Patent Application
20070042667
The present invention relates generally to devices and methods for generating electrons from diamond-like carbon material, and to devices and methods that utilize electrons generated by diamond-like carbon material. Accordingly, the present application involves the fields of physics, chemistry, electricity, and material science.
Thermionic and field emission devices are well known and used in a variety of applications. Field emission devices such as cathode ray tubes and field emission displays are common examples of such devices. Generally, thermionic electron emission devices operate by ejecting hot electrons over a potential barrier, while field emission devices operate by causing electrons to tunnel through a barrier. Examples of specific devices include those disclosed in U.S. Pat. Nos. 6,229,083; 6,204,595; 6,103,298; 6,064,137; 6,055,815; 6,039,471; 5,994,638; 5,984,752; 5,9,81,071; 5,874,039; 5,777,427; 5,722,242; 5,713,775; 5,712,488; 5,675,972; and 5,562,781, each of which is incorporated herein by reference.
The electron emission properties of thermionic devices are more highly temperature dependent than in field emission devices. An increase in temperature can dramatically affect the number of electrons which are emitted from thermionic device surfaces.
Although basically successful in many applications, thermionic devices have been less successful than field emission devices, as field emission devices generally achieve a higher current output. Despite this key advantage, most field emission devices suffer from a variety of other shortcomings that limit their potential uses, including materials limitations, versatility limitations, cost effectiveness, lifespan limitations, and efficiency limitations, among others.
A variety of different materials have been used in field emitters in an effort to remedy the above-recited shortcomings, and to achieve higher current outputs using lower energy inputs. One material that has recently become of significant interest for its physical properties is diamond. Specifically, pure diamond has a low positive electron affinity which is close to vacuum. Similarly, diamond doped with a low ionization potential element, such as cesium, has a negative electron affinity (NEA) that allows electrons held in its orbitals to be shaken therefrom with minimal energy input. However, diamond also has a high band gap that makes it an insulator and prevents electrons from moving through, or out of it. A number of attempts have been made to modify or lower the band gap, such as doping the diamond with a variety of dopants, and forming it into certain geometric configurations. While such attempts have achieved moderate success, a number of limitations on performance, efficiency, and cost, still exist. Therefore, the possible applications for field emitters remain limited to small scale, low current output applications.
As such, materials capable of achieving high current outputs by absorbing relatively low amounts of energy from an energy source, and which are suitable for use in practical applications continue to be sought through ongoing research and development efforts.
Accordingly, the present invention provides materials, devices, and methods for conversion of energy using an energy device. In one aspect, a diamond-like carbon energy conversion device is provided. Such a device may include a cathode having a base member with a layer of diamond-like carbon material coated over at least a portion thereof, an intermediate member electrically coupled to the diamond-like carbon material, the intermediate member including a plurality of carbon structures coated with a layer of an insulating material and an anode electrically coupled to the intermediate member opposite the diamond-like carbon material.
Though numerous insulating materials are contemplated, in one aspect the insulating material may be a polymer. Non-limiting examples of polymers that may be utilized in various aspects of the present invention may include natural rubbers, polyisoprenes, urethane rubbers, polyester rubbers, chloroprene rubbers, epichlorhydrin rubbers, silicone rubbers, styrene-butadiene-styrene block co-polymers, styrene-isoprene-styrene block co-polymers, styrene-ethylene butylene-styrene co-polymers, butyl rubbers, phosphazine rubbers, polyethylenes, polypropylenes, polyethyleneoxides, polypropyleneoxides, polystylenes, vinylchlorides, ethylene-ethylacetate copolymers, 1,2-polybutadiene, 1,4-polybutadiene, epoxy resins, phenol resins, cyclic polybutadienes, cyclic polyisoprenes, polytetrafluoroethylenes, polymethylmethacrylates, and combinations thereof. In one specific aspect, the insulating material may be polytetrafluoroethylene (PTFE). In another specific aspect the insulating material may be an epoxy resin.
In addition to polymeric materials, the insulating material may be an inorganic insulating material. Non-limiting examples may include sulfur, talc, pyrophylite, and combinations thereof.
The carbon structures of the intermediate member can be any form of carbon structure known that provides energy conversion properties as described herein. In one aspect, for example, the plurality of carbon structures may include various single-walled and multi-walled carbon structures. Non-limiting examples may include carbon nanotubes, bucky balls, carbon onions, and combinations thereof. In another aspect, the plurality of carbon structures may include nanodiamond particles. Various sizes of nanodiamond particles are contemplated that may vary depending on the configuration of a particular embodiment of the present invention. For example, in one aspect the nanodiamond particles may range from about 1 nm to about 100 nm in size. In another aspect, the nanodiamond particles may range from about 10 nm to about 50 nm in size.
The intermediate member thickness may vary depending on numerous factors such as the intended configuration of a particular device, the operating parameters of a particular device, the method of coating the plurality of carbon structures, the nature of the carbon structures, etc. In one aspect, however, the intermediate member may be less than about 20 microns thick. In another aspect, the intermediate member may be less than about 10 microns thick. In yet another aspect, the intermediate member may be less than about 5 microns thick.
The intermediate members according to the various aspects of the present invention have low thermal conductivity and low electrical resistivity properties. For example, in one aspect the intermediate member has a thermal conductivity of from about 0.1 W/mK to about 10.0 W/mK. In another aspect, the intermediate member has a thermal conductivity of from about 1.0 W/mK to about 5.0 W/mK. Additionally, in one aspect the intermediate member has an electrical resistivity less than about 1×106 Ω-cm at 20° C. In another aspect, the intermediate member has a thermal resistivity less than about 1 Ω-cm at 20° C.
Various cathode configurations are also contemplated. In one aspect, the base member may comprise at least two layers. These multiple layers may be configured to have different work functions. For example, in one aspect, the base member may include a first conductive cathode layer and a second layer, the second layer having a work function less than a work function of the first conductive cathode layer. Exemplary materials for use in constructing the second layer may include, without limitation, Cs, Sm, Al—Mg, Li, Na, K, Rb, Be, Mg, Ca, Sr, Ba, B, Ce, Al, La, Eu, and mixtures or alloys thereof.
In yet another detailed aspect, the cathode and the anode can be flexible such that the energy conversion device can be placed on contoured surfaces or used in applications where flexibility is required.
The energy conversion devices of the present invention may be configured as either, or both, an electrical generator and cooling device. In one aspect, an energy collector can be coupled to the cathode opposite the diamond-like carbon material such that the diamond-like carbon energy conversion device is configured as an electrical generator. This embodiment can operate under conversion of thermal and/or photonic energy into electrical energy. Alternatively, or in addition to an electrical generator, a voltage source can be operatively connected between the anode and the cathode such that the diamond-like carbon energy conversion device is configured as a cooling device. In this way, the device can selectively control heat flow across the device to cool an adjacent structure or space.
The energy conversion devices of the present invention can be conveniently formed using various techniques such as vapor deposition. In addition, the devices of the present invention do not require formation of a vacuum space and are typically completely solid throughout. As a result, the devices of the present invention are capable of mass production at reduced costs and are highly robust and reliable for an extended period of time.
In another aspect, a method of making a diamond-like carbon energy conversion device as described above is provided. Such a method may include forming the layer of diamond-like carbon material on the cathode using a vapor deposition technique, the diamond-like carbon material having an electron emission surface opposite the cathode, and forming the plurality of insulating material-coated carbon structures into the intermediate member on the electron emission surface. The anode may be further coupled to the intermediate member opposite the cathode.
In yet another aspect, a method of generating an electrical current is provided. Such a method may include inputting an amount of photonic or thermal energy into the layer of diamond-like carbon material as described above sufficient to produce a current.
There has thus been outlined, rather broadly, the more important features of the invention so that the detailed description thereof that follows may be better understood, and so that the present contribution to the art may be better appreciated. Other features of the present invention will become clearer from the following detailed description of the invention, taken with the accompanying drawings and claims, or may be learned by the practice of the invention.
The drawings will be described further in connection with the following detailed description. Further, these drawings are not necessarily to scale and are by way of illustration only such that dimensions and geometries can vary from those illustrated.
Before the present invention is disclosed and described, it is to be understood that this invention is not limited to the particular structures, process steps, or materials disclosed herein, but is extended to equivalents thereof as would be recognized by those ordinarily skilled in the relevant arts. It should also be understood that terminology employed herein is used for the purpose of describing particular embodiments only and is not intended to be limiting.
It must 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. Thus, for example, reference to “a layer” includes one or more of such layers, reference to “a carbon source” includes reference to one or more of such carbon sources, and reference to “a cathodic arc technique” includes reference to one or more of such techniques.
Definitions
In describing and claiming the present invention, the following terminology will be used in accordance with the definitions set forth below.
As used herein, “vacuum” refers to a pressure condition of less than 10−2 torr.
As used herein, “diamond” refers to a crystalline structure of carbon atoms bonded to other carbon atoms in a lattice of tetrahedral coordination known as sp3 bonding. Specifically, each carbon atom is surrounded by and bonded to four other carbon atoms, each located on the tip of a regular tetrahedron. Further, the bond length between any two carbon atoms is 1.54 angstroms at ambient temperature conditions, and the angle between any two bonds is 109 degrees, 28 minutes, and 16 seconds although experimental results may vary slightly. A representation of carbon atoms bonded in a normal or regular tetrahedron configuration in order to form diamond is shown in
As used herein, “distorted tetrahedral coordination” refers to a tetrahedral bonding configuration of carbon atoms that is irregular, or has deviated from the normal tetrahedron configuration of diamond as described above. Such distortion generally results in lengthening of some bonds and shortening of others, as well as the variation of the bond angles between the bonds. Additionally, the distortion of the tetrahedron alters the characteristics and properties of the carbon to effectively lie between the characteristics of carbon bonded in sp3 configuration (i.e. diamond) and carbon bonded in sp2 configuration (i.e. graphite). One example of material having carbon atoms bonded in distorted tetrahedral bonding is amorphous diamond. A representation of carbon atoms bonded in distorted tetrahedral coordination is shown in
As used herein, “diamond-like carbon” refers to a carbonaceous material having carbon atoms as the majority element, with a substantial amount of such carbon atoms bonded in distorted tetrahedral coordination. Diamond-like carbon (DLC) can typically be formed by PVD processes, although CVD or other processes could be used such as vapor deposition processes. Notably, a variety of other elements can be included in the DLC material as either impurities, or as dopants, including without limitation, hydrogen, sulfur, phosphorous, boron, nitrogen, silicon, tungsten, etc.
As used herein, “amorphous diamond” refers to a type of diamond-like carbon having carbon atoms as the majority element, with a substantial amount of such carbon atoms bonded in distorted tetrahedral coordination. In one aspect, the amount of carbon in the amorphous diamond can be at least about 90%, with at least about 20% of such carbon being bonded in distorted tetrahedral coordination. Amorphous diamond also has a higher atomic density than that of diamond (176 atoms/cm3). Further, amorphous diamond and diamond materials contract upon melting.
As used herein, “vapor deposition” refers to a process of depositing materials on a substrate through the vapor phase. Vapor deposition processes can include any process such as, but not limited to, chemical vapor deposition (CVD) and physical vapor deposition (PVD). A wide variety of variations of each vapor deposition method can be performed by those skilled in the art. Examples of vapor deposition methods include hot filament CVD, rf-CVD, laser CVD (LCVD), metal-organic CVD (MOCVD), sputtering, thermal evaporation PVD, ionized metal PVD (IMPVD), electron beam PVD (EBPVD), reactive PVD, atomic layer deposition (ALD) and the like.
As used herein, “asperity” refers to the roughness of a surface as assessed by various characteristics of the surface anatomy. Various measurements may be used as an indicator of surface asperity, such as the height of peaks or projections thereon, and the depth of valleys or concavities depressing therein. Further, measures of asperity include the number of peaks or valleys within a given area of the surface (i.e. peak or valley density), and the distance between such peaks or valleys.
As used herein, “metallic” refers to a metal, or an alloy of two or more metals. A wide variety of metallic materials are known to those skilled in the art, such as aluminum, copper, chromium, iron, steel, stainless steel, titanium, tungsten, zinc, zirconium, molybdenum, etc., including alloys and compounds thereof.
As used herein, “electron affinity” refers to the tendency of an atom to attract or bind a free electron into one of its orbitals. Further, “negative electron affinity” (NEA) refers to the tendency of an atom to either repulse free electrons, or to allow the release of electrons from its orbitals using a small energy input. NEA is generally the energy difference between a vacuum and the lowest energy state within the conduction band. Those of ordinary skill in the art will recognize that negative electron affinity may be imparted by the compositional nature of the material, or the crystal irregularities, e.g. defects, inclusions, grain boundaries, twin planes, or a combination thereof.
As used herein, “dielectric” refers to any material which is electrically resistive. Dielectric materials can include any number of types of materials such as, but not limited to, glass, polymers, ceramics, graphites, alkaline and alkali earth metal salts, and combinations or composites thereof.
As used herein, “work function” refers to the amount of energy, typically expressed in eV, required to cause electrons in the highest energy state of a material to emit from the material into a vacuum space. Thus, a material such as copper having a work function of about 4.5 eV would require 4.5 eV of energy in order for electrons to be released from the surface into a theoretical perfect vacuum at 0 eV.
As used herein, “electrically coupled” refers to a relationship between structures that allows electrical current to flow at least partially between them. This definition is intended to include aspects where the structures are in physical contact and those aspects where the structures are not in physical contact. Typically, two materials which are electrically coupled can have an electrical potential or actual current between the two materials. For example, two plates physically connected together by a resistor are in physical contact, and thus allow electrical current to flow between them. Conversely, two plates separated by a dielectric material are not in physical contact, but, when connected to an alternating current source, allow electrical current to flow between them by capacitive means. Moreover, depending on the insulative nature of the dielectric material, electrons may be allowed to bore through, or jump across the dielectric material when enough energy is applied.
As used herein, “thermoelectric conversion” relates to the conversion of thermal energy to electrical energy or of electrical energy to thermal energy, or flow of thermal energy. Further, in context of the present invention, diamond-like carbon typically operates under thermionic emission. As discussed elsewhere herein, thermionic emission is a property wherein increased electron emission is achieved from a material with increases in temperatures. Diamond-like materials such as amorphous diamond exhibit thermionic emission at temperatures far below that of most materials. For example, many materials tend to exhibit substantial thermionic emission or temperature related effects in emission properties at temperatures over about 1100° C. In contrast, amorphous diamond exhibits increases in emission at temperature changes near room temperature up to 1000° C. or more. Thus, thermionic materials such as amorphous diamond can be useful at temperatures from below room temperature to about 300° C.
As used herein, “electrical generator” refers to thermoelectric conversion devices which are used and configured in a manner to produce electricity.
As used herein, “cooling device” refers to a thermoelectric conversion device which is configured to control heat transfer across the device as a result of an applied voltage.
As used herein, “carbon structures” refers to materials comprised substantially completely of carbon. Non-limiting examples may include microndiamond particles, nanodiamond particles, carbon nanotubes (CNTs), bucky balls, carbon onions, etc.
As used herein, the term “substantially” refers to the complete or nearly complete extent or degree of an action, characteristic, property, state, structure, item, or result. For example, an object that is “substantially” enclosed would mean that the object is either completely enclosed or nearly completely enclosed. The exact allowable degree of deviation from absolute completeness may in some cases depend on the specific context. However, generally speaking the nearness of completion will be so as to have the same overall result as if absolute and total completion were obtained. The use of “substantially” is equally applicable when used in a negative connotation to refer to the complete or near complete lack of an action, characteristic, property, state, structure, item, or result. For example, a composition that is “substantially free of” particles would either completely lack particles, or so nearly completely lack particles that the effect would be the same as if it completely lacked particles. In other words, a composition that is “substantially free of” an ingredient or element may still actually contain such item as long as there is no measurable effect thereof.
As used herein, the term “about” is used to provide flexibility to a numerical range endpoint by providing that a given value may be “a little above” or “a little below” the endpoint.
As used herein, a plurality of items, structural elements, compositional elements, and/or materials may be presented in a common list for convenience. However, these lists should be construed as though each member of the list is individually identified as a separate and unique member. Thus, no individual member of such list should be construed as a de facto equivalent of any other member of the same list solely based on their presentation in a common group without indications to the contrary.
Concentrations, amounts, and other numerical data may be expressed or presented herein in a range format. It is to be understood that such a range format is used merely for convenience and brevity and thus should be interpreted flexibly to include not only the numerical values explicitly recited as the limits of the range, but also to include all the individual numerical values or sub-ranges encompassed within that range as if each numerical value and sub-range is explicitly recited. As an illustration, a numerical range of “about 1 to about 5” should be interpreted to include not only the explicitly recited values of about 1 to about 5, but also include individual values and sub-ranges within the indicated range. Thus, included in this numerical range are individual values such as 2, 3, and 4 and sub-ranges such as from 1-3, from 2-4, and from 3-5, etc., as well as 1, 2, 3, 4, and 5, individually.
This same principle applies to ranges reciting only one numerical value as a minimum or a maximum. Furthermore, such an interpretation should apply regardless of the breadth of the range or the characteristics being described.
The Invention
The present invention involves an amorphous diamond material that can be used to generate electrons upon input of a sufficient amount of energy. As recited in the background section, utilization of a number of materials have been attempted for this purpose, including the diamond materials and devices disclosed in WO 01/39235, which is incorporated herein by reference. Due to its high band gap properties, diamond is unsuitable for use as an electron emitter unless modified to reduce or alter the band gap. Thus far, the techniques for altering diamond band gap, such as doping the diamond with various dopants, and configuring the diamond with certain geometric aspects have yielded electron emitters of questionable use.
It has now been found that various diamond-like carbon materials can easily emit electrons when an energy source is applied. Such materials retain the NEA properties of diamond, but do not suffer from the band gap issues of pure diamond. Thus, electrons energized by applied energy are allowed to move readily through the diamond-like carbon material, and be emitted using significantly lower energy inputs, than those required by diamond. Further, the diamond-like carbon material of the present invention has been found to have a high energy absorption range, allowing for a wider range of energies to be converted into electrons, and thus increasing the conversion efficiency.
A variety of specific diamond-like carbon materials that provide the desired qualities are encompassed by the present invention. In one specific embodiment, the diamond-like carbon material can be amorphous diamond material. One aspect of the amorphous diamond material that facilitates electron emission is the distorted tetrahedral coordination with which many of the carbon atoms are bonded. Tetrahedral coordination allows carbon atoms to retain the sp3 bonding characteristic that may facilitate the surface condition required for NEA, and also provides a plurality of effective band gaps, due to the differing bond lengths of the carbon atom bonds in the distorted tetrahedral configuration. In this manner, the band gap issues of pure diamond are overcome, and the amorphous diamond material becomes effective for emitting electrons. In one aspect of the present invention, the amorphous diamond material can contain at least about 90% carbon atoms with at least about 20% of such carbon atoms being bonded with distorted tetrahedral coordination. In another aspect, the amorphous diamond can have at least about 95% carbon atoms with a least about 30% of such carbon atoms being bonded with distorted tetrahedral coordination. In another aspect, the amorphous diamond can have at least about 80% carbon atoms with at least about 20%, and more preferably at least about 30%, of such carbon atoms being bonded with distorted tetrahedral coordination. In yet another aspect, the amorphous diamond can have at least 50% of the carbon atoms bonded in distorted tetrahedral coordination.
Another aspect of the present amorphous diamond material that facilitates electron emission is the presence of certain geometric configurations. Referring now to
While a number of prior devices have attempted to thusly focus electrons, for example by imparting a plurality of pyramids or cones to an emission surface, none have as of yet, been able to achieve the high current output required to be viable for many applications, using a feasible energy input in a cost effective manner. More often than not, this inadequacy results from the fact that the pyramids, cones, etc. are too large and insufficiently dense to focus the electrons as needed to enhance flow. Such sizes are often greater than several microns in height, thus allowing only a projection density of less than 1 million per square centimeter.
In one aspect of the present invention, the asperity of the emission surface can have a height of from about 10 to about 10,000 nanometers. In another aspect, the asperity of the emission surface can have a height of from about 10 to about 1,000 nanometers. In another aspect, the asperity height can be about 800 nanometers. In yet another aspect, the asperity height can be about 100 nanometers. Further, the asperity can have a peak density of at least about 1 million peaks per square centimeter of emission surface. In yet another aspect, the peak density can be at least about 100 million peaks per square centimeter of the emission surface. In a further aspect, the peak density can be at least about 1 billion peaks per square centimeter of the emission surface. Any number of height and density combinations can be used in order to achieve a specific emission surface asperity, as required in order to generate a desired electron output. However, in one aspect, the asperity can include a height of about 800 nanometers and a peak density of at least about, or greater than about 1 million peaks per square centimeter of emission surface. In yet another aspect, the asperity can include a height of about 1,000 nanometers and a peak density of at least about, or greater than 1 billion peaks per square centimeter of emission surface.
The amorphous diamond material of the present invention is capable of utilizing a variety of different energy input types in order to generate electrons. Examples of suitable energy types can include without limitation, heat or thermal energy, light or photonic energy, and electric and electric field energy. Thus, suitable energy sources are not limited to visible light or any particular frequency range and can include the entire visible, infrared, and ultraviolet ranges of frequencies. Those of ordinary skill in the art will recognize other energy types that may be capable of sufficiently vibrating the electrons contained in the amorphous diamond material to affect their release and movement through and out of the material. Further, various combinations of energy types can be used in order to achieve a specifically desired result, or to accommodate the functioning of a particular device into which the amorphous diamond material is incorporated.
In one aspect of the invention, the energy type utilized can be thermal energy. To this end, an energy absorber and collection layer can be used in connection with or coupled to the diamond-like carbon material of the present invention that aids in the absorption and transfer of heat into the material. As will be recognized by those of ordinary skill in the art, such an absorber can be composed of a variety of materials that are predisposed to the absorption of thermal energy, such as carbon black, etc. In accordance with the present invention, the thermal energy absorbed by the diamond-like carbon material can have a temperature of less than about 500° C. Additionally, the photonic or thermal energy can be sufficient to maintain the cathode at a temperature from about 100° C. to about 1800° C. Typically, an energy input of from about 200° C. to about 300° C. can be common. Additionally, absorber collection layers can be designed for absorbing photonic and/or thermal energy such as carbon black, sprayed graphite particles, or any other dark or black body. In one alternative, the absorber collection layer can have an increased surface roughness to enhance the amount of light and/or heat absorbed. Various methods of providing textured surfaces are known to those skilled in the art.
In another aspect of the present invention, the energy used to facilitate electron flow can be electric field energy (i.e. a positive bias). Thus, in some embodiments of the present invention a positive bias can be applied in conjunction with other energy sources such as heat and/or light. Such a positive bias can be applied to the amorphous diamond material and/or intermediate member described below, or with a variety of other mechanisms known to those of ordinary skill in the art. Specifically, the negative terminal of a battery or other current source can be connected to the electrode and/or amorphous diamond and the positive terminal connected to the intermediate material or gate member placed between the amorphous diamond electron emission surface and the anode.
The diamond-like carbon material of the present invention can be further coupled to, or associated with a number of different components in order to create various devices. Referring now to
In one aspect of the present invention, the entire diamond-like carbon thermoelectric conversion device is a solid assembly having each layer in continuous intimate contact with adjacent layers and/or members. Most typically, the anode and the cathode are substantially parallel such that the distance between the anode and cathode is substantially the same across the entire device.
Those of ordinary skill in the art will readily recognize other components that can, or should, be added to the assembly of
The above-recited components can take a variety of configurations and be made from a variety of materials. Each of the layers discussed below can be formed using any number of known techniques such as, but not limited to, vapor deposition, thin film deposition, preformed solids, powdered layers, screen printing, or the like. In one aspect, each layer is formed using deposition techniques such as PVD, CVD, or any other known thin-film deposition process. In one aspect, the PVD process is sputtering or cathodic arc. Further, suitable electrically conductive materials and configurations will be readily recognized by those skilled in the art for the cathode 25 and the anode 30. Such materials and configurations can be determined in part by the function of the device into which the assembly is incorporated. Additionally, the layers can be brazed, glued, or otherwise affixed to one another using methods which do not interfere with the thermal and electrical properties as discussed below. Although, a variety of geometries and layer thicknesses can be used typical thicknesses are from about 10 nanometers to about 3 microns for the amorphous diamond emission surface and from about 1 micron to about 1 millimeter for other layers.
The cathode 25 can be formed having a base member 60 with a layer of amorphous diamond 5 coated over at least a portion thereof. The base member can be formed of any conductive electrode material such as a metal. Suitable metals include, without limitation, copper, aluminum, nickel, alloys thereof, and the like. One specific example of a material used in forming the base member is copper. In another aspect, the material used in forming the base member can be an aluminum-magnesium alloy. Similarly, the anode 30 can be formed of the same materials as the base member or of different conductive materials. In one aspect, for example, the cathode material may be copper. As a general guideline, the anode and/or cathode base member can have a work function of from about 3.5 eV to about 6.0 eV and in a second embodiment from about 3.5 eV to about 5.0 eV. Although a variety of thicknesses are functional for the cathode and/or anode, typical thickness range from about 0.1 mm to about 10 mm.
The base member 60 of the cathode 25 can be a single or multiple layers. In one aspect, the base member is a single layer of material. In another aspect, the base member may include a first layer and a second layer (not shown) such that the second layer is coupled between the first layer and the energy input surface of the amorphous diamond layer. The second layer acts to improve electron conduction to the emission surface of the diamond layer. Generally, when a second layer is used as part of the base member, it is preferred that the second layer comprise a material which has a work function which is less than the work function of the first layer. In one aspect, the second layer comprises a material having a low work function of from about 2.0 eV to about 4.0 eV, although work functions of from about 2.0 eV to about 3.0 eV are also suitable. In another aspect, the second layer comprises a material having a work function of from about 1.5 eV to about 3.5 eV. Suitable materials for use in the second layer include, without limitation, Cs, Sm, Al—Mg, Li, Na, K, Rb, Be, Mg, Ca, Sr, Ba, B, Ce, Al, La, Eu, and mixtures or alloys thereof. In one specific aspect, the second layer can comprise Cs, Sm, Al—Mg and alloys thereof. In a more specific aspect, the second layer can comprise Be, Mg, Cs, Sm, or combinations thereof. In another more specific aspect, the second layer can comprise Cs.
In order to improve heat transfer toward the diamond-like carbon layer, the second layer can comprise a material which has a thermal conductivity of greater than about 100 W/mK. As with other layers or members, a variety of thicknesses can be used however, the second layer is often from about 1 micron to about 1 millimeter. Those skilled in the art will recognize that typical low work function materials also readily oxidize. Thus, it may be desirable to form at least the second layer, and often the entire thermoelectric conversion device, under a vacuum or other inert environment.
Without wishing to be bound to any particular theory, the ability of the present invention to produce electricity can be viewed as a stepping process related to the band gap between materials, work function, and thermal conductivity of each layer. Specifically, the second layer of the cathode can be made of a material that acts to step the electrons closer to vacuum energy or conduction band, (i.e. decrease the band gap between the first layer and vacuum energy). Additionally, the second layer can have a high thermal conductivity in order to improve electron flow toward the electron emission surface. The electrons in the second layer can then be transmitted to the diamond-like carbon layer where the distorted tetrahedral coordinations of the amorphous diamond create a variety of different work function and band gap values (i.e. within the unoccupied conduction band) within the amorphous diamond layer, such that some of the electron states approach and exceed the vacuum energy.
The material for use in the intermediate member can then be chosen to minimize heat loss by allowing the electrons to transfer, or “step” back down to the anode material. This decreases the amount of energy which is lost in the system. For example, a large step from amorphous diamond down to a high work function material can be used in the present invention; however, some of the electrical energy is lost as heat. Thus, more than one intermediate member and/or base member layers can be incorporated into the device to provide varying degrees of “steps up” and “steps down” between the energy band gaps among the respective layers. Thus, the intermediate member can be formed of a plurality of layers each having different electrical and thermal properties.
In addition, it is frequently desirable to minimize the thermal conductivity of the intermediate member such that there is a thermal gradient maintained from the cathode to the anode. Further, operating temperatures can vary greatly depending on the application and energy source. Cathode temperatures can be from about 100° C. to about 1800° C. and can often be above about 300° C. Alternatively, cathode temperatures can be below about 100° C. such as from about 0° C. to about 100° C. Although temperatures outside these ranges can be used, these ranges provide an illustration of the temperature gradient which can exist across the devices of the present invention.
As shown in
It is also contemplated that the insulating materials according to various aspects of the present invention may also include inorganic insulating materials. Non-limiting examples of such materials may include sulfurs, talcs, pyrophylites, and combinations thereof.
Carbon structures may include any form of carbon that, when coated with an insulating material such as PTFE, demonstrates desired thermal and electrical properties. Non-limiting examples of carbon structures may include, however, nano-diamond particles, carbon nanotubes (CNTs), bucky balls, carbon onions, and combinations thereof.
Nano-diamond particles refer to diamond particles having a size in the nano-range. It should be noted that size ranges may vary depending on a particular use or configuration of a particular device. In one aspect, however, nano-diamond particles may range in size from about 1 nm to about 1000 nm. In another aspect, nano-diamond particles may range in size from about 1 nm to about 100 nm. In yet another aspect, nano-diamond particles may range in size from about 10 nm to about 50 nm. Such nano-particles may take a variety of shapes, including round, oblong, square, euhedral, etc., and they may be single crystal or polycrystalline.
CNTs are essentially graphene planes (the basal planes of graphite) in a rolled geometry of a tube. Single-walled nanotubes (SWNT) containing a single CNT exhibit desirable properties for many applications. However, the SWNTs are currently difficult to produce in large quantities and high purity. Currently most CNTs produced contain multiple layers wherein several CNTs are concentrically formed, and are therefore referred to as multi-walled carbon nanotubes (MWNT). A typical SWNT has a diameter of 1.3 nanometers; and a MWNT may range from about 10 to 20 nanometers, depending on the number of layers they contain and the manufacturing process used. Just like graphite, the inter-atomic distance on the same graphene plane in a CNT is 1.45 Å (angstrom or 10−8 cm), and the separation between any two walls in a MWNT is about 3.4 Å.
The following descriptions of intermediate members are described for PTFE coated CNTs. It should be noted that this descriptions is for convenience, and may equally apply to other types of insulating materials and carbon structures.
As has been described, a useful material for the intermediate member may include PTFE coated CNTs. The linear CNT structures may allow a current path within a relatively small fraction of the volume of the intermediate member. The bulk of the layer can be thermally insulating due to the higher relative volume of the PTFE. Thus in one aspect, the plurality of carbon structures may be coated with the layer of an insulating material such that the plurality of carbon structures is substantially isolated from one another by a portion of the insulating material. A uniform dispersion of CNTs within the PTFE material may further enhance the thermal properties of the intermediate member. Various methods of coating the PTFE onto the CNT structures are contemplated. For example, the structures may be sprayed with PTFE, dipped in PTFE, etc. Depending on the method of coating, the intermediate member may be utilized in a variety of thicknesses. For example, in one aspect, the intermediate member may be less than about 20 microns thick. In another aspect, the intermediate member may be less than about 10 microns thick. In yet another the intermediate member may be less than about 5 microns thick.
Various methods of forming the plurality of insulating material-coated carbon structures are contemplated, all of which are considered to be within the present scope. In one aspect, the carbon structures may be mixed into molten PTFE. Ultrasonic vibration may be introduced into the molten mixture to preclude clumping or clustering of the carbon structures. The molten PTFE/carbon structure mixture may then be pressed or otherwise applied to the diamond-like carbon layer of the cathode and allowed to cool. Alternatively, the PTFE/carbon structure mixture may be pressed or otherwise applied to the anode. Additionally, the PTFE/carbon structure mixture may be sandwiched in-between the diamond-like carbon layer of the cathode and the anode and then be allowed to cool.
In another aspect of the present invention, a mixture of PTFE-coated carbon structures can be spray coated onto the diamond-like carbon layer of the cathode, the anode, or both. As such, the mixture may be formed into an aerosol and sprayed onto the receiving surface of the electrode.
As has been described, the intermediate member has thermally insulating properties that make it ideal for incorporation into devices according to aspects of the present invention. In one aspect, for example, the intermediate member may have a thermal conductivity of from about 0.1 W/mK to about 10.0 W/mK. In another aspect, the intermediate member may have a thermal conductivity of from about 1.0 W/mK to about 5.0 W/mK. In addition to thermally insulation, the intermediate member has electrically conductive properties that also make it ideal for incorporation into devices according to aspects of the present invention. In one aspect, for example, the intermediate member may have an electrical resistivity less than about 1×106 Ω-cm at 20° C. In another aspect, the intermediate member may have a thermal resistivity less than about 1 Ω-cm at 20° C.
In accordance with additional aspects of the present invention, the intermediate member can also be made from other dielectric materials. The dielectric material can be any dielectric material known to one of ordinary skill in the art, including polymers, glasses, ceramics, inorganic compounds, organic compounds, or mixtures thereof. Examples include, without limitation, BaTiO3, PZT, Ta2O3, PET, PbZrO3, PbTiO3, NaCl, LiF, MgO, TiO2, Al2O3, BaO, KCl, Mg2SO4, fused silica glass, soda lime silica glass, high lead glass, and mixtures or composites thereof. In one aspect, the dielectric material is BaTiO3. In another aspect, the dielectric material is PZT. In another aspect, the dielectric material is PbZrO3. In yet another aspect, the dielectric material is PbTiO3. Additionally, the dielectric material can be a graphitic material. A number of graphitic materials can have a sufficiently high electrical resistivity to support a voltage of 0.1 V. Further, materials having a relatively low thermal conductivity such as hexagonal boron nitride (about 40 W/mK), alumina, zirconia, other ceramics, or dielectrics listed above can be mixed with relatively higher thermal conductivity graphite (above about 200 W/mK). For example, in one currently preferred embodiment the intermediate member can comprise graphite and hexagonal boron nitride. These materials can be provided as a layered combination or as a compressed powder mixture.
Almost any material useful in construction of a capacitor can be useful. However, in one aspect, the dielectric material can also be a piezoelectric material. The presence of the diamond-like layer on the cathode makes using almost any other type of material for the intermediate member impractical.
The dielectric material can be configured in any way that maintains separation between the diamond-like carbon layer and the anode. Alternatively, diamond-like carbon layers can be electrically coupled to both electrodes. In another alternative aspect, the intermediate member can be a single layer or a number of layers. In this case the dielectric material can be tailored to improve conversion efficiency and the more closely match the bandgap of adjacent materials. Advantageously, this configuration of dielectric layers may decrease the incidence of preferred pathways of electron flow, due to a more uniform distribution of charge across the intermediate member. Further, in such multi-layered configurations, the intermediate member can include one or more additional layers of diamond-like carbon.
The thickness of the dielectric layer can be any thickness that allows the conversion of thermal energy to electrical energy or visa versa in various aspect of the present invention. Specifically, the thickness and composition of the intermediate member can be adjusted to control resistivity. In addition, adjusting the thickness of the intermediate member is a balance between voltage and current, e.g., efficiency. For example, a thinner intermediate member will increase current, while also decreasing voltage. Diamond materials typically have a bandgap of about 5 eV, and in some cases greater than 5 eV, depending on the ratio of sp2/sp3 bonding in the amorphous diamond material. Prior art solar cells tend to have about 0.5 V output (silicon based devices have a bandgap of only 1.1 eV which can result in about 0.6 V), while diamond solar cells of the present invention can have up to 5.5 V output. Further, amorphous diamond presents a wide range of bandgaps such that dopants are not required. Thus, excited electrons can generally be maintained at higher energy states without immediately falling back to the ground state. The energy states in amorphous diamond are, however, discrete, unlike metallic materials which are overlapping. Consequently, electrons can “step” up the discrete energy positions much like stepping up a ladder. Thus, the thickness of the intermediate member can be used to design the thermoelectric conversion device for a specific application. In some applications it can be desirable to have a lower voltage and a higher current, while other applications can require higher voltage with less current. Typically, the intermediate member can be a solid material which is of a sufficient thickness and material type capable of supporting a voltage of greater than about 0.1 V, such as from about 0.1 V to about 6 V, and preferably from about 1 V to about 5.5 V. As mentioned above, the material and the thickness of the intermediate member can affect the resistivity and thus the voltage which can be supported across the intermediate member.
Although the thickness of a particular material is best determined based on experimentation and the guidelines set forth herein, the intermediate member can have a thickness sufficient to achieve a resistivity from about 0.1 μΩ-cm to about 100 μΩ-cm, and preferably from about 20 μΩ-cm to about 80 μΩ-cm. This can often correspond to a thickness which will vary with the material, but can usually range from about 0.05 μm to about 500 μm thick. In another aspect, the dielectric material can be from about 0.2 μm to about 100 μm thick. In yet another aspect, the layer of dielectric material is from about 0.5 μm to about 10 μm thick. For example; an intermediate member formed of PZT at a thickness of about 1 μm can provide good results.
Additionally, amorphous diamond has a high radiation hardness such that it is resistant to aging and degradation over time. In contrast, typical semiconductor materials are UV degradable and tend to become less reliable over time. As mentioned elsewhere, electrons in amorphous diamond are excited via the thermoelectric effect rather than the photoelectric effect. As such, amorphous diamond materials exhibit a change in electron emission properties with changes in temperature. For example, amorphous diamond can be used to convert a substantial portion of heat into electricity, regardless of the temperature. Thus, as the temperature increases, a substantial increase in electron emission is also realized. Conversion efficiencies of over 30% and in many cases over 50% can be achieved in solar cells constructed in accordance with the principles of the present invention.
In one aspect, the intermediate member can be formed of a material having a thermal conductivity of less than about 200 W/mK, and in many cases less than about 100 W/mK. Further, the intermediate member can have a resistivity of less than about 80 μΩ-cm at 20° C. In choosing appropriate materials for use in the intermediate member, at least two factors are considered. First, the material should act to minimize thermal transfer across the layer. Thus, materials having a relatively low thermal conductivity are desirable. In one aspect, the intermediate member comprises a material having a thermal conductivity less than about 200 W/mK such as below about 80 W/mK. Materials having thermal conductivities of below about 40 W/mK can also be advantageously used. Second, the intermediate member should be relatively conductive. In one aspect, the intermediate member also has a resistivity of less than about 80 μΩ-cm at 20° C. and more preferably below about 10 μΩ-cm at 20° C. Specifically, reference is now made to
Referring to
In an alternative embodiment, the intermediate member can be constructed so as to satisfy the above guidelines regarding thermal and electrical conductivity while expanding the types of materials which can be used. Specifically, the intermediate member can be formed of a primary thermally insulating material having a plurality of apertures extending therethrough (not shown). Although electrically conductive materials are of course preferred any thermally insulating material can be used. Suitable insulating materials can be chosen by those skilled in the art. Non-limiting examples of suitable thermally insulating materials include ceramics and oxides. Several currently preferred oxides include ZrO2, SiO2, and Al2O3. The apertures extend from the electron emission surface of the diamond layer to the anode. One convenient method of forming the apertures is by laser drilling. Other methods include anodization of a metal such as aluminum. In such a process small indentations can be formed in the aluminum surface, and then upon anodization, electrons will flow preferentially through the indented areas and dissolve the aluminum to form straight and parallel apertures. The surrounding aluminum is oxidized to form Al2O3.
Once the apertures are formed, a more highly conductive metal can be deposited into the apertures. The apertures can be filled by electrodeposition, physical flow, or other methods. Almost any conductive material can be used, however in one aspect the conductive material can be copper, aluminum, nickel, iron, and mixtures or alloys thereof. In this way, conductive metals can be chosen which have high conductivity without the limitations on thermal conductivity. The ratio of surface of area covered by apertures to surface area of insulating material can be adjusted to achieve an overall thermal conductivity and electrical conductivity within the guidelines set forth above. Further, the pattern, aperture size, and aperture depth can be adjusted to achieve optimal results. In one aspect, the surface area of the apertures constitute from about 10% to about 40% of the surface of the intermediate member which is in contact with the electron emission surface of the amorphous diamond layer.
Because of the ease with which electrons can be generated using the diamond-like carbon material of the present invention, it has been found that inducing electron flow using an applied electric field facilitates the absorption of heat at the electron input surface, thus enabling the electron emitter of the present invention to be used as a cooling device. As such, the present invention encompasses a cooling device that is capable of absorbing heat by emitting electrons under an induced electrical field. Such a device can take a variety of forms and utilize a number of supporting components, such as the components recited in the electrical generator above. In one aspect, the cooling device is capable of cooling an adjacent area to a temperature below 100° C. Alternatively, the present invention can be used as a heat pump to transfer heat from a low heat area or volume to an area having higher amounts heat.
In these embodiments of the present invention, application of electrical current results in a forced heat flow from the cathode to the anode. In this way, the thermoelectric conversion device can also function as a cooling device. Such a cooling device can be used in connection with dissipating heat from high powered electronics such as ULSI, laser diodes, CPUs, or the like, or as a cooling device for use in refrigeration systems.
The amorphous diamond material used in the present invention can be produced using a variety of processes known to those skilled in the art. However, in one aspect, the material can be made using a cathodic arc method. Various cathodic arc processes are well known to those of ordinary skill in the art, such as those disclosed in U.S. Pat. Nos. 4,448,799; 4,511,593; 4,556,471; 4,620,913; 4,622,452; 5,294,322; 5,458,754; and 6,139,964, each of which is incorporated herein by reference. Generally speaking, cathodic arc techniques involve the physical vapor deposition (PVD) of carbon atoms onto a target, or substrate. The arc is generated by passing a large current through a graphite electrode that serves as a cathode, and vaporizing carbon atoms with the current. The vaporized atoms also become ionized to carry a positive charge. A negative bias of varying intensity is then used to drive the carbon atoms toward an electrically conductive target. If the carbon atoms contain a sufficient amount of energy (i.e. about 100 eV) they will impinge on the target and adhere to its surface to form a carbonaceous material, such as amorphous diamond. Amorphous diamond can be coated on almost any metallic substrate, typically with no, or substantially reduced, contact resistance.
In general, the kinetic energy of the impinging carbon atoms can be adjusted by the varying the negative bias at the substrate and the deposition rate can be controlled by the arc current. Control of these parameters as well as others can also adjust the degree of distortion of the carbon atom tetrahedral coordination and the geometry, or configuration of the amorphous diamond material (i.e. for example, a high negative bias can accelerate carbon atoms and increase sp bonding). By measuring the Raman spectra of the material the sp3/sp2 ratio can be determined. However, it should be kept in mind that the distorted tetrahedral portions of the amorphous diamond layer are neither sp nor sp2 but a range of bonds which are of intermediate character. Further, increasing the arc current can increase the rate of target bombardment with high flux carbon ions. As a result, temperature can rise so that the deposited carbon will convert to more stable graphite. Thus, final configuration and composition (i.e. band gaps, NEA, and emission surface asperity) of the amorphous diamond material can be controlled by manipulating the cathodic arc conditions under which the material is formed. Additionally, other processes can be used to form DLC such as various vapor deposition processes, e.g. PVD or the like. The diamond-like carbon material and other layers of the device can be formed without the necessity of a vacuum space between the electron emitting layer and the anode which greatly reduces production costs and increase reliability of the devices formed thereby.
Various applications of the devices and methods discussed herein will occur to those skilled in the art. In one aspect, the thermoelectric conversion devices of the present invention can be incorporated into devices which produce waste heat. The cathode side or energy input surface of the present invention can be coupled to a heat source such as a boiler, battery such as rechargeable batteries, CPUs, resistors, other electrical components, or any other device which produces waste heat as a byproduct of its operation which is not otherwise utilized. For example, an electrical generator of the present invention can be coupled to a laptop battery. As such the electrical generator can supplement the power supply and thus extend battery life. In another example, one or more electrical generators can be attached to the outer surface of a boiler or other heat producing unit of a manufacturing plant to likewise supplement the electrical demands of the manufacturing process. Thus, as can be seen, a wide variety of applications can be devised using thermal, light or other energy sources to produce electricity in useful amounts.
Moreover, diamond-like carbon may be coated onto ordinary electrodes to facilitate the flow of electrons. Such electrodes can be used in batteries and electro-deposition of metals, such as electroplating. In one aspect, the electrodes can be used in an aqueous solution. For example, electrodes that are used to monitor the quality of water or other food stuff, such as juice, beer, soda, etc. by measuring the resistivity of the water. Due to its anti-corrosive properties, electrodes of amorphous diamond pose a significant advantage over conventional electrodes.
One particular application where amorphous diamond electrodes would be of significant advantage is in electro-deposition applications. Specifically, one problem experienced by most electro-deposition devices is the polarization of the electrode by the absorption of various gasses. However, due to the strongly inert nature of amorphous diamond, cathodes and anodes coated therewith are virtually unpolarizable. Further, this inert nature creates an electric potential in aqueous solution that is much higher than that obtained using metallic or carbon electrodes. Under normal circumstances, such a voltage would dissociate the water. However, due to the high potential of amorphous diamond, the solute contained in the solution is driven out before the water can be dissociated. This aspect is very useful, as it enables the electro-deposition of elements with high oxidation potentials, such as Li and Na which has been extremely difficult, if not impossible in the past.
In a similar aspect, because of the high potential achieved by amorphous diamond electrodes in solution, solutes that are present in very minute amounts may be driven out of solution and detected. Therefore, the material of the present invention is also useful as part of a highly sensitive diagnostic tool or device which is capable of measuring the presence of various elements in solution, for example, lead, in amounts as low as parts per billion (ppb). Such applications include the detection of nearly any element that can be driven or attracted to an electrical charge, including biomaterials, such as blood and other bodily fluids, such as urine.
In one alternative embodiment of the present invention, at least one of the cathode and the anode can be configured to transmit light. One example of an electrode configured to transmit light can be constructed of a transparent material coated with indium tin oxide. The transparent or translucent material can be any transparent material known, such as a glass, or a polymer such as a plastic or an acrylic. In such embodiments, the transparency can be desirable for aesthetic or practical reasons. A more detailed description of specific light emitting devices and configurations that utilize DLC or amorphous diamond and configurations therefor is contained in Applicant's copending U.S. patent application Ser. No. 11/045,016, filed on Jan. 26, 2005, which is incorporated herein by reference.
The cathode and the anode can be of any shape or configuration that may be of use in the various potential embodiments of the present invention. In one aspect, the cathode and the anode can be planar. In another aspect, the cathode and/or anode can be rigid. However, in many commercial embodiments, it can be desirable to provide flexible materials. Thus, providing a flexible cathode and/or anode can allow for construction of flexible solar cells.
Other aspects of the present invention contemplate improving the reliability of the thermoelectric conversion device. In one aspect, the reliability can be improved by avoiding organic adhesives to bond the electrodes together. Many organic materials are not stable, particularly at higher temperatures. One way to avoid using organic adhesives is to deposit a layer of dielectric material and any cathode and/or anode materials directly on an electrode. One skilled in the art would recognize various methods of accomplishing this, including, without limitation, the use of a low temperature plasma spray. In another aspect, organic adhesives can be avoided by bonding together various layers with low temperature sintering. As such, sintering should be accomplished below about 500° C. in order to avoid degradation of the amorphous diamond layer. In yet another aspect, a thermally stable adhesive can be used such as, without limitation, a silicone adhesive.
As alluded to above, the present invention encompasses methods for making the diamond-like thermoelectric conversion devices disclosed herein, as well as methods for the use thereof. In addition to the electrical generator and cooling devices recited above, a number of devices that operate on the principles of emitting electrons may beneficially utilize the amorphous diamond material of the present invention. A number of such devices will be recognized by those skilled in the art, including without limitation, transistors, ultra fast switches, ring laser gyroscopes, current amplifiers, microwave emitters, luminescent sources, and various other electron beam devices.
In one aspect, a method for making an amorphous diamond material capable of emitting electrons by absorbing a sufficient amount of energy, includes the steps of providing a carbon source, and forming an amorphous diamond material therefrom, using a cathodic arc method. A method for generating a flow of electrons or generating an electrical current can include the steps of forming an amorphous diamond material as recited herein, and inputting an amount of energy into the material that is sufficient to generate electron flow. The second layer of the base member of the cathode and the intermediate member can be formed using CVD, PVD, sputtering, or other known process. In one aspect, the layers are formed using sputtering. In addition, the anode can be coupled to the intermediate member using CVD, PVD, sputtering, brazing, gluing (e.g. with a silver paste) or other methods known to those skilled in the art. Although the anode is commonly formed by sputtering or arc deposition, the anode can be coupled to the intermediate member by brazing.
In an optional step, the diamond-like carbon thermoelectric conversion devices can be heat treated in a vacuum furnace. Heat treatment can improve the thermal and electrical properties across the boundaries between different materials. The diamond-like carbon thermoelectric conversion device can be subjected to a heat treatment to consolidate interfacial boundaries and reduce material defects. Typical heat treatment temperatures can range from about 200° C. to about 800° C. and more preferably from about 350° C. to about 500° C. depending on the specific materials chosen.
The following are examples illustrate various methods of making electron emitters in accordance with the present invention. However, it is to be understood that the following are only exemplary or illustrative of the application of the principles of the present invention. Numerous modifications and alternative compositions, methods, and systems can be devised by those skilled in the art without departing from the spirit and scope of the present invention. The appended claims are intended to cover such modifications and arrangements. Thus, while the present invention has been described above with particularity, the following Examples provide further detail in connection with several specific embodiments of the invention.
A copper foil is glued to a polyimide support layer. A one micron layer of amorphous diamond is deposited on the exposed copper foil electrode using a cathodic arc process. The amorphous diamond has a 50 nm asperity. An intermediate member of PZT is deposited by screen printing to a thickness of 30 μm on the amorphous diamond. A layer of silver grease is coated on the PZT intermediate member by screen printing to form an anode. The assembly is then cured in an oven to drive off the binder used in screen printing and to consolidate the device. Attachment of wires to the copper electrodes can allow this thermoelectric conversion device to act as either an electrical generator by absorption of heat or as a cooling device by application of an electrical current.
The same procedure is followed as in Example 1, except the PZT layer is replaced by a mixture of graphite powder and hexagonal boron nitride powder.
The same procedure is followed as in Example 1, except the PZT layer is replaced by a mixture of graphite powder and aluminum oxide powder.
The same procedure is followed as in Example 1, except the PZT layer is replaced by a mixture of graphite powder and zirconium oxide powder.
The same procedure is followed as in Example 1, except the PZT layer is replaced by a silver impregnated epoxy such that the resistivity is sufficient to support and withstand a voltage of 0.1 V across the two electrodes.
A glass plate is coated with carbon black and then silver grease is coated over the carbon black as a cathode layer. Amorphous diamond is then formed on the silver grease by cathodic arc. An intermediate member of BaTiO3 is then deposited on the amorphous diamond. A second coating of silver grease is formed on the intermediate member followed by a thin layer of epoxy. These successive layers are coated in such a way that substantially no air or moisture is trapped in or between each layer. Air reduces flow of electrons and moisture will deteriorate the coating layers and reduce reliability.
The transparent glass outer layer can trap heat from the sun, similar to the green house effect. Carbon black will absorb the sun light to increase the temperature (e.g. to 200° C.). The thermionic amorphous diamond will convert the heat to electricity through emission of electrons into the intermediate member. The BaTiO3 intermediate member is used to control the resistivity and hence voltage generated. Silver grease is used as flexible electrodes, although other flexible conductive materials can be used. The epoxy can serve as a convenient packaging material for mechanical protection as well as insulation.
The above design is simple and easy to manufacture by automation. The thickness and uniformity of each layer is important. If the rigid glass is replaced by flexible PET or other transparent or translucent material, the solar panel becomes bendable so it can be mounted on a variety of substrates such as the curved roof of an automobile.
Referring to
An amorphous diamond material was made as shown in
The amorphous diamond material was then coupled to an electrode to form a cathode, and an electrical generator in accordance with the present invention was formed. An external electrical bias was applied and the resultant electrical current generated by the amorphous diamond material was measured and recorded as shown in
A 10 micron layer of copper can be deposited on a substrate using sputtering. Onto the copper was deposited 2 microns of samarium by sputtering onto the copper surface under vacuum. Of course, care should be taken so as to not expose the beryllium to oxidizing atmosphere (e.g. the entire process can be performed under a vacuum). A layer of amorphous diamond material can then be deposited using the cathodic arc technique as in Example 4 resulting in a thickness of about 0.5 microns. Onto the growth surface of the amorphous diamond a layer of magnesium can be deposited by sputtering, resulting in a thickness of about 10 microns. Finally a 10 microns thick layer of copper was deposited by sputtering to form the anode.
A 10 micron layer of copper can be deposited on a substrate using sputtering. Onto the copper was deposited 2 microns of cesium by sputtering onto the copper surface under vacuum. Of course, care should be taken so as to not expose the cesium to oxidizing atmosphere (e.g. the entire process can be performed under a vacuum). A layer of amorphous diamond material can then be deposited using the cathodic arc technique as in Example 4 resulting in a thickness of about 65 nm. Onto the growth surface of the amorphous diamond a layer of molybdenum can be deposited by sputtering, resulting in a thickness of about 16=n. Additionally, a 20 nm thick layer of In—Sn oxide was deposited by sputtering to form the anode. Finally, a 10 micron layer of copper was deposited on the In—Sn layer by sputtering. The cross-sectional composition of the assembled layers is shown in part by
A first set of indium tin oxide (ITO) coated glass electrodes are constructed by coating a first ITO electrode with an amorphous diamond layer by cathodic arc, and a second ITO electrode with copper-doped zinc sulfide by screen printing. The ITO electrodes are then glued together with the coated surfaces facing each other using an epoxy. The total epoxy-filled gap between the coated surfaces of the ITO electrodes is approximately 60 microns.
A second set of ITO coated glass electrodes are constructed similarly to the first set, with the exception that the first ITO electrode lacks an amorphous diamond layer. These ITO electrodes are then glued together with the copper-doped zinc sulfide coating facing the first electrode using an epoxy. The total epoxy-filled gap between the first ITO electrode and the coated surface of the second ITO electrode is approximately 60 microns.
A direct current is applied to the first and second sets of electrodes of Example 7. When direct current is applied to the first set of electrodes, 40 Volts is required to generate luminescence from the copper-doped zinc sulfide layer. When direct current is applied to the second set of electrodes, 80 Volts is required to generate luminescence from the copper-doped zinc sulfide layer.
A set of electrodes is constructed as per the first electrodes of Example 7, having a diamond-like carbon layer. An alternating current is applied to the set of electrodes. At 60 Hz, 40 Volts is required to generate a given level of luminescence from the copper-doped zinc sulfide material. At 100 Hz, 3 Volts is required to generate a level of luminescence that is greater than the level of luminescence generated at 60 Hz. At 1000 Hz, 3 Volts is able to generate a level of luminescence that is greater than the level of luminescence generated at 100 Hz. At 3500 Hz, 3 Volts is able to generate a level of luminescence that is greater than the level of luminescence generated at 1000 Hz.
A set of ITO electrodes are constructed by coating both ITO electrodes with amorphous diamond layers by cathodic arc. Because amorphous diamond is deposited on both ITO electrodes, heat utilized in further construction should be less than 500° C. in order to avoid degradation of the amorphous carbon layers. Copper-doped zinc sulfide powder is mixed with a binder and spin coated on a substrate to form a thin layer. The layer of copper-doped zinc sulfide is then sandwiched between two layers of dielectric material, dried, roasted, and heat treated to diffuse the dopant into the zinc sulfide.
CNTs are fluorine treated and dispersed in molten PTFE with ultrasonic vibration to prevent clustering of the CNTs. A fluorinated amorphous diamond coated ITO glass panel is pressed onto the molten PTFE/CNT mixture to cause the mixture to wet and stick to the amorphous diamond layer of the ITO glass panel. After the ITO glass panel is allowed to cool, silver grease is applied to the solidified PTFE/CNT layer with a screen printer to form an anode. The assembly is then cured in an oven to drive off the binder used in screen printing and to consolidate the device. The device receives sun light from the ITO glass panel. A portion of this energy is absorbed to accelerate electrons, and a portion becomes heat that warms up the amorphous diamond layer. Thermal phonons are also accumulated to accelerate electrons. The excited electrons flow to the silver grease electrode.
Of course, it is to be understood that the above-described arrangements are only illustrative of the application of the principles of the present invention. Numerous modifications and alternative arrangements may be devised by those skilled in the art without departing from the spirit and scope of the present invention and the appended claims are intended to cover such modifications and arrangements. Thus, while the present invention has been described above with particularity and detail in connection with what is presently deemed to be the most practical and preferred embodiments of the invention, it will be apparent to those of ordinary skill in the art that numerous modifications, including, but not limited to, variations in size, materials, shape, form, function and manner of operation, assembly and use may be made without departing from the principles and concepts set forth herein.
This application is a continuation-in-part of U.S. patent application Ser. No. 11/157,179 filed Jun. 20, 2005, which is a continuation-in-part of U.S. patent application Ser. No. 11/112,724, filed on Apr. 21, 2005, which is a continuation-in-part of U.S. patent application Ser. No. 11/045,016, filed on Jan. 26, 2005, which is a continuation-in-part of U.S. patent application Ser. No. 10/460,052, filed on Jun. 11, 2003, now issued as U.S. Pat. No. 6,949,873, which is a continuation-in-part of U.S. patent application Ser. No. 10/094,426, filed on Mar. 8, 2002, now issued as U.S. Pat. No. 6,806,629, each of which are incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 11157179 | Jun 2005 | US |
| Child | 11510478 | Aug 2006 | US |
| Parent | 11112724 | Apr 2005 | US |
| Child | 11157179 | Jun 2005 | US |
| Parent | 11045016 | Jan 2005 | US |
| Child | 11112724 | Apr 2005 | US |
| Parent | 10460052 | Jun 2003 | US |
| Child | 11045016 | Jan 2005 | US |
| Parent | 10094426 | Mar 2002 | US |
| Child | 10460052 | Jun 2003 | US |
