Title:
High thermal conductivity materials aligned within resins
Kind Code:
A1


Abstract:
In one embodiment the present invention provides for a high thermal conductivity resin that comprises a host resin matrix 32 a high thermal conductivity filler 30. The high thermal conductivity filler forms a continuous organic-inorganic composite with the host resin matrix, and the fillers have an aspect ratio of between 3-100. The fillers are substantially evenly distributed through the host resin matrix, and are aligned in essentially the same direction. In some embodiments the resins are highly structured resin types.



Inventors:
Smith, James David Blackhall (Monroeville, PA, US)
Stevens, Gary (Surrey, GB)
Wood, John William (Winter Springs, FL, US)
Application Number:
11/152985
Publication Date:
12/15/2005
Filing Date:
06/14/2005
Assignee:
Siemens Westinghouse Power Corporation
Primary Class:
Other Classes:
524/495
International Classes:
C08K3/04; C08K3/14; C08K3/18; C08K3/22; C08K3/28; (IPC1-7): C08K3/18; C08K3/04
View Patent Images:



Primary Examiner:
NERANGIS, VICKEY M
Attorney, Agent or Firm:
Siemens Corporation (Iselin, NJ, US)
Claims:
1. A high thermal conductivity resin comprising: a host resin matrix; and a high thermal conductivity filler; wherein said high thermal conductivity filler forms a continuous organic-inorganic composite with said host resin matrix; and wherein high thermal conductivity fillers have an aspect ratio of between 3-100; wherein said high thermal conductivity fillers are substantially evenly distributed through said host resin matrix, and wherein said high thermal conductivity fillers are aligned in essentially the same direction.

2. The high thermal conductivity resin of claim 1, wherein said high thermal conductivity fillers are from 1-1000 nm in length.

3. The high thermal conductivity resin of claim 1, wherein said high thermal conductivity fillers are at least one of diamond, Al2O3, AlN, MgO, ZnO, BeO, BN, Si3N4, SiC and SiO2.

4. The high thermal conductivity resin of claim 1, wherein said high thermal conductivity fillers are surface coated onto a non-high thermal conductivity filler.

5. The high thermal conductivity resin of claim 1, where said resin is a highly structured resin.

6. A method for making a thermal conductivity resin comprising: impregnating a host resin matrix with a high thermal conductivity filler; distributing said high thermal conductivity filler evenly through said resin matrix; aligning at least 75% of said high thermal conductivity fillers within 15 degrees of a common direction; and curing said resin matrix; wherein said high thermal conductivity fillers have an aspect ratio of between 3-100.

7. The method of claim 6, wherein said high thermal conductivity filler forms a continuous organic-inorganic composite with said host resin matrix.

8. The method of claim 6, wherein said high thermal conductivity fillers are from 1-1000 nm in length.

9. The method of claim 6, wherein the alignment is done by the self-alignment and aggregation of said high thermal conductivity fillers.

10. The method of claim 6, wherein the alignment is done by the application of an external field.

11. The method of claim 10, wherein said external field is one of mechanical, electric, magnetic, sonic and ultrasonic.

12. The method of claim 6, further comprising first surface coating said high thermal conductivity fillers with field responsive materials

13. The method of claim 6, further comprising coating field responsive fillers with high thermal conductivity coatings.

14. The method of claim 6, wherein said host resin matrix comprises a highly structured resin that is aligned uniformly with said high thermal conductivity filler.

15. A high thermal conductivity resin comprising: a host resin matrix; and a high thermal conductivity filler; wherein said high thermal conductivity filler forms a continuous organic-inorganic composite with said host resin matrix; and wherein said high thermal conductivity fillers have an aspect ratio of between 3-100; wherein said high thermal conductivity fillers are substantially evenly distributed through said host resin matrix, and wherein said high thermal conductivity fillers form substructures within said host resin matrix; wherein said substructures comprise at least one of columns, layers and super lattices.

16. The high thermal conductivity resin of claim 15, wherein said high thermal conductivity fillers are at least one of oxides, nitrides and carbides.

17. The high thermal conductivity resin of claim 15, wherein said high thermal conductivity fillers contain at least one of metallic and organo-metallic compounds that are capable of responding to an external field.

18. A porous media impregnated with a high thermal conductivity resin comprising: a porous media; and a high thermal conductivity material loaded resin, wherein said high thermal conductivity material comprises 5-60% by volume of said resin; wherein said high thermal conductivity materials have aspect ratios of 10-50 and are aligned within said porous media in essential the same direction.

Description:

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority to U.S. provisional 60/580,023, filed Jun. 15, 2004, by Smith, et al., which is incorporated herein by reference. This also claims priority to U.S. application Ser. No. 11/106,845, filed on Apr. 15, 2005, which is incorporated herein by reference. This application is further related to US patent applications High Thermal Conductivity Materials Incorporated into Resins, High Thermal Conductivity Materials with Grafted Surface Functional Groups, Structured Resin Systems with High Thermal Conductivity Fillers, all by Smith, et al., all filed herewith, and all incorporated herein by reference.

FIELD OF THE INVENTION

The field of the invention relates to resins with aligned high thermal conductivity materials incorporated therein.

BACKGROUND OF THE INVENTION

With the use of any form of electrical appliance, there is a need to electrically insulate conductors. With the push to continuously reduce the size and to streamline all electrical and electronic systems there is a corresponding need to find better and more compact insulators and insulation systems.

Various epoxy resin materials have been used extensively in electrical insulation systems due to their practical benefit of being tough and flexible electrical insulation materials that can be easily adhered to surfaces. Traditional electrical insulation materials, such as mica flake and glass fiber, can be surface coated and bonded with these epoxy resins, to produce composite materials with increased mechanical strength, chemical resistance and electrical insulating properties. In many cases epoxy resins have replaced traditional varnishes despite such materials having continued use in some high voltage electrical equipment.

Good electrical insulators, by their very nature, also tend to be good thermal insulators, which is undesirable. Thermal insulating behavior, particularly for air-cooled electrical equipment and components, reduces the efficiency and durability of the components as well as the equipment as a whole. It is desirable to produce electrical insulation systems having maximum electrical insulation and minimal thermal insulation characteristics.

Electrical insulation often appears in the form of insulating tapes, which themselves have various layers. Common to these types of tapes is a paper layer that is bonded at an interface to a fiber layer, both layers tending to be impregnated with a resin. A favored type of insulation material is a mica-tape. Improvements to mica tapes include catalyzed mica tapes as taught in U.S. Pat. No. 6,103,882. The mica-tape may be wound around conductors to provide extremely good electrical insulation. An example of this is shown in FIG. 1. Illustrated here is a coil 13, comprising a plurality of turns of conductors 14, which in the example illustrated here are assembled into a bakelized coil. The turn insulation 15 is prepared from a fibrous material, for example glass or glass and Dacron which is heat treated. Ground insulation for the coil is provided by wrapping one or more layers of composite mica tape 16 about the bakelized coil 14. Such composite tape may be a paper or felt of small mica flakes combined with a pliable backing sheet 18 of, for example, glass fiber cloth or polyethylene glycol terephthalate mat, the layer of mica 20 being bonded thereto by a liquid resinous binder. Generally, a plurality of layers of the composite tape 16 are wrapped about the coil depending upon voltage requirements. A wrapping of an outer tape 21 of a tough fibrous material, for example, glass fiber, may be applied to the coil.

