100  that enter the Depletion Region  70  will experience a force between the neutral part of the Liquid Semiconductor  20  and the metal of the Schottky Contact  30  because of the electric field resulting from the Potential Barrier  80  in the Liquid Semiconductor  20 . The Diffusion Length  110  depends upon the properties of the Liquid Semiconductor  20  used and is a measure of how far excess Electrons  90  or Holes  100  on average can diffuse in the Liquid Semiconductor  20  before recombining. The Collection Volume  115  is a combination of the Depletion Region  70  and a multiple of the Diffusion Length  110  and represents the volume in which Electrons  90  and Holes  100  are collected. These carriers, Electrons  90  and Holes  100 , initiate the generation process that results in current flowing through the Liquid Semiconductor  20 . 
     As persons familiar with the art will understand, while the potential energy diagrams will be different if a p-type liquid semiconductor is used, the same overall result, the flow of Electrons  90  and Holes  100  and creation of an electrical current may be produced by either the use of an n-type or a p-type liquid semiconductor. 
     In a preferred embodiment of the invention, the Liquid Semiconductor  20  is liquid selenium at a temperature above 233° Celsius. Liquid selenium is a preferred Liquid Semiconductor  20  because it has a very large band-gap, which produces a large Potential Barrier  80  across the Depletion Region  70 , and a large Diffusion Length  110 . However, other liquid semiconductors may be used which improve on the characteristics of selenium. 
       FIG. 3  shows a cross section of the present invention when a Fission Event  120  occurs. In a preferred embodiment of the invention, the Nuclear Material  50  is Uranium-235. A Fission Event  120  occurs when the atom of the Nuclear Material  50  splits. As persons familiar with the art will understand, a Fission Event  120  may occur naturally or, more likely, as a result of an impact with a neutron ejected during another fission event. As a result of the Fission Event  120 , two fragments of the Nuclear Material  50  are created. In the embodiment of the present invention shown in  FIG. 3 , one fragment of the Nuclear Material  50 , the Lost Fission Fragment  130 , does not enter the Liquid Semiconductor  20 . The other Fission Fragment  140 , however, enters the Liquid Semiconductor  20 . As persons familiar with the art will understand, the Fission Fragment  140  is highly energetic. For example in the case of Uranium-235, the average energy of Fission Fragment  140  is between 67 and 95 MeV. When the Fission Fragment  140  enters the Liquid Semiconductor  20  it interacts with the atoms and electrons of the Liquid Semiconductor  20  and creates Electron-Hole Pairs  150  along a track in the Liquid Semiconductor  20 . This process creates large quantities of Electrons  90  and Holes  100  in the Liquid Semiconductor  20 . The Fission Fragment  140  may also interact with the atoms and electrons of the Liquid Semiconductor  20 . Such interaction can cause the creation of a High Energy Electron  160  and Knock-On Host Atom  170 . The High Energy Electron  160  and the Knock-On Atom  170  may also result in the creation of more Electrons  90  and Holes  100 . Because of the Potential Barrier  80  between the low resistance or Ohmic Contact  10  and the Schottky Contact  30 , the Electrons  90  and the Holes  100  move in opposite directions and result in the flow of electric current between the Ohmic Contact  10  and the Schottky Contact  30 . As shown in  FIG. 2 , the Potential Barrier  80  exists across the Depletion Region  70 . As a result, only Electrons  90  or Holes  100  that are in the Depletion Region  70  or diffuse into the Depletion Region  70  will become part of the flow of Electrons  90  and Holes  100  between the Ohmic Contact  10  and the Schottky Contact  30 . As discussed above, liquid selenium is a preferred liquid semiconductor because it has a large Diffusion Length  110  associated with it and consequently provides for the capture of more Electrons  90  and Holes  100 . 
     The Nuclear Material  50  not only produces Fission Fragments  140  when its atom is split, but also produces secondary radiation that will ionize the atoms of the Liquid Semiconductor  20  producing Electrons  90  and Holes  100  that will result in electrical energy generation. In an alternative embodiment of the present invention, the Nuclear Material  50  may be a non-fissile radioactive isotope that produces either of or a combination of alpha, beta or gamma radiation as it decays. In such an embodiment of the present invention, the alpha, beta or gamma rays when they enter the Liquid Semiconductor  20  will produce Electrons  90  and Holes  100 . As such, the operation of the present invention is the same as when Nuclear Material  50  is used except, however, the alpha, beta or gamma rays do not produce as many Electrons  90  and Holes  100  per incident radiation and, as a consequence, an embodiment of the present invention using a non-fissile radioactive isotope may not be able to generate as much electrical power as an embodiment using Nuclear Material  50 . 
     In one embodiment of the present invention, non-fissile radioactive isotopes may be used to provide lower power outputs with less associated radiation. This type of power source is more practical for use in devices that are in close proximity to a human operator because a lightweight radioactive shield can be placed around the device. Such a power source is well suited for use in space vehicles and military equipment where high power outputs are not required and a smaller device that is not highly radioactive is necessary. 
       FIG. 4  shows a cross section of a preferred embodiment of the present invention wherein the Nuclear Material  50  is in solution in the Liquid Semiconductor  20 . In this preferred embodiment, the Liquid Semiconductor  20  is sandwiched between the low resistance or Ohmic Contact  10  and the Schottky Contact  30  and the Nuclear Material  50  is in solution in the Liquid Semiconductor  20 . This is a preferred embodiment of the invention because when a Fission Event  120  occurs there are no lost fission fragments and both fission fragments will travel through the Liquid Semiconductor  20  and either fission fragment may cause generation of electron-hole pairs within the Liquid Semiconductor  20 . As a consequence, this preferred embodiment is more efficient than the embodiment described in  FIG. 2 . 
       FIG. 5  shows a Fission Event  120  occurring within the Liquid Semiconductor  20 , and illustrates that in the embodiment wherein the Nuclear Material  50  is in solution in the Liquid Semiconductor  20 , both Fission Fragments  140  are available to generate electron-hole pairs in the Liquid Semiconductor  20 . 
       FIG. 6  shows an alternative embodiment of the present invention where the Nuclear Material  50  is a non-fissile radioactive isotope. In a preferred embodiment, the non-fissile material would be in solution in the Liquid Semiconductor  20  so that Radiation Emission  190  in any direction may cause the creation of electron-hole pairs in the Liquid Semiconductor  20 . 
       FIG. 7  shows a preferred embodiment of the present invention in which the axially opposed layers of the present invention, as described in  FIG. 1 , are wound around a Mandrel  200  to create a single Nuclear Voltaic Cell  5  with characteristics similar to a chemical cell. The advantage of this preferred embodiment of the present invention is that it minimizes the volume of the present invention and provides for stability since long, thin Nuclear Voltaic Cells  5  that are wound around a Mandrel  200  are mechanically sturdy. In an alternative embodiment, the axially opposed layers of the Nuclear Voltaic Cell  5  may be stacked on top of each other; however, this does not reduce the volume of the present invention as much as the winding method described above, since a means must be provided for maintaining the mechanical integrity of the stack. 
       FIG. 8  shows how, in a preferred embodiment of the present invention, multiple Nuclear Voltaic Cells  5  may be connected using Perforated Sheet Conductors  210  to create an Array  220 . In this preferred embodiment, by connecting the Nuclear Voltaic Cells  5  into an Array  220 , the power produced by each Nuclear Voltaic Cell  5  may be combined for greater electrical power generation. The number of Nuclear Voltaic Cells  5  used in the Array  220  may be varied depending upon the amount of electrical energy required. Because the Nuclear Voltaic Cells  5  are connected in a series/parallel fashion, if one Nuclear Voltaic Cell  5  fails, the rest of the Array  220  will continue to function. 
       FIG. 9  shows a preferred embodiment of the present invention whereby multiple Nuclear Voltaic Cells  5  are combined to create a Nuclear Voltaic Reactor  230 . In this embodiment, individual Nuclear Voltaic Cells  5  are connected using a Perforated Sheet Conductor  210 . In a preferred embodiment of the present invention, a Biological Shield  240  and an Outer Housing  250  are provided that surround the assembly of Nuclear Voltaic Cells  5  to prevent the escape of any radiation. A Coolant  180  is pumped around the inside of the Nuclear Voltaic Reactor  230 , between the Biological Shield  240  and the Outer Housing  250 , to prevent overheating. In a preferred embodiment of the present invention, the Coolant  180  is a Liquid Semiconductor  20 . In this way, the Liquid Semiconductor  20  may be used both to cool the Nuclear Voltaic Reactor  230  and to produce electric power. 
       FIG. 10  shows a preferred embodiment of the present invention wherein the Liquid Semiconductor  20  is circulated from the Cold Legs  280  through the Nuclear Voltaic Reactor Core  230  to the Hot Legs  290 , serving as coolant for removing waste heat (fission fragment energy not converted into electricity) as well as performing energy conversion. In this preferred embodiment, chilled Liquid Semiconductor  20  is made to flow by the Reciprocating Pneumatic Piston  300 . The Reciprocating Pneumatic Piston  300  compresses an Inert Gas  320  causing the Liquid Semiconductor  20  to flow from the First Heat Extractor  310  through the Nuclear Voltaic Reactor Core  230 , where it provides for attaining nuclear criticality, energy conversion, and cooling. The Liquid Semiconductor  20  then flows into the Second Heat Extractor  330  at low inert gas pressure, flow direction being governed by Oscillating Valves  340  and the direction of the Reciprocating Pneumatic Piston  300  movement. When the Second Heat Extractor  330  is filled, the Oscillating Valves  340  change position and the Reciprocating Pneumatic Piston  300  reverses direction to force chilled coolant from the Second Heat Extractor  330  through the Nuclear Voltaic Core  230  to the First Heat Extractor  310  for continuous quiet cooling. The heat removed can also be used to produce auxiliary electrical power via the conventional heat exchange process (e.g., thermoelectric converters). Similarly, by combining a scrubbing mechanism with the Second Heat Extractor  330 , the Liquid Semiconductor  20  can flow intermittently into the Second Heat Extractor  330  where unwanted pieces of fission fragment material and unwanted neutron activation products can be removed from the Liquid Semiconductor  20 . This is a preferred embodiment of the current invention as it allows for the present invention to be a self-contained system in which there is continuous cooling and purification or scrubbing wherein the Liquid Semiconductor  20  is continuously used without the need for adding new Liquid Semiconductor  20  when the Liquid Semiconductor  20  becomes too contaminated with Fission Fragments  140  and neutron activation products. 
     In combination with the scrubbing of fission fragments and of neutron activation products, fissile material may be added intermittently in the First Heat Extractor  310  to replace the fissile material burned up in the fission process to sustain a critical nuclear condition in the reactor. 
       FIG. 11  shows an embodiment of the present invention wherein the Coolant  180 , which may or may not be a Liquid Semiconductor  20 , accomplishes the coolant phase. The Coolant  180  and the Liquid Semiconductor  20  are in separate loops circulated through the Nuclear Voltaic Reactor Core  230 . In this preferred embodiment, a first Pump  370  is used to pump the Coolant  180  to flow in the direction of the Arrow  350 , and the Liquid Semiconductor  20  is pumped by a second Pump  370  to flow in the direction of the Arrow  360 . The Coolant  180  flows into a Heat Extractor  380  that allows for the removal of heat energy so that the Coolant  180  can be used as a means for continuous cooling. The heat removed can also be used to produce auxiliary electrical power via the conventional heat exchange process (e.g., thermoelectric converters). The Liquid Semiconductor  20  is pumped to flow through the Scrubber  390  where unwanted pieces of fission fragment material and unwanted neutron activation products can be removed from the Liquid Semiconductor  20 . 
     Having described the present invention, it will be understood by those skilled in the art that many changes in construction and circuitry and widely different embodiments and applications of the invention will suggest themselves without departing from the scope of the present invention.