Patent Publication Number: US-2023135684-A1

Title: Composite material

Description:
TECHNICAL FIELD 
     The present invention relates to a composite material. 
     BACKGROUND ART 
     Efforts have been made to increase the heat conductivity of materials, such as foam materials, having a plurality of voids. 
     For example, Patent Literature 1 discloses a composite material including: scaly fillers formed of an inorganic material; and a binding resin formed of a thermosetting resin binding the fillers. This composite material is a foam material in which a plurality of voids are dispersed, and the fillers accumulate on inner walls of the voids such that flat surfaces of the fillers overlap each other (claim  1  and  FIG.  1   ). According to Patent Literature 1, the flat surfaces of the fillers are less likely to overlap each other when a ratio, namely, an aspect ratio, of an average length of the flat surfaces of the fillers to a thickness of the filler is less than 50. 
     A composite material including an inorganic filler but having excellent thermal insulation properties was also proposed. Patent Literature 2 discloses a polyurethane foam obtained from a composition including a polyol, a blowing agent, a layered clay mineral, etc. This composite material has a high closed cell rate, and the layered clay mineral which is an inorganic filler is uniformly dispersed therein. 
     CITATION LIST 
     Patent Literature 
     
         
         Patent Literature 1: JP 2018-109101 A 
         Patent Literature 2: JP 2009-191171 A 
       
    
     SUMMARY OF INVENTION 
     Technical Problem 
     A composite material obtained by a conventional foaming technique needs to be improved as it is difficult to control placement of a filler. The present invention aims to provide a new composite material unobtainable by a conventional foaming technique. 
     Solution to Problem 
     The present invention provides a composite material including 
     a solid portion including inorganic particles and a resin, wherein 
     the composite material has a porous structure including a plurality of voids surrounded by the solid portion, 
     a value P 1  determined by the following equation (1) is 6 or more: 
         P   1 =( a  heat conductivity[ W /( m·K )] of the composite material/an amount[volume %] of the inorganic particles)×100  (1),
 
     where the heat conductivity is a value measured for one test specimen in a symmetric configuration according to an American Society for Testing and Materials (ASTM) standard D5470-01. 
     Advantageous Effects of Invention 
     The present invention can provide a composite material suitable for achieving a high heat conductivity by a small amount of inorganic particles. 
    
    
     
       BRIEF DESCRIPTION OF DRAWINGS 
         FIG.  1    is a cross-sectional view schematically showing an example of a composite material according to the present embodiment. 
         FIG.  2    is a cross-sectional view schematically showing another example of the composite material according to the present embodiment. 
         FIG.  3    illustrates a measurement position in the composite material according to the present embodiment measured by energy dispersive X-ray spectroscopy using an ultra-high-resolution field-emission scanning electron microscope. 
         FIG.  4    shows the results of optical microscope observation of a cross-section of a composite material according to Sample 1. 
     
    
    
     DESCRIPTION OF EMBODIMENTS 
     Embodiments of the present invention will be described hereinafter with reference to the drawings. The following description describes examples of the present invention, and the present invention is not limited to the following embodiments. 
     As shown in  FIG.  1   , a composite material  1  according to the present embodiment includes a solid portion  10 . The solid portion  10  includes inorganic particles  20  and a resin  30 . For example, the composite material  1  has a porous structure including a plurality of voids  40  in contact with each other via the inorganic particle  20  or directly without the inorganic particle  20 . For example, at least a portion of the inorganic particles  20  is present on a wall surface of the solid portion  10 , the wall surface facing the void  40 . Heat transmission paths  5  and  6  stretch, for example, through the plurality of voids  40 , that is, along the plurality of voids  40 . The heat transmission paths  5  and  6  are formed of the plurality of inorganic particles  20  arranged continuously, i.e., in contact with each other or close to each other. The heat transmission paths  5  and  6  stretch, for example, without extending through the inside of the solid portion  10 , more specifically, along the wall surface of the solid portion  10 . For example, some of the heat transmission paths  5  stretch from a surface  1   a  of the composite material  1  to a surface  1   b  on the opposite side thereof. 
     In the composite material  1 , a value P 1  determined by the following equation (1) is 6 or more. In the equation (1), a heat conductivity is a value measured for one test specimen in a symmetric configuration according to an American Society for Testing and Materials (ASTM) standard D5470-01. 