Generally, multiple layers of the mica tape 16 are wrapped about the coil with sixteen or more layers generally being used for high voltage coils. Resins are then impregnated into the tape layers. Resins can even be used as insulation independently from the insulating tape. Unfortunately this amount of insulation only further adds to the complications of dissipating heat. What is needed is electrical insulation that can conduct heat higher than that of conventional methods, but that does not compromise the electrical insulation and other performance factors including mechanical and thermal compatability.

Other difficulties with the prior art also exist, some of which will be apparent upon further reading.

SUMMARY OF THE INVENTION

With the foregoing in mind, methods and apparatuses consistent with the present invention, which inter alia facilitates the transport of phonons through a high thermal conductivity (HTC) impregnated medium to reduce the mean distances between the HTC materials below that of the phonon mean free path length. This reduces the phonon scattering and produces a greater net flow or flux of phonons away from the heat source. The resins may then be impregnated into a host matrix medium, such as a multi-layered insulating tape.

High Thermal Conductivity (HTC) organic-inorganic hybrid materials may be formed from discrete two-phase organic-inorganic composites, from organic-inorganic continuous phase materials based on molecular alloys and from discrete organic-dendrimer composites in which the organic-inorganic interface is non-discrete within the dendrimer core-shell structure. Continuous phase material structures may be formed which enhance phonon transport and reduce phonon scattering by ensuring the length scales of the structural elements are shorter than or commensurate with the phonon distribution responsible for thermal transport, and/or that the number of phonon scattering centers are reduced such as by enhancing the overall structural order of the matrix, and/or by the effective elimination or reduction of interface phonon scattering within the composite. Continuous organic-inorganic hybrids may be formed by incorporating inorganic, organic or organic-inorganic hybrid nano-particles in linear or cross-linked polymers (including thermoplastics) and thermosetting resins in which nano-particles dimensions are of the order of or less than the polymer or network segmental length (typically 1 to 50 nm or greater). These various types of nano-particles will contain reactive surfaces to form intimate covalently bonded hybrid organic-inorganic homogeneous materials. Similar requirements exist for inorganic-organic dendrimers which may be reacted together or with matrix polymers or reactive resins to form a continuous material. In the case of both discrete and non-discrete organic-inorganic hybrids it is possible to use sol-gel chemistry to form a continuous molecular alloy. The resulting materials will exhibit higher thermal conductivity than conventional electrically insulating materials and may be used as bonding resins in conventional mica-glass tape constructions, when utilized as unreacted vacuum-pressure impregnation resins and as stand alone materials to fulfill electrical insulation applications in rotating and static electrical power plant and in both high (approximately over 5 kV) and low voltage (approximately under 5 kV) electrical equipment, components and products.

The formation of engineered electrical insulation materials having prescribed physical properties and performance characteristics, and based on the use of nano-to-micro sized inorganic fillers in the presence of organic host materials, requires the production of particle surfaces which can form an intimate interface with the organic host. This may be achieved through the grafting of chemical groups onto the surface of the fillers to make the surface chemically and physically compatible with the host matrix, or the surfaces may contain chemically reactive functional groups that react with the organic host to form covalent bonds between the particle and the host. The use of nano-to-micro sized inorganic fillers in the presence of organic host materials requires the production of particles with defined surface chemistry in addition to bulk dielectric and electrical properties and thermal conductivity. Most inorganic materials do not allow independent selection of structural characteristics such as shape and size and properties to suit different electrical insulation applications or to achieve composites having the right balance of properties and performance. This may be achieved by selecting particles with appropriate bulk properties and shape and size characteristics and then modifying the surface and interfacial properties and other characteristics to achieve the additional control of composite properties and performance required for electrical insulation applications. This may be achieved by appropriate surface coating of the particles which may include the production of metallic and non-metallic inorganic oxides, nitrides, carbides and mixed systems and organic coatings including reactive surface groups capable of reacting with appropriate organic matrices which act as the host material in the electrical insulation system. The resulting hybrid materials and composites in unreacted or partially reacted form may be used as bonding resins in mica-glass tape constructions, as unreacted vacuum-pressure impregnation resins for conventional mica tape constructions, in other glass fiber, carbon fiber and ply-type and textile composites and as stand alone materials to fulfill electrical insulation applications in rotating and static electrical power plant and in both high and low voltage electrical equipment, components and products.

In one embodiment the present invention provides for a high thermal conductivity resin that comprises a host resin matrix containing a high thermal conductivity filler. The high thermal conductivity filler forms a continuous organic-inorganic composite with the host resin matrix, and the fillers have an aspect ratio of between 3-100. The fillers are substantially evenly distributed through the host resin matrix, and are aligned in essentially the same direction or they link within a percolation structure that crosses the material. In some embodiments the resins are highly structured resin types.

In another embodiment the present invention provides for a method for making a thermal conductivity resin that comprises impregnating a host resin matrix with a high thermal conductivity filler and distributing the high thermal conductivity filler evenly through the resin matrix. Then aligning at least 75% of the high thermal conductivity fillers within 15 degrees of a common direction and curing or semi-curing the resin matrix. The high thermal conductivity fillers have an aspect ratio of between 3-100. In some embodiments, the filler forms a continuous organic-inorganic composite with the host resin matrix. In particular embodiments host resin matrix comprises a highly structured resin that is aligned uniformly with the high thermal conductivity filler.

In one embodiment the alignment is done by the self-alignment and aggregation of the high thermal conductivity fillers forming a percolation structure, and in another the alignment is done by the application of an external field. Examples of the external field include mechanical, electric, magnetic, sonic and ultrasonic. In some cases the fillers are first surface coated with field responsive materials, and in other cases field responsive fillers are coated with high thermal conductivity materials.

In yet another embodiment the present invention provides for a high thermal conductivity resin that comprises a host resin matrix and a high thermal conductivity filler. The high thermal conductivity filler forms a continuous organic-inorganic composite with the host resin matrix, and the high thermal conductivity fillers have an aspect ratio of between 3-100. The fillers are substantially evenly distributed through the host resin matrix, and the high thermal conductivity fillers form substructures within the host resin matrix. The substructures may be at least one of columns, layers and super lattices.

In still another embodiment the present invention provides for a porous media impregnated with a high thermal conductivity resin that comprises a porous media and a high thermal conductivity material loaded resin. The high thermal conductivity material comprises 5-60% by volume of the resin, and the high thermal conductivity materials have aspect ratios of 10-50 and are aligned within the porous media in essential the same direction.

Other embodiments of the present invention also exist, which will be apparent upon further reading of the detailed description.

BRIEF DESCRIPTION OF THE FIGURES

The invention is explained in more detail by way of example with reference to the following drawings:

FIG. 1 shows the use of an insulating tape being lapped around a stator coil.

FIG. 2 illustrates phonons traveling through a loaded resin of the present invention.

FIG. 3 illustrates phonons traveling through a loaded resin with aligned fillers of the present invention.

FIG. 4 illustrates a column arrangement of aligned fillers according to one embodiment of the present invention.

FIG. 5 illustrates a cross-sectional view of a layer arrangement of aligned fillers according to one embodiment of the present invention.

FIG. 6 illustrates HTC fillers aligned within a highly structured resin according to one embodiment of the present invention.

DETAILED DESCRIPTION OF THE INVENTION

High thermal conductivity (HTC) composites comprise a resinous host network combined with fillers that are two phase organic-inorganic hybrid materials. The organic-inorganic hybrid materials are formed from two phase organic-inorganic composites, from organic-inorganic continuous phase materials that are based on molecular alloys, and from discrete organic-dendrimer composites in which the organic-inorganic interface is non-discrete with the dendrimer core-shell structure. Phonon transport is enhanced and phonon scattering is reduced by ensuring the length scales of the structural elements are shorter than or commensurate with the phonon distribution responsible for thermal transport.

Two phase organic-inorganic hybrids may be formed by incorporating inorganic micro, meso or nano-particles in linear or cross linked polymers (thermoplastics) and thermosetting resins. Host networks include polymers and other types of resins, definitions of which are given below. In general, the resin that acts as a host network may be any resin that is compatible with the particles and, if required, is able to react with the groups introduced at the surface of the filler. Nano-particle dimensions are typically of the order of or less than the polymer network segmental length. For example 1-30 nm. The inorganic particles contain reactive surfaces to form covalently bonded hybrid organic-inorganic homogeneous materials. The particles may be oxides, nitrides, carbides and hybrid stoichiometric and non-stoichiometric mixes of the oxides, nitrides and carbides, more examples of which are given below.

The inorganic particles are surface treated to introduce a variety of surface functional groups which are capable of participating in reactions with the host network. The surface functional groups include but are not limited to hydroxyl, carboxylic, amine, epoxide, silane and vinyl groups. The groups may be applied using wet chemical methods, non-equilibrium plasma methods, chemical vapor and physical vapor deposition, laser beams, sputter ion plating and electron and ion beam evaporation methods. Some of these techniques can also be used when applying coating to fillers.

The discrete organic-dendrimer composites may be reacted together or with the resin matrix to form a single material. The surface of the dendrimer can contain reactive groups similar to those mentioned above, which will either allow dendrimer-dendrimer or dendrimer-organic matrix reactions to occur. The dendrimer will have an inorganic core and an organic shell containing the reactive groups of interest. It may also be possible to have an organic core with an inorganic shell which also contains reactive groups such as hydroxyl or silane groupings which can participate in inorganic reactions similar to those involved in common sol-gel chemistries.

In regards to the use of non-discrete organic-inorganic hybrids it is possible to use sol-gel chemistry to form a continuous molecular alloy. Gel sol-chemistries involving aqueous and non-aqueous reactions may be used. Other compounds for the formation of organic-inorganic hybrids include the polyhedral oligomeric silsesquioxanes (POSS), tetraethyl orthosilicate (TEOS) and tetrabutyl orthotitanate (TBOT) and related monomeric and oligomeric hybrid compounds which are organic functionalized inorganic compounds. In the example of POSS, molecules are built around a building block of R—SiO1.5 in which the R group is chosen to compatibilize with and/or react with other organic compounds and the host network. The base compounds may be combined to yield larger molecules commensurate with the size of polymer segment and coil structures. POSS may be used to create organic-inorganic hybrids and may be grafted into existing polymers and networks to control properties, including thermal conductivity. The materials may be obtained from suppliers such as Aldrich™ Chemical Co., Hybrid Plastics™ Inc. and Gelest™ Inc.

As mentioned, it is important to control the structural form of the materials to reduce phonon scattering. This can be further assisted by using nano-particles whose matrices are known to exhibit high thermal conductivity and to ensure that the particles size and its interfacial characteristics with the resin are sufficient to sustain this effect, and also to satisfy the length scale requirement to reduce phonon scattering. A choice of structures that are more highly ordered will also benefit this, including reacted dendrimer lattices having both short and longer range periodicity and ladder or ordered network structures that may be formed from a host resin, such as liquid crystal epoxies and polybutadienes.

The filled resins may be used as bonding resins in a variety of industries such as circuit boards and insulating tapes. A particular kind of insulating tape is the mica-glass tape used in the electrical generator fields. Resins with these types of tapes can be used as bonding resins, or as impregnating resins as is known in the art. The filled resin may also be used in the electrical generator field without the tapes to fulfill electrical insulation applications in the rotating and static electrical equipment components.

The tapes may be impregnated with resin before or after being applied to electrical objects. Resin impregnation techniques include VPI and GVPI, discussed more below. In VPI, once a tape is lapped and impregnated it is compressed. Once in position, the resin in the compressed tape is cured, which effectively locks the position of the HTC materials. In some embodiments the resin is cured in a two stage process, as will be apparent to one of ordinary skill in the art. However, optimal compression of the loaded HTC materials favors a completely uncured resin during the compression stage.

FIG. 2 shows one embodiment of the present invention. Illustrated here are HTC materials 30 loaded into a resinous matrix 32. Phonons 34 traveling through the matrix have a mean path length n, this is the phonon mean free path. This path length can vary depending on the exact composition of the resin matrix, but is generally from 2 to 100 nm, and more typically 5-50 nm, for resins such as epoxy resins. Therefore the mean distance between the loaded HTC materials should be on average less than this distance. Note that the distance between the HTC materials can vary in the thickness versus transverse direction of the tape, and it is generally the thickness direction where the spacing needs to be optimalized.

As phonons 34 travel through the resin 32 they will tend to pass along the embedded HTC materials 30. This will increase the local phonon flux since the raw HTC materials will have a thermal conductivity of between 10-1000 W/mK, as opposed to the resin which is about 0.1-0.5 W/mK. As phonons pass along a loaded HTC material the phonons 36 pass to the next HTC material if the distance between the materials is less than n, therefore the HTC materials form an interconnecting network. FIG. 2 illustrates an idealized path. In practice there will be phonon scattering as the phonons pass between the resin and HTC materials, although the shorter the distance between the materials, and the better the match of phonon propagation characteristics between the HTC materials and the resin, the less the scattering.

The amount of HTC materials loaded in the resin could actually be quite low, for example about 10% as illustrated in FIG. 2. The average distances, or length scales, between loaded HTC materials therefore may be slightly greater than n, however, a large percentage will still be less than n and therefore fall within embodiments of the present invention. In particular embodiment, the percentage materials that are less than n distance from the next HTC material is over 50%, with particular embodiment-being over 75%. In particular embodiment the average length of the HTC materials is greater than n, which further aids in phonon transport.

The shorter n the greater the concentration of loaded HTC materials, and conversely, the greater the particle size, the less HTC materials needed. Particular embodiment use 5-60% loaded HTC materials by total volume of the resins and fillers, with more particular embodiments at 25-40%. When the resin is impregnated into the tape, it will fill up the spaces between the tape fibers and substrates. The HTC distribution within the tape at this point, however, is often not optimized, and can even have the mean distance between HTC materials greater than n. Practice of the present invention then compresses the resin impregnated tapes and reduces the distances between the loaded HTC materials.

When a loaded resin is being impregnated into a tape, the fibers or particles of the tape act to block some of the HTC materials, particularly if the resin is 30% or more filler. However, by compressing the tapes, the reverse happens, and more fillers are trapped within the tape as the HTC materials attach themselves to non-mobile parts of the overall structure. The HTC fillers even get pinned to one another. In the embodiments given, it has been implied that the fillers do not react with the resin matrix, however, in some embodiments the fillers do form covalent bonds with the resin and form more homogeneous matrixes. In a homogenous matrix, the resin molecules that are bound to fillers will be retained better than the unbound resin molecules during compression.

Resins are used in a plurality of industries, and have a large number of uses. Different properties of the resins affect not only their uses, but also the quality and efficiency of the products that they are used with. For example, when resins are used in electrical insulation applications, their characteristics of dielectric strength and voltage endurance needs to be high, as does the thermal stability and thermal endurance. However, often contrary to these objectives, resins usually will also have a low thermal conductivity. The present invention balances the various physical properties of resins and the insulation system they are introduced into to produce a system that has a higher thermal conductivity than conventional electrically insulating materials while maintaining adequate, and even enhancing, key physical properties such as dielectric strength, voltage endurance, thermal stability and thermal endurance, mechanical strength and viscoelastic response. Delamination and microvoid formation resulting from stresses caused by thermal, vibration and mechanical cycling effects are reduced or eliminated. As used herein, the term resin refers to all resins and epoxy resins, including modified epoxies, polyesters, polyurethanes, polyimides, polyesterimides, polyetherimides, bismaleimides, silicones, polysiloxanes, polybutadienes, cyanate esters, hydrocarbons etc. as well as homogeneous blends of these resins. This definition of resins includes additives such as cross-linking agents, accelerators and other catalysts and processing aids. Certain resins, such as liquid crystal thermosets (LCT) and 1,2 vinyl polybutadiene combine low molecular weights characteristics with good crosslinking properties. The resins can be of an organic matrix, such as hydrocarbons with and without hetero atoms, an inorganic matrix, containing silicate and/or alumino silicate components, and a mixture of an organic and inorganic matrix. Examples of an organic matrix include polymers or reactive thermosetting resins, which if required can react with the reactive groups introduced on inorganic particle surfaces. Cross-linking agents can also be added to the resins to manipulate the structure and segmental length distribution of the final crosslinked network, which can have a positive effect on thermal conductivity. This thermal conductivity enhancement can also be obtained through modifications by other resin additives, such as catalysts, accelerators and other processing aids. Certain resins, such as liquid crystal thermosets (LCT) and 1,2 vinyl polybutadiene combine low molecular weights characteristics with good crosslinking properties. These types of resins tend to conduct heat better because of enhanced micro and macro ordering of their sub-structure which may lead to enhanced conduction of heat as a result of improved phonon transport. The better the phonon transport, the better the heat transfer.

When the high thermal conductivity fillers of the present invention are mixed with resins they form a continuous product, in that there is no interface between the resins and the fillers. In some cases, covalent bonds are formed between the fillers and the resin. However, continuous is somewhat subjective and depends on the scale to which the observer is using. On the macro-scale the product is continuous, but on the nano-scale there can still be distinct phases between the fillers and the resin network. Therefore, when referring high thermal conductivity fillers mixing with the resin, they form a continuous organic-inorganic composite, on the macro-scale, while on the micro-scale the same mixture can be referred to as a hybrid. Similarly there is continuity between the filler and any coating that they may have.

As mentioned, filled resin may be used in the electrical generator field without the tapes to fulfill electrical insulation applications in the rotating and static electrical equipment components. The use of high thermal conductivity materials in a generator is multiple. Within the stator coil there are component materials other than the groundwall which must have high thermal conductivity to optimize the design. Likewise other components associated with the coils to maximize heat removal. Improvements to stator design dictate that improvements be made to rotor design so that generator efficiency can by maximized.

The distribution of the HTC fillers/materials in the resin can be of equal importance to the type of HTC filler used. It is important that the fillers do not agglomerate together and overly react with each other rather than the resin matrix. What is also important is the alignment that the HTC materials take once they are in the resin. Typically the fillers will be randomly aligned and may self aggregate if left to conventional incorporation techniques. However, the present invention aligns the HTC fillers either in the resin alone or when the resin is impregnated into a porous medium so that heat may pass more along the direction of the aligned fillers.

FIG. 3 shows one embodiment of this. The HTC materials 30 in the host resin 32 are aligned in roughly the same direction d. As a result heat 36 passing though the resin will tend to travel in the direction of d more readily than in other directions. Not all of the HTC materials need to aligned, but one embodiment of the present inventions envisions at least 75% of the nanofillers being aligned within +/−15° of d.

The alignment of the HTC fillers may be controlled by characteristics such as surface coating and surface functional groups, which can also affect the general distribution of the fillers in the resin by having the surface groups more or less reactive with one another, while maintaining optimal reactivity with the resin matrix. Inorganic surface coatings such as diamond like coatings, oxides, nitrides and carbides may be generated that, when combined with filler size and shape distribution, provide a defined percolation structure with control of the bulk thermal and electrical conductivity of the insulation system. Reactive surface functional groups may also be formed from surface groups that are part of an inorganic coating or may be achieved by applying additional functional groups, or both. Additional functional groups include such as organic coatings include hydroxyl, carboxylic, amine, epoxide, silane or vinyl groups which will be available for chemical reaction with the host organic matrix as described above.

In regards to surface coated fillers, the orientation, position and structural organization of the fillers may be controlled either through the selected nature of the surface coating to align and aggregate itself, or by the application an external field. Examples of such fields are magnetic, electric and mechanical (AC/dynamic, DC/static, pulsed and combinations thereof), sonic and ultrasonic. For example, dielectrophoresis or electrophoresis may be used. Coatings such as TiO2 would respond to electric fields, while coatings containing or consisting of Ni, Co, Mn, V, Cr, or Fe compounds would respond to magnetic fields, in either a paramagnetic or ferromagnetic manner. Organo-metallic compound may also be used, such as metal acetylacetonates, ferrocene, metal porphyrins and metal phthalocyanines.

It is also possible that HTC materials can be surface coated onto non-HTC fillers that are responsive to the fields mentioned above. For example, a TiO2 core could be given a BN surface coating: This can in fact be more effective than putting a field responsive surface coating onto an HTC filler, since by this method the bulk of the filler will be responsive to the field, while heat passing to the filler will tend to travel along the surface.

The resins simply need to be cured to lock the alignment in place. However, in some embodiments, the resins may be unreacted or may be in a semi-cured, or even a semi-fluid state so that the resins may be properly applied or positioned before curing. For example, a resin with HTC fillers may be impregnated into a tape and the HTC fillers aligned. The tape may then be wound around an electrical object, the HTC fillers maintaining their alignment relative to the tape. Once the object has been wound, the resin may then be cured. In the case of VPI and GVPI the resin containing the HTC fillers would be impregnated into the mica tape, then aligned by a field, and the alignment locked in during the cure process.

the above description assumes that the fillers align with little direct contact with one another. However, in some embodiments the fillers form structures within the resin, such as columns, layers or super lattices and pearl necklaces. Examples of these are given in FIGS. 4-6. As used herein, materials, particles and fillers when used in conjunction with HTC are synonymous.

Referring to FIG. 4, a column 42 is present along with other HTC fillers 30 in the resin 32. In this example the non-columnar fillers 30 are aligned in approximately the same direction as the column. Heat passing though the resin (not shown) will tend to favor the closely packed column. Note that this is just one example, other examples may include higher particle concentrations as well as translation of particles into the column due to the external field effect or self-agglomeration. The columns could be formed due to a combination of effects, such as the switching on and off of a field, or a slow change in the field, at measured times.

Referring to FIG. 5, a cross-sectional view of layers 44 are seen within a resin 32 along with some scattered fillers 30. Similarly to the columns of FIG. 4, heat will pass along the layer with a diminished heat flow passing between the layers. Similarly in a super lattice heat will conduct along the super lattice structure rapidly. The shape of the super lattice, for example, can be a ring or cage unit cell of nanoparticles or POSS type molecules, which could create an organized crystallographic type structure e.g. cubic or face-centered cubic super lattice.

The resins, such as liquid crystal resins in the liquid phase can also be aligned by the same fields of force, in a similar manner as that described. This will give a preferred orientation and structural characteristic of the resin which may be locked by cross-linking to achieve the required fixed structures. The liquid crystals may also interact with fillers during orientation leading to dual structural alignment to create enhanced properties. Also, fillers may be covalently bound to the resin molecules and be aligned in concert.

FIG. 6 shows an example of this. In this figure the resin is an LCT type resin that forms mesogenic groups 40 that tend to self align on a small scale. The mesogenic groups tend to be from 0.5-100 nm in length, depending on the type of resin, and aggregates of mesogenic groups can be several hundred nanometers long. Aligned within the mesogenic groups are HTC fillers 30. In particular embodiments the mesogenic groups are aligned in concert with the HTC fillers. The alignment of the nanofillers can thereby aid in the in the alignment of the mesogenic groups, creating aligned area that are thousands of nanometers in length. Conversely, it is also possible for highly structured resins systems to help align the impregnated HTC fillers.

One embodiment of the present invention adds high thermal conductivity (HTC) materials to resins to improve the thermal conductivity of the resins. In some embodiments the other physical properties of the resins are reduced in a trade-off with higher thermal conductivity, but in other embodiments, some of the other physical properties will not be significantly affected, and in some particular embodiments these other properties will be improved. In particular embodiments, the HTC materials are added to resins, such as LCT epoxy, that have ordered sub-structures. When added to these types of resins, the amount of HTC material used can be reduced versus use in resins without ordered sub-structures.

The HTC materials loaded into the resins are of a variety of substances that can be added so that they may physically and/or chemically interact with or react with the resins to improve thermal conductivity. In one embodiment, the HTC materials are dendrimers, and in another embodiment they are nano or micro inorganic fillers having a defined size or shape including high aspect ratio particles with aspect ratios (ratio mean lateral dimension to mean longitudinal dimension) of 3 to 100 or more, with a more particular range of 10-50.

In a related embodiment, the HTC materials may have a defined size and shape distribution. In both cases the concentration and relative concentration of the filler particles is chosen to enable a bulk connecting (or so-called percolation) structure to be achieved which confers high thermal conductivity with and without volume filling to achieve a structurally stable discrete two phase composite with enhanced thermal conductivity. In another related embodiment, the orientation of the HTC materials increases-thermal conductivity. In still another embodiment, the surface coating of the HTC materials enhances phonon transport. These embodiments may stand apart from other embodiments, or be integrally related. For example, dendrimers are combined with other types of highly structured materials such as thermoset and thermoplastic materials. They are uniformly distributed through a resin matrix such that the HTC materials reduce phonon scattering and provide micro-scale bridges for phonons to produce good thermally conducting interfaces between the HTC materials. The highly structured materials are aligned so that thermal conductivity is increased along a single direction or directions to produce either localized or bulk anisotropic electrically insulating materials. In another embodiment HTC is achieved by surface coating of lower thermal conductivity fillers with metal oxides; carbides or nitrides and mixed systems having high thermal conductivity which are physically or chemically attached to fillers having defined bulk properties, such attachment being achieved by processes such as chemical vapour deposition and physical vapour deposition and also by plasma treatment.

In related embodiments, the HTC materials form essentially homogenous mixtures with the resins, essentially free of undesired microscopic interfaces, variable particle wetting and micro void formation. These homogeneous materials form a continuous-phase material which are non-discrete at length scales shorter than either the phonon wavelength or phonon mean free path in conventional electrical insulating materials. In some embodiments, intentional interfaces can be placed in the resin structure so as to control dielectric breakdown. In insulating materials, dielectric breakdown will occur given the right conditions. By controlling the nature and spatial distribution of the interfaces in two-phase system, dielectric breakdown strength and long term electrical endurance can be enhanced. Increases in dielectric strength will take place in part because of increased densification, the removal of micro voids and a higher level of internal mechanical compression strength.

Resins of the present invention may be used for impregnation of other composite constructions such as a mica tape and glass and polyester tape. In addition to the standard mica (Muscovite,Phlogopite) that is typically used for electrical insulation there is also Biotite mica as well as several other mica-like Alumino-Silicate materials such as Kaolinite, Halloysite, Montmorillonite and Chlorite. Montmorillonite has lattices in its structure which can be readily intercalated with polymer resins, metal cations and nano particles to give high dielectric strength composites.

In other embodiments, the present invention is used as a continuous coating on surfaces where insulation is desired; note that “continuous coating” is a description of a macro-scale application. In a continuous coating, the resin forms a coating on materials without the need for a tape or other substrate. When used with a substrate, the HTC materials can be combined with the resin by a variety of different methods. For example, they can be added prior to the resin being added to the substrate, or the HTC materials can be added to the substrate before the resin is impregnated thereon, or the resin can be added first, followed by the HTC material and then an additional impregnation of resin. Other fabrication and process methods will be apparent to one of ordinary skill in the art.

In one embodiment the present invention uses novel organic-inorganic materials which offer higher thermal conductivity and also maintain or enhance other key properties and performance characteristics. Such materials have applications in other high voltage and low voltage electrical insulation situations where high thermal conductivity confers advantage in terms of enhanced power rating, reduced insulation thickness, more compact electrical designs and high heat transfer. The present invention adds nano, meso, and micro inorganic HTC-materials such as alumina, magnesium oxide, silicon carbide, boron nitride, aluminium nitride, zinc oxide and diamond, as well as others, to give higher thermal conductivity. These materials can have a variety of crystallographic and morphological forms and they may be processed with the matrix materials either directly or via a solvent which acts as a carrier liquid. The solvent mixture may be used to mix the HTC-materials into the matrix to various substrates such as mica-tape. In contrast, molecular hybrid materials which form another embodiment of the present invention, do not contain discrete interfaces, and have the advantages conferred by an inorganic phase within an organic. These materials may also confer enhancement to other physical properties such as thermal stability, tensile strength, flexural strength, and impact strength, variable frequency and temperature dependant mechanical moduli and loss and general viscoelastic response, etc.

In another embodiment, the present invention comprises discrete organic-dendrimer composites in which the organic-inorganic interface is non-discrete with a dendrimer core-shell structure. Dendrimers are a class of three-dimensional nanoscale, core-shell structures that build on a central core. The core may be of an organic or inorganic material. By building on a central core, the dendrimers are formed by a sequential addition of concentric shells. The shells comprise branched molecular groups, and each branched shell is referred to as a generation. Typically, the number of generations used is from 1-10, and the number of molecular groups in the outer shell increase exponentially with the generation. The composition of the molecular groups can be precisely synthesized and the outer groupings may be reactive functional groups. Dendrimers are capable of linking with a resin matrix, as well as with each other. Therefore, they may be added to a resin as an HTC material, or, in other embodiments, may form the matrix themselves without being added to traditional resins.

The molecular groups can be chosen for their ability to react, either with each other or with a resin. However, in other embodiments, the core structure of the dendrimers will be selected for their own ability to aid in thermal conductivity; for example, metal oxides as discussed below.

Generally, the larger the dendrimer, the greater its ability to function as a phonon transport element. However, its ability to permeate the material and its percolation potential can be adversely affected by its size so optimal sizes are sought to achieve the balance of structure and properties required. Like other HTC materials, solvents can be added to the dendrimers so as to aid in their impregnation of a substrate, such as a mica or a glass tape. In many embodiments, dendrimers will be used with a variety of generations with a variety of different molecular groups.

Commercially available organic Dendrimer polymers include Polyamido-amine Dendrimers (PAMAM) and Polypropylene-imine Dendrimers (PPI) and PAMAM-OS which is a dendrimer with a PAMAM interior structure and organo-silicon exterior. The former two are available from Aldrich Chemical™ and the last one from Dow-Corning™.

Similar requirements exist for inorganic-organic dendrimers which may be reacted together or with matrix polymers or reactive resins to form a single material. In this case the surface of the dendrimer could contain reactive groups similar to those specified above which will either allow dendrimer-dendrimer, dendrimer-organic, dendrimer-hybrid, and dendrimer-HTC matrix reactions to occur. In this case the dendrimer will have an inorganic core and an organic shell, or vice-versa containing either organic or inorganic reactive groups or ligands of interest. It is therefore also possible to have an organic core with an inorganic shell which also contains reactive groups such as hydroxyl, silanol, vinyl-silane, epoxy-silane and other groupings which can participate in inorganic reactions similar to those involved in common sol-gel chemistries.

In all cases phonon transport is enhanced and phonon scattering reduced by ensuring the length scales of the structural elements are shorter than or commensurate with the phonon distribution responsible for thermal transport. Larger HTC particulate materials can actually increase phonon transport in their own right, however, smaller HTC materials can alter the nature of the resin matrix, thereby affect a change on the phonon scattering. This may be further assisted by using nano-particles whose matrices are known to exhibit high thermal conductivity and to ensure that the particle size and interface characteristics are sufficient to sustain this effect and also to satisfy the length scale requirements for reduced phonon scattering. It is also necessary to consider the choice of structures that are more highly ordered including reacted dendrimer lattices having both short and longer range periodicity and ladder or ordered network structures that may be formed from matrices such as liquid crystal epoxy resins and polybutadienes. A resin matrix of the prior art will have a maximum thermal conductivity of about 0.15 W/mK. The present invention provides resins with a thermal conductivity of 0.5 to 5 W/mK and even greater.

Continuous organic-inorganic hybrids may be formed by incorporating inorganic nano-particles in linear or crosslinked polymers and thermosetting resins in which nano-particles dimensions are of the order of or less than the polymer or network segmental length (typically 1 to 50 nm). This would include, but is not exclusive to three routes or mechanisms by which this can occur (i) side chain grafting, (ii) inclusive grafting e.g. between two polymer chain ends, (iii) cross-link grafting involving at least two and typically several polymer molecules. These inorganic nano-particles will contain reactive surfaces to form intimate covalently bonded hybrid organic-inorganic homogeneous materials. These nano-particles may be metal oxides, metal nitrides, and metal carbides, as well as some non-metal oxides, nitrides and carbides. For example, alumina, magnesium oxide and zinc oxide and other metal oxides, boron nitride and aluminum nitride and other metal nitrides, silicon carbide and other carbides, diamond of natural or synthetic origin, and any of the various physical forms of each type and other metal carbides and hybrid stoichiometric and non-stoichiometric mixed oxides, nitrides and carbides. More specific examples of these include Al2O3, AlN, MgO, ZnO, BeO, BN, Si3N4, SiC and SiO2 with mixed stoichiometric and non-stoichiometric combinations. Further, these nano-particles will be surface treated to introduce a variety of surface functional groups which are capable of participating in reactions with the host organic polymer or network. It is also possible to coat non-HTC materials, such as silica and other bulk filler materials, with an HTC material. This may be an option when more expensive HTC materials are used.

The volume percentage of the HTC materials in the resin may be up to approximately 60% or more by volume, and more particularly up to approximately 35% by volume. Higher volume filling tends to give higher structural stability to a matrix. However, with control of the size and shape distribution, degree of particle association and alignment the HTC materials can occupy as little as 1% by volume or less. Although, for structural stability reasons, it might be useful to add an amount greater than the minimum needed for percolation to occur. Therefore the resin can withstand physical strains and deformation without damaging the percolation structure and the HTC characteristics.

The addition of surface functional groups may include hydroxyl, carboxylic, amine, epoxide, silane or vinyl groups which will be available for chemical reaction with the host organic polymer or network forming resin system. These functional groups may be naturally present on the surface of inorganic fillers or they may be applied using wet chemical methods, non-equilibrium plasma deposition including plasma polymerization, chemical vapour and physical vapour deposition, laser beams, sputter ion plating and electron and ion beam evaporation methods. The matrix polymer or reactive resin may be any system which is compatible with the nano-particles and, if required, is able to react with the reactive groups introduced at the nano-particle surface. These may be epoxy, polyimide epoxy, liquid crystal epoxy, cyanate-ester and other low molecular weight polymers and resins with a variety of crosslinking agents.

In the case of non-discrete organic-inorganic hybrids it is possible to use sol-gel chemistry to form a continuous molecular alloy. In this case sol-gel chemistries involving aqueous and non-aqueous reactions may be considered.

The products of the present invention exhibit higher thermal conductivity than conventional electrically insulating materials and may be used as bonding resins in mica-glass tape constructions, as unreacted vacuum-pressure impregnation resins for conventional mica tape constructions and as stand alone materials to fulfill electrical insulation applications in rotating and static electrical power plant and in both high and low voltage electrical and electronic equipment, components and products. Products of the present invention may be combined with each other, as well as HTC-material, and other materials, of the prior art.

Micro and nano HTC particles may be selected on their ability to self aggregate into desired structural forms such as filaments and branched dendrites. Particles may be selected for their ability to self-assemble naturally, though this process may also be modified by external forces such as an electric field, magnetic field, sonics, ultra-sonics, pH control, use of surfactants and other methods to affect a change to the particle surface charge state, including charge distribution, of the particle. In a particular embodiment, particles such as boron nitride, aluminum nitride, diamond are made to self assemble into desired forms. In this manner, the desired aggregation structures can be made from highly thermally conductive materials at the outset or assembled during incorporation into the host matrix.

In many embodiments, the size and shape of the HTC-materials are varied within the same use. Ranges of size and shape are used in the same product. A variety of long and shorter variable aspect ratio HTC-materials will enhance the thermal conductivity of a resin matrix, as well as potentially provide enhanced physical properties and performance. One aspect that should be observed, however, is that the particle length does not get so long as to cause bridging between layers of substrate/insulation. Also, a variety of shapes and length will improve the percolation stability of the HTC-materials by providing a more uniform volume filing and packing density, resulting in a more homogeneous matrix. When mixing size and shapes, in one embodiment the longer particles are more rod-shaped, while the smaller particles are more spheroidal, platelet or discoid and even cuboids. For example a resin containing HTC-materials could contain about 55-65% by volume 10-50 nm diameter spheroids and about 15-25% by volume 10-50 μm length rods, with 10-30% volume resin.

In another embodiment the present invention provides for new electrical insulation materials based on organic-inorganic composites. The thermal conductivity is optimized without detrimentally affecting other insulation properties such as dielectric properties (permittivity and dielectric loss), electrical conductivity, electric strength and voltage endurance, thermal stability, tensile modulus, flexural modulus, impact strength and thermal endurance in addition to other factors such as viscoelastic characteristics and coefficient of thermal expansion, and overall insulation. Organic and inorganic phases are constructed and are selected to achieve an appropriate balance of properties and performance.

In one embodiment the surface coating of nano, meso and micro inorganic fillers having the desired shape and size distribution and the selected surface characteristics and bulk filler properties are complimentary to each other. This enables the percolation structure of the filler phase in the organic host and the interconnection properties to be controlled independently while maintaining required bulk properties. In addition organic and inorganic coatings, as singular or secondary coatings may be used to ensure compatibilisation of the particle surfaces with the organic matrix and allow chemical reactions to occur with the host organic matrix.

In regards to shape, the present invention utilizes individual particle shapes tending towards natural rods and platelets for enhanced percolation, with rods being the most preferred embodiment including synthetically processed materials in addition to those naturally formed. A rod is defined as a particle with a mean aspect ratio of approximately 5 or greater, with particular embodiments of 10 or greater, though with more particular embodiments of no greater than 100. In one embodiment, the axial length of the rods is approximately in the range 10 nm to 100 microns. Smaller rods will percolate a resin matrix better, and have less adverse effect on the viscosity of the resin.

Many micro and nano particles form spheroidal and discoid shapes, which have reduced ability to distribute evenly under certain conditions and so may lead to aggregated filamentary structures that reduce the concentration at which percolation occurs. By increasing the percolation, the thermal properties of the resin can be increased, or alternately, the amount of HTC material that needs to be added to the resin can be reduced. Also, the enhanced percolation results in a more even distribution of the HTC materials within the resin rather than agglomeration which is to be avoided, creating a more homogenous product that is less likely to have undesired interfaces, incomplete particle wetting and micro-void formation. Likewise aggregated filamentary or dendritic structures, rather than globular (dense) aggregates or agglomerates, formed from higher aspect ratio particles confer enhanced thermal conductivity.

Additionally, fluid flow fields and electric and magnetic fields can be applied to the HTC materials to distribute and structurally organize them inside of the epoxy resin. By using alternating or static electric fields, the rod and platelet shapes can be aligned on a micro-scale. This creates a material that has different thermal properties in different directions. The creation of an electric field may be accomplished by a variety of techniques known in the art, such as by attaching electrodes across an insulated electrical conductor or by use of a conductor in the centre of a material or the insulation system.

Organic surface coatings, and inorganic surface coatings such as, metal-oxide, -nitride, -carbide and mixed systems may be generated which, when combined with the selected particle size and shape distribution, provide a defined percolation structure with control of the bulk thermal and electrical conductivity of the insulation system while the particle permittivity may be chosen to control the permittivity of the system. Another type of coating is micro-particulate and- nano-particulate diamond coatings and of natural or synthetic origin. In poly-crystalline and mono-crystalline nano-particulate form, the particles may associate with the surface of a carrier particle, eg silica. Silica by itself is not a strong thermally conducting material, but with the addition of a surface coating it becomes more of a higher thermal conductivity material. Silica and other such materials, however, have beneficial properties such as being readily formed into rod-shaped particles, as discussed above. In this manner, various HTC properties can be combined into one product. These coatings may also have application to mica tape structures, including both the mica and the glass components, with or without resin impregnation.

Reactive surface functional groups may be formed from surface groups intrinsic to the inorganic coating or may be achieved by applying additional organic coatings both of which may include hydroxyl, carboxylic, amine, epoxide, silane, vinyl and other groups which will be available for chemical reaction with the host organic matrix. These single or multiple surface coatings and the surface functional groups may be applied using wet chemical methods, non-equilibrium plasma methods including plasma polymerization and chemical vapour and physical vapour deposition, laser beams, sputter ion plating and electron and ion beam evaporation methods.

In another embodiment the present invention provides for new electrical insulation systems based on organic-inorganic composites. The interface between the various inorganic and organic components is made to be chemically and physically intimate to ensure a high degree of physical continuity between the different phases and to provide interfaces which are mechanically strong and not prone to failure during the operation of the electrical insulation system in service in both high and low voltage applications. Such materials have applications in high voltage and low voltage electrical insulation situations where enhanced interfacial integrity would confer advantage in terms of enhanced power rating, higher voltage stressing of the insulation systems, reduced insulation thickness and would achieve high heat transfer.

A particular embodiment uses a variety of surface treatments, nano, meso and micro inorganic fillers, so as to introduce a variety of surface functional groups which are capable of compatibilizing the inorganic surface with respect to the organic matrix or to allow chemical reactions to occur with the host organic matrix. These surface functional groups may include hydroxyl, carboxylic, amine, epoxide, silane or vinyl groups which will be available for chemical reaction with the host organic matrix. These functional groups may be applied using wet chemical methods, non-equilibrium plasma methods, chemical vapour and physical vapour deposition, laser beams, sputter ion plating and electron and ion beam evaporation methods.

In many embodiments, the surface treated materials may be used in bonding resins in mica-glass tape constructions, in unreacted vacuum-pressure impregnation (GVPI &VPI) resins for conventional mica tape constructions and in stand alone electrical insulation coatings or bulk materials to fulfill either electrically insulating or conducting applications in rotating and static electrical power plant and in both high and low voltage electrical equipment, components and products. Also, all chemical reactions should be the result of addition, and not condensation reactions so as to avoid volatile by-products.

Improvements in epoxy resins have recently been made by using liquid crystal polymers. By mixing an epoxy resin with a liquid crystal monomer or by incorporating a liquid crystalline mesogen into an epoxy resin molecule such as DGEBA, a liquid crystal thermoset (LCT) epoxy resin is produced that contains polymers or monomers that can be cross-linked to form ordered networks having significantly improved mechanical properties. See U.S. Pat. No. 5,904,984, which is incorporated herein by reference. A further benefit of LCTs is that they also have improved thermal conductivity over standard epoxy resins, and lower coefficient of thermal expansion (CTE) values as well.

What makes LCT epoxy resins even more appealing is that they are also better able to conduct heat than a standard epoxy resin. U.S. Pat. No. 6,261,481, which is incorporated herein by reference, teaches that LCT epoxy resins can be produced with a thermal conductivity greater than that of conventional epoxy resins. For example, a standard Bisphenol A epoxy is shown to have thermal conductivity values of 0.18 to 0.24 wafts per meter degree Kelvin (W/mK) in both the transverse (plane) and thickness direction. By contrast, an LCT epoxy resin is shown to have a thermal conductivity value, when used in practical applications, of no more than 0.4 W/mK in the transverse direction and up to 0.9 W/mK in the thickness direction.

As used in reference to HTC materials being applied to paper, the term substrate refers to the host material that the insulating paper is formed from, while paper matrix refers to the more complete paper component made out of the substrate. These two terms may be used somewhat interchangeable when discussing this embodiment of the present invention. The increase of thermal conductivity should be accomplished without significantly impairing the electrical properties, such as dissipation factor, or the physical properties of the substrate, such as tensile strength and cohesive properties. The physical properties can even be improved in some embodiments, such as with surface coatings. In addition, in some embodiments the electrical resistivity of the host paper matrix can also be enhanced by the addition of HTC materials.

In addition to the standard mica (Muscovite,Phlogopite) that is typically used for electrical insulation there is also Biotite mica as well as several other Mica-like Alumino-Silicate materials such as Kaolinite, Halloysite, Montmorillonite and Chlorite. Montmorillonite has lattices in its structure which can be readily intercalated with HTC materials such as metal cations, organic compounds and monomers and polymers to give high dielectric strength composites.

Insulating papers are just one type of porous media that may be impregnated with the resin of the present invention. Many other materials and components made therefrom, in many industries, some of which are mentioned below, can use different types of porous media to impregnate the resin into. By way of examples there are glass fiber matrices or fabric, and polymer matrices or fabric, where the fabric might typically be cloth, matt, or felt. Circuit boards, which are glass fabric laminate, with planar lamination, will be one product which will benefit from the use of resins of the present invention.

Types of resin impregnation used with stator coils are known as VPI and GVPI. Tape is wrapped around the coil and then impregnated with low viscosity liquid insulation resin by vacuum-pressure impregnation (VPI). That process consists of evacuating a chamber containing the coil in order to remove air and moisture trapped in the mica tape, then introducing the insulation resin under pressure to impregnate the mica tape completely with resin thus eliminating voids, producing resinous insulation in a mica host. A compression of about 20% is particular to the VPI process in some embodiments. After this is completed, the coils are heated to cure the resin. The resin may contain an accelerator or the tape may have one in it. A variation of this, global VPI (GVPI) involves the process where dry insulated coils are wound, and then the whole stator is vacuum pressure impregnated rather than the individual coils. In the GVPI process, the coils are compressed prior to impregnation with the resin since the dry coils are inserted into their final position prior to impregnation. Although various compression methods have been discussed above, it is also possible to use the VPI/GVPI impregnating process for the actual compression stage of the present invention.

In one embodiment the present invention provides for a high thermal conductivity resin that comprises a host resin matrix containing a high thermal conductivity filler. The high thermal conductivity filler forms a continuous organic-inorganic composite with the host resin matrix, and the fillers have an aspect ratio of between 3-100. The fillers are substantially evenly distributed through the host resin matrix, and are aligned in essentially the same direction. In some embodiments the resins are highly structured resin types.

In a related embodiments, the fillers are from 1-1000 nm in length, and may be composed of materials such as diamond, Al2O3, AlN, MgO, ZnO, BeO, BN, Si3N4, SiC and SiO2. The fillers may have non-high thermal conductivity coatings, or they may be comprised on non-high thermal conductivity cores with HTC coatings.

In another embodiment the present invention provides for a method for making a thermal conductivity resin that comprises impregnating a host resin matrix with a high thermal conductivity filler and distributing the high thermal conductivity filler evenly through the resin matrix. Then aligning at least 75% of the high thermal conductivity fillers within 15 degrees of a common direction and curing or semi-curing the resin matrix. The high thermal conductivity fillers have an aspect ratio of between 3-100. In some embodiments, the filler forms a continuous organic-inorganic composite with the host resin matrix. In particular embodiments host resin matrix comprises a highly structured resin that is aligned uniformly with the high thermal conductivity filler.

In one embodiment the alignment is done by the self-alignment and aggregation of the high thermal conductivity fillers, and in another the alignment is done by the application of an external field. Examples of the external field include mechanical, electric, magnetic, sonic and ultrasonic. In some cases the fillers are first surface coated with field responsive materials, and in other cases field responsive fillers are coated with high thermal conductivity materials.

In yet another embodiment the present invention provides for a high thermal conductivity resin that comprises a host resin matrix and a high thermal conductivity filler. The high thermal conductivity filler forms a continuous organic-inorganic composite with the host resin matrix, and the high thermal conductivity fillers have an aspect ratio of between 3-100. The fillers are substantially evenly distributed through the host resin matrix, and the high thermal conductivity fillers form substructures within the host resin matrix. The substructures may be at least one of columns, layers and super lattices.

In a related embodiment, the high thermal conductivity fillers are at least one of oxides, nitrides and carbides. In another related embodiment the high thermal conductivity fillers contain at least one of metallic and organo-metallic compounds that are capable of responding to an external field.

In still another embodiment the present invention provides for a porous media impregnated with a high thermal conductivity resin that comprises a porous media and a high thermal conductivity material loaded resin. The high thermal conductivity material comprises 5-60% by volume of the resin, and the high thermal conductivity materials have aspect ratios of 10-50 and are aligned within the porous media in essential the same direction.

Although the present invention has been discussed primarily in use with electrical industries, the invention is equally applicable in other areas. Industries that need to increase heat transference would equally benefit from the present invention. For example, the energy, chemical, process and manufacturing industries, inclusive of oil and gas, and the automotive and aerospace industries. Other focuses of the present invention include power electronics, conventional electronics, and integrated circuits where the increasing requirement for enhanced density of components leads to the need to remove heat efficiently in local and large areas. Also, while specific embodiments of the invention have been described in detail, it will be appreciated by those skilled in the art that various modifications and alternatives to those details could be developed in light of the overall teachings of the disclosure. Accordingly, the particular arrangements disclosed are meant to be illustrative only and not limiting as to the scope of the inventions which, is to be given the full breadth of the claims appended and any and all equivalents thereof.