         P   1 =(the heat conductivity[ W /( m·K )] of the composite material 1/an amount[volume %] of the inorganic particles 20)×100  Equation (1)
 
     The value P 1  may be 7.5 or more, 10 or more, 12 or more, or 14 or more. The upper limit of the value P 1  is not limited to a particular value. The upper limit of the value P 1  is, for example, 50 and may be 40, 30, or 25. 
     The composite material  1  can exhibit a high heat conductivity relative to the amount of the inorganic particles  20 . The heat conductivity of the composite material  1  is, for example, 0.5 W/(m·K) or more, and can be preferably 0.55 W/(m·K) or more, more preferably 0.6 W/(m·K) or more, and, in some cases, 0.7 W/(m·K) or more. The upper limit of the heat conductivity is not limited to a particular value. The upper limit of the heat conductivity may be, for example, 2.1 W/(m·K), 2.0 W/(m·K), or 1.9 W/(m·K). The heat conductivity of the composite material  1  is a value measured for one test specimen in a symmetric configuration according to the American Society for Testing and Materials (ASTM) standard D5470-01 (steady state longitudinal heat flow method). 
     To form, as in the technique described in Patent Literature 1, a heat transmission path via a route including voids spaced from each other, inorganic particles need to connect outer surfaces of the voids spaced from each other in the solid portion  10 . Therefore, the aspect ratio of the inorganic particle needs to be set high. On the other hand, according to the embodiment shown in  FIG.  1   , even when the aspect ratio of the inorganic particle  20  is not high, the heat transmission paths  5  and  6  are formed and the composite material  1  can exhibit high heat conduction performance. The composite material  1  does not need to include the inorganic particle  20  by which the voids  40  adjacent to each other are connected and which is, between the voids  40  adjacent to each other, surrounded by the solid portion  10 . 
     It should be noted that all heat transmission paths not necessarily appear in a particular cross-section as shown in  FIG.  1    and that all portions of a particular heat transmission path not necessarily appear in a particular cross-section as shown in  FIG.  1   . For example, in  FIG.  1   , the heat transmission path  6  does not seem to stretch to the surface  1   b . Actually, however, the heat transmission path  6  stretches via the inorganic particles not appearing in this cross-section and reaches the surface  1   b . Similarly, it is impossible to confirm in a particular cross-section that every void is in contact with another void. For example, a void  50  seems to be isolated in  FIG.  1   . Actually, however, the void  50  is in contact with another void adjacent thereto in a thickness direction of the page. 
     However, not all heat transmission paths need to stretch from the surface  1   a  to the surface  1   b . Moreover, not every void included in the porous structure needs to be in contact with another void directly or via the inorganic particle. 
     The resin  30  is not present at connecting portions  41  and  43 . The resin  30  and the inorganic particle  20  are not present at the connecting portion  41 . The voids  40  directly in contact with each other at the connecting portion  41  communicate to each other to form one space. The voids  40  in contact with each other at the connecting portion  43  at which inorganic particles  21  are present may communicate to each other via a small gap between the inorganic particles  21  to form one space or may be present as spaces separated from each other. However, the voids  40  that seem to be in contact with each other via the inorganic particle  21  in  FIG.  1    may be directly in contact with and communicate to each other in a cross-section different from the one in  FIG.  1   . 
     As shown in  FIG.  2   , a particle  60  may be present inside the void  40 . The particle  60  is typically a resin particle. The resin particle may be a later-described first resin. The particle  60  can be the first resin shrunk by a heat treatment. The resin particle before shrinking may be in a shape corresponding to the void  40 . The resin occupying the void may be removed as shown in  FIG.  1   , or may deform and remain as shown in  FIG.  2   . In the latter case, the particle  60  may be in contact with the inorganic particle  20 . In a particular cross-section, presence of the particle  60  cannot be confirmed inside of the void  50 ; however, in another cross-section, presence of the particle  60  may be confirmed inside the same void  50 . In the embodiment shown in  FIG.  2   , the particle  60  is present in at least some of the voids  40  and  50 , the particle  60  being smaller than the at least some of the voids  40  and  50 . 
     The inorganic particles  20  around the void  40  may be exposed to the void  40  or does not need to be exposed to the void  40 . A surface layer including no inorganic particles  20  may be present between the wall surface of the void  40  and the inorganic particles  20  that are present continuously along the periphery of the void  40 , i.e., in contact with each other or close to each other. 
     The material of the inorganic particle  20  is not limited to a particular material as long as, for example, the inorganic particle  20  has a higher heat conductivity than the heat conductivity of the resin  30 . Examples of the material of the inorganic particle  20  include hexagonal boron nitride (h-BN), alumina, crystalline silica, amorphous silica, aluminum nitride, magnesium oxide, carbon fibers, silver, copper, aluminum, silicon carbide, graphite, zinc oxide, silicon nitride, silicon carbide, cubic boron nitride (c-BN), beryllia, and diamond. The shape of the inorganic particle  20  is not limited to a particular shape. Examples of the shape of the inorganic particle  20  include sphere-like, rod-like (including short-fiber), scaly, and granular shapes. The “granular” shape refers to, for example, the shape of the plurality of inorganic particles  20  aggregated using a binder or a sintered body of the plurality of inorganic particles  20 . 
     The aspect ratio of the inorganic particle  20  is not limited to a particular value. The aspect ratio of the inorganic particle  20  may be less than 50, 40 or less, or even 30 or less. The aspect ratio of the inorganic particle  20  may be 1 or more, or may be a greater value, e.g., 2 or more or even 3 or more. The aspect ratio is defined as a ratio (maximum diameter/minimum diameter) of a maximum diameter of the particle to a minimum diameter of the particle, unless otherwise specified. Herein, the minimum diameter is defined as a shortest line segment passing through a midpoint of a line segment defined as the maximum diameter. 
     The average particle diameter of the inorganic particles  20  is not limited to a particular value. The average particle diameter of the inorganic particles  20  is, for example, 0.05 μm to 100 μm, and may be 0.1 μm to 50 μm, 0.1 μm to 30 μm, or 0.5 to 10 μm. The average particle diameter can be determined, for example, by laser diffraction-scattering. The average particle diameter is, for example, a 50% cumulative value (median diameter) d 50  determined from a particle size distribution curve, in which a frequency is represented by a volume-based fraction, obtained using a particle size distribution analyzer (Microtrac MT3300EX11) manufactured by MicrotracBEL Corp. 
     The shape of the inorganic particle  20  can be determined, for example, by observation using, for example, a scanning electron microscope (SEM). For example, the inorganic particle  20  is considered to have a sphere-like shape when the aspect ratio (maximum diameter/minimum diameter) thereof is 1.0 or more and less than 1.7, particularly 1.0 or more and 1.5 or less, or even 1.0 or more and 1.3 or less and at least a portion of an outline of the inorganic particle  20  observed, particularly, substantially the entire outline of the inorganic particle  20  observed, is a curve. 
     The “scaly” shape refers to the shape of a plate having a pair of principal surfaces and a lateral surface. The term “principal surface” of the inorganic particle  20  refers to a face thereof having the largest area, and is typically a substantially flat face. When the inorganic particle  20  has a scaly shape, the aspect ratio is defined as a ratio of an average dimension of the principal surfaces to the average thickness, instead of the above definition. The thickness of the scaly inorganic particle  20  refers to the distance between the pair of principal surfaces. The average thickness can be determined by measuring thicknesses of any 50 inorganic particles  20  using a SEM and calculating the average of the thicknesses. A value of d 50  measured using the above particle size distribution analyzer can be used as the average dimension of the principal surfaces. The aspect ratio of the scaly inorganic particle  20  may be 1.5 or more, 1.7 or more, or even 5 or more. 
     Examples of the rod-like shape include stick-like shapes such as stick-like, columnar, tree-like, needle-like, and conical shapes. The aspect ratio of the rod-like inorganic particle  20  may be 1.5 or more, 1.7 or more, or even 5 or more. Examples of the upper limit of the aspect ratio are as described above regardless of the shape of the inorganic particle  20 . 
     When the inorganic particles  20  have a sphere-like shape, the average particle diameter thereof is, for example, 0.1 μm to 50 μm, preferably 0.1 μm to 10 μm, and more preferably 0.5 μm to 5 μm. When the inorganic particle  20  has a rod-like shape, a length of a minor axis of the inorganic particle  20  is, for example, 0.01 μm to 10 μm and preferably 0.05 μm to 1 μm. When the inorganic particle  20  has a rod-like shape, a length of a major axis of the inorganic particle  20  is, for example, 0.1 μm to 20 μm and preferably 0.5 μm to 10 μm. When the inorganic particles  20  have a scaly shape, the average dimension of the principal surfaces of the inorganic particles  20  is, for example, 0.1 μm to 20 μm and preferably 0.5 μm to 15 μm. When the inorganic particle  20  has a scaly shape, the thickness of the inorganic particle  20  is, for example, 0.05 μm to 1 μm and preferably 0.08 μm to 0.5 μm. When the inorganic particle  20  has a rod-like shape, the minimum diameter (commonly the length of the minor axis) of the inorganic particle  20  is, for example, 0.01 μm to 10 μm and preferably 0.05 μm to 1 μm. When the inorganic particle  20  has a rod-like shape, the maximum diameter (commonly the length of the major axis) of the inorganic particle  20  is, for example, 0.1 μm to 20 μm and preferably 0.5 μm to 10 μm. When the size of the inorganic particle  20  is in these ranges, the inorganic particles  20  are likely to be placed along the void  40 , the heat transmission path  5  stretching through the plurality of voids  40  can be reliably formed. When the inorganic particles  20  have a granular shape, the average particle diameter thereof is, for example, 10 μm to 100 μm, and preferably 20 μm to 60 μm. 
     The amount of the inorganic particles  20  in the composite material  1  is not limited to a particular value. The amount of the inorganic particles  20  in the composite material  1  is, for example, 10 mass % to 80 mass %, preferably 10 mass % to 70 mass %, and more preferably 10 mass % to 55 mass %. The amount of the inorganic particles  20  in the composite material  1  is, for example, 1 volume % to 50 volume %, preferably 2 volume % to 45 volume %, more preferably 5 volume % to 40 volume %, and particularly preferably 5 volume % to 30 volume %. The composite material  1  can exhibit higher heat conduction performance and an appropriate rigidity by appropriate adjustment of the amount of the inorganic particles  20 . 
     The amount [mass %] of the inorganic particles  20  in the composite material  1  can be determined by removing a material other than the inorganic particle  20  from the composite material  1  by, for example, burning. For accurate measurement, the amount[mass %] of the inorganic particles may be calculated by element analysis. Specifically, an acid is added to the composite material  1 , and a microwave is applied to the acid and the composite material  1  for acid decomposition of the composite material  1  under pressure. For example, hydrofluoric acid, concentrated sulfuric acid, concentrated hydrochloric acid, aqua regia, or the like can be used as the acid. Element analysis is performed by an inductively coupled plasma atomic emission spectroscopy (ICP-AES) for a solution obtained by the acid decomposition under pressure. The amount [mass %] of the inorganic particles  20  can be determined on the basis of the analysis result. 
     The amount [volume %] of the inorganic particles  20  in the composite material  1  can be determined from the mass and density of the inorganic particles  20  included in the composite material  1  and the volume and void ratio of the composite material  1 . Specifically, a volume A of the inorganic particles  20  in the composite material  1  is calculated from the mass and density of the inorganic particles  20 . Separately, a volume B of the composite material  1  is calculated on the basis of the void ratio of the composite material  1 , the volume B not including the volume of the voids  40 . The amount [volume %] of the inorganic particles  20  can be determined by (A/B)×100. The method for calculating the void ratio will be later described. 
     The density of the inorganic particles  20  can be determined according to Japanese Industrial Standards (JIS) R 1628: 1997 or JIS Z 2504: 2012 for the inorganic particles  20  left over after burning an organic material by heating the composite material  1  in an electric furnace at high temperatures. 
     At least a portion of the inorganic particles  20  is present on the wall surface of the solid portion  10 , the wall surface facing the voids  40 . Other portions  21  and  22  of the inorganic particles  20  may be present at the connecting portion  43  between the voids  40 . On the wall surface of the solid portion  10 , a portion  23  of the inorganic particles  20  may be stacked on another inorganic particle  20 . At least a portion of the inorganic particles  20  is in contact with or very close to the inorganic particle adjacent thereto and form a portion of the heat transmission paths  5  and  6 . However, another portion  24  of the inorganic particles  20  may be surrounded by the resin  30 . In other words, the solid portion  10  can include the inorganic particle  24  not in contact with the void  40 . 
     Substantially all the inorganic particles  20  may each be present on the wall surface of the solid portion  10  or at the connecting portion  41  or  43  between the voids  40 . Herein, the term “substantially all” means 70 mass % or more, even 80 mass % or more, and particularly 90 mass % or more. In this embodiment, a proportion of the inorganic particles contributing to improvement of the heat conductivity is higher. Distribution of the inorganic particles  20  inside the solid portion  10  can be analyzed, for example, using an ultra-high-resolution field-emission scanning electron microscope by energy dispersive X-ray spectroscopy. 
     A portion of the wall surface of the solid portion  10  may be formed of a material, typically the resin  30 , other than the inorganic particle  20 , the wall surface facing the void  40 . The resin  30  is, for example, a later-described second resin. 
     The resin  30  of the solid portion  10  is, for example, a crosslinking polymer, and specifically a thermosetting resin. Examples of the thermosetting resin include phenolic resins, urea resins, melamine resins, diallyl phthalate resins, polyester resins, epoxy resins, aniline resins, silicone resins, furan resins, polyurethane resins, alkylbenzene resins, guanamine resins, xylene resins, and imide resins. A curing temperature of the resin is, for example, 25° C. to 160° C. 
     Outer shapes of the voids  40  and  50  may be in a sphere-like shape, and may be substantially spherical. Herein, the term “substantially spherical” means that a ratio (maximum diameter/minimum diameter) of the maximum diameter to the minimum diameter is 1.0 to 1.5, particularly 1.0 to 1.3. However, the outer shapes of the voids  40  and  50  are not limited to particular shapes. The outer shapes of the voids  40  and  50  may be a rod-like or polyhedral shape, or may be an ellipsoidal shape having too large a ratio of the maximum diameter to the minimum diameter to call the shape a sphere-like shape. 50% or more or even 80% or more of the voids  40  and  50  may have a sphere-like shape. It is difficult to form voids having shapes as uniform as the above by a foaming technique, by which irregularly shaped voids are formed. 
     The average diameter of the voids  40  is not limited to a particular value. The average diameter of the voids  40  is, for example, 50 μm to 5000 μm, preferably 100 μm to 2000 μm, and more preferably 300 μm to 1500 μm. Herein, the “average diameter” of the voids  40  refers to the average of diameters thereof determined by observation of a cross-section of the composite material  1  using a SEM. Specifically, any one hundred voids  40  that are each observable entirely are measured for their maximum and minimum diameters, the average of the maximum and minimum diameters of each void is defined as the diameter of the void, and the average of the diameters of fifteen voids having the largest to fifteenth largest diameters is defined as the “average diameter”. However, depending on the size of the voids  40 , an optical microscope may be used instead of a SEM to measure the average diameter of the voids  40 . It should be noted that when the particle diameters of the first resins used in a later-described composite material manufacturing method are highly uniform, the particle diameters of the first resins and the average diameter of the voids of the composite material are substantially the same and any of the particle diameters of the first resins is considered the average diameter of the voids of the composite material. 
     In the composite material  1 , a ratio of the volume of the voids  40  to the volume of the composite material  1 , namely, the void ratio, is not limited to a particular value. The void ratio is, for example, 10 volume % to 60 volume %, preferably 15 volume % to 50 volume %, and more preferably 20 volume % to 45 volume %. 
     The void ratio can be determined by observing a cross-section of the composite material  1  using a SEM, calculating a ratio of the total area of the voids  40  to the total area observed, and averaging thus-obtained ratios in 10 images of different cross-sections. However, the void ratio may be determined in the following manner only when the manufacturing process is known. From the mass of the later-described first resin and the mass of the composite particle in which the inorganic particles  20  are placed on a surface of the first resin, the mass of the inorganic particles  20  included in the composite particle is calculated. Separately, the amount [mass %] of the inorganic particles  20  in the composite material  1  is calculated by inorganic element analysis. The mass of the inorganic particles  20  in the composite material  1  is calculated from the amount [mass %] of the inorganic particles  20  and the mass of the composite material  1 . The number of composite particles used to manufacture the composite material  1  is calculated from the mass of the inorganic particles  20  in the composite material  1  and the mass of the inorganic particles  20  included in the composite particle. The volume of the void  40  is calculated from the average diameter of the voids  40 . The total volume of the voids  40  in the composite material  1  is determined by multiplying the volume of the void  40  by the number of the composite particles. The total volume of the voids  40  in the composite material  1  is divided by the volume of the composite material  1  to calculate the void ratio. 
     The plurality of voids  40  may have substantially similar outer shapes. Herein, the term “substantially similar” means that on a number basis, 80% or more, particularly 90% or more, of the voids  40  have the same type of a geometric shape, for example, a sphere-like or regular polyhedron shape. The outer shapes of the substantially similar voids  40  preferably have sphere-like shapes. The outer shapes thereof may be substantially spherical. A plurality of voids formed by foaming can also come in contact with each other as a result of expansion. However, in this case, an internal pressure caused by foaming commonly acts on a connecting portion between the voids, greatly deforming a vicinity of the connecting portion. Therefore, it is virtually impossible to form a plurality of voids in contact with each other and having substantially similar outer shapes by a foaming technique. 
     The porous structure may have a through hole extending from one principal surface to the other principal surface of the composite material  1 . When the composite material  1  has a plate shape, the void provided on one principal surface of the composite material  1  may communicate to a space facing the other principal surface of the composite material  1 . The void provided on one principal surface of the composite material  1  may communicate to a space in contact with a lateral face adjacent to the one principal surface of the composite material  1 . With such structural features, the composite material  1  can have both heat conductivity and air permeability. Herein, the term “principal surface” of the composite material  1  refers to a surface thereof having the largest area. 
     The plurality of voids  40  may be locally in contact with each other. In this case, the strength of the composite material  1  is unlikely to be decreased even when the void ratio is increased. The diameter of a communicating portion allowing communication between the voids at the connecting portion  41  may be 25% or less, 20% or less, or even 15% or less of the average diameter of the voids  40 . The diameter of the communicating portion can be measured by a SEM or X-ray CT, as for the average diameter. Since the inorganic particle  21  separates the voids  40  at the connecting portion  43 , there is no communicating portion at the connecting portion  43 . 
     In the composite material  1  according to the present embodiment, for example, a value P 0  determined by the following equation (2) may be 30 or more. In this case, the composite material  1  whose physical properties and functions, such as elastic modulus, hardness, shock-absorbing properties, and anti-vibration properties, are unlikely to vary can be obtained. Moreover, in this case, the amount of the inorganic particles  20  used can be reduced and thus the manufacturing cost of the composite material  1  can be reduced. 
         P   0 =(the average diameter[μ m ] of the voids 40/the average particle diameter[μ m ] of the inorganic particles 20)×(the void ratio[volume %]/100)  Equation (2)
 
     The upper limit of the value P 0  is not limited to a particular value. The upper limit of the value P 0  is, for example, 1000, preferably 700, more preferably 500, and particularly preferably 450. 
     As is obvious from the above description, the composite material  1  may be a non-foam body. Conventional foam bodies as described in Patent Literature 1 cannot have characteristic structures as shown in  FIGS.  1  and  2   , namely, structures in which placement of the inorganic particles  20  is controlled delicately and precisely. 
     An example of a method for determining herein a measurement region for determining elemental composition in a particular region of the composite material  1  will be described with reference to  FIG.  3   . First, the void  40  of the composite material  1  is observed using a SEM. The maximum diameter of the void  40  observed using the SEM was measured, and a line segment A having a length L of the maximum diameter is defined. Next, a line segment B passing through a midpoint of the line segment A to be perpendicular to the line segment A is defined, the line segment B having a length L′ from one end of the void  40  to the other end of the void  40 . Furthermore, a rectangle C having a center of gravity at the midpoint of the line segment A is defined, the rectangle C having a first side and a second side adjacent to the first side, the first side being parallel to the line segment A and having a length (2 L in a direction parallel to the line segment A) twice as long as the line segment A, the second side being parallel to the line segment B and having a length (2 L′ in a direction parallel to the line segment B) twice as long as the line segment B. A region determined by removing a void portion from the rectangle C is defined as a measurement region. 
     This measurement region is divided into a plurality of regions D each defined by a 50-μm square. For each of the plurality of regions D, a proportion of an atom included in the region D is analyzed. For example, energy dispersive X-ray spectroscopy using an ultra-high-resolution field-emission scanning electron microscope is employed for the analysis. 
     As a result of the above analysis of the plurality of regions D, a largest proportion [atomic %] of the atom (e.g., B) included in the inorganic particle(s) is defined as Y, the largest proportion being determined for one of the plurality of regions D. Similarly, a smallest proportion [atomic %] of the atom (e.g., B) included in the inorganic particle(s) is defined as X, the smallest proportion being determined for another one of the plurality of regions D. Y/X satisfies, for example, a relation Y/X≥2. The lower limit of Y/X may be 2.2, 2.5, or, in some cases, 3.0. The upper limit of Y/X is not limited to a particular value. The upper limit of Y/X may be 10, 9.5, 9, 8, 7, or 6. When the inorganic particle is formed of a compound, the atom to be analyzed is recommended to be an element of a cation in the compound. When the inorganic particle is formed of a simple substance, the atom to be analyzed is recommended to be an element forming the simple substance. For example, when the inorganic particle is formed of boron nitride (BN), the atom to be analyzed is boron (B). When the inorganic particle is formed of alumina (Al 2 O 3 ), the atom to be analyzed is aluminum (Al). 
     The region D for which Y is determined may be a region having no additional void between the region D and the void  40 , i.e., a region adjacent to the void  40 . In the present embodiment, a value Q determined by the following equation is, for example, 65 or more. The value Q may be 68 or more or 70 or more. The maximum of the value Q is not limited to a particular value. The maximum of the value Q may be 100 or 95. 
         Q= 100× Y /( Y+X )
 
     &lt;Composite Material Manufacturing Method&gt; 
     An example of a method for manufacturing the composite material  1  according to the present embodiment will be described hereinafter. 
     The composite material  1  includes: the solid portion  10  including a second resin; and the plurality of voids  40 . The method for manufacturing the composite material  1  includes, in the following order: charging a fluid in a gap of a particle aggregate including a plurality of first resins, which are typically resin particles, the fluid including a second resin or a precursor of the second resin; and shrinking or removing the plurality of resin particles by heating the plurality of resin particles to form the plurality of voids  40 . Surfaces of the plurality of resin particles include the plurality of the inorganic particles  20 . 
     First, a mixture of the first resin and an adhesive is produced to obtain the composite particles. The adhesive is an adhesive for adhering the inorganic particles  20  to the surface of the first resin particle. The adhesive includes, for example, polyethylene glycol (PEG) and/or an emulsion. Next, the inorganic particles  20  are added to and mixed with the mixture to obtain composite particles in which the inorganic particles  20  are placed on the surface of the first resin. The mixing method is not limited to a particular method. Examples of the mixing method include mixing using a ball mill, a bead mill, a planetary mixer, an ultrasonic mixer, a homogenizer, or a planetary centrifugal mixer. 
     Next, the composite particles are put in a mold such that the composite particles are in contact with each other to form a particle aggregate. A fluid separately prepared is further added to the mold to prepare a mixed body. The fluid includes the second resin. The fluid may include the precursor of the second resin. The fluid is charged in the gap of the particle aggregate in which at least two of the plurality of composite particles are in contact with each other. The fluid is present at least on a surface of the composite particle and in a portion where the composite particles are in contact with each other. In this manner, the aggregate of the composite particles is formed in which at least two of the plurality of composite particles are in contact with each other such that a heat transmission path formed of the inorganic particles  20  in contact with each other stretches along the surfaces of the plurality of composite particles. 
     Next, bubbles are removed from the mixed body. The method for removing bubbles from the mixed body is not limited to a particular method. An example of the method is degassing under reduced pressure. Degassing under reduced pressure is performed, for example, at 25° C. to 200° C. for 1 second to 10 seconds. 
     Subsequently, the flowability of the fluid is decreased by heating the mixed body. Heating of the fluid causes progression of, for example, a reaction of generating the second resin from the precursor of the second resin or curing of the second resin, thereby decreasing the flowability of the fluid. The solid portion  10  including the second resin is generated in this manner. A precursor of the composite material can be obtained in this manner. 
     Next, the composite material  1  is produced by shrinking the first resin or removing the first resin from the precursor of the composite material. The method for shrinking the first resin or removing the first resin from the precursor of the composite material is not limited to a particular method. Examples of the method include a method in which the precursor of the composite material is heated and a method in which the precursor of the composite material is immersed in a particular solvent. These methods may be used in combination. The voids  40  are formed by shrinking or removing the first resins. In this manner, the inorganic particles  20  are “transferred” from the surface of the first resin to a surface of the second resin, and the composite material  1  in which the inorganic particles  20  are on a wall surface of the second resin can be obtained. 
     A temperature at which the precursor of the composite material is heated is not limited to a particular temperature as long as the first resin can be softened at the temperature. The temperature may be, for example, 95° C. to 130° C. or 120° C. to 160° C. 
     In the case where the precursor of the composite material is immersed in a particular solvent, the solvent is not limited to a particular solvent as long as the solvent does not dissolve the second resin but can dissolve the first resin. Examples of the solvent include toluene, ethyl acetate, methyl ethyl ketone, and acetone. 
     The first resin (resin particle) may have a hollow structure. A hollow portion in the hollow structure may be a single hollow portion, or may be formed of a plurality of hollow portions as a foamed resin bead is. When the resin particles having the hollow structure are used, a resin forming the first resins is softened by a heating treatment and the hollow portions therein disappear or shrink to form the plurality of voids  40 . However, the hollow structure of the resin particle is not essential. In the case where the precursor of the composite material is immersed in a particular solvent, it is preferable that the first resin be, for example, more easily dissolved in the solvent than the second resin. The void  40  having a desired shape is likely to be formed by this method. Examples of the material of the first resin include polystyrene (PS), polyethylene (PE), polymethyl methacrylate (PMMA), ethylene-vinyl acetate copolymer (EVA), polyethylene (PE), polyvinyl chloride (PVC), polypropylene (PP), acrylonitrile-butadiene-styrene copolymer (ABS), ethylene-propylene-diene rubber (EPDM), and thermoplastic elastomers (TPE). The resin particle may be produced by a later-described method, or a commercially-available resin particle having a particular size may be used as the resin particle. A raw material of the second resin is, for example, a crosslinking polymer, or any of the thermosetting resins shown above as examples of the resin  30 . 
     The size of the first resin is not limited to a particular one. When the first resin is spherical, the average diameter thereof is, for example, 50 μm to 5000 μm, preferably 300 μm to 2000 μm, and particularly 500 μm to 1500 μm. The composite material  1  can have an appropriate void ratio by appropriate adjustment of the size of the first resin. In addition, the composite material can have the voids of an appropriate size by appropriate adjustment of the size of the first resin. Resin particles of different sizes selected from the above sizes may be used as the first resins. That is, the plurality of first resins may have substantially similar outer shapes from each other. As a result, the plurality of voids  40  of the composite material  1  can have substantially similar outer shapes from each other. 
     According to the method for manufacturing the composite material  1  according to the present embodiment, at least a portion of the inorganic particles  20  can face the void  40 . Moreover, a heat transmission path stretching through the plurality of voids  40  can be formed of the inorganic particles  20 . 
     According to the method for manufacturing the composite material  1  according to the present embodiment, the voids  40  are formed without a foaming step. That is, the voids  40  are not formed by foaming. 
     EXAMPLES 
     Hereinafter, the present invention will be described in more detail with reference to examples. The present invention is not limited to the following examples. 
     (Production of Polystyrene Beads) 
     Into an autoclave equipped with a stirrer were added 100 parts by weight of pure water, 0.2 parts by weight of tricalcium phosphate, and 0.01 parts by weight of sodium dodecylbenzene sulfonate. Into the autoclave were added 0.15 parts by weight of benzoyl peroxide and 0.25 parts by weight of 1,1-bis(t-butylperoxy)cyclohexane as initiators to produce a liquid mixture. An amount of 100 parts by weight of a styrene monomer was added to the liquid mixture while the liquid mixture was stirred at 350 revolutions per minute. After that, the temperature of the solution was increased to 98° C. to perform a polymerization reaction. When the polymerization reaction is about 80% complete, the temperature of the reaction solution was increased to 120° C. over 30 minutes. The reaction solution was then maintained at 120° C. for 1 hour to produce a styrene-resin-particle-containing solution. The styrene-resin-particle-containing solution was cooled to 95° C., and then 2 parts by weight of cyclohexane and 7 parts by weight of butane as blowing agents were introduced into the autoclave by pressure. After that, the temperature of the solution was increased to 120° C. again. The solution was then maintained at 120° C. for 1 hour and then cooled to room temperature to obtain a polymerized slurry. The polymerized slurry was dehydrated, washed, and dried to obtain expandable styrene resin particles. The expandable styrene resin particles were sieved to obtain expandable styrene resin particles having a particle diameter of 0.2 mm to 0.3 mm. From the expandable styrene resin particles, sphere-like expanded polystyrene beads having an average diameter of 650 μm to 1200 μm were obtained using a pressurized foaming machine (BHP) manufactured by Obiraki Industry Co., Ltd. The expanded polystyrene beads were sieved using JIS test sieves having nominal aperture sizes (JIS Z 8801-1: 2019) of 1.18 mm and 1 mm. Expanded polystyrene beads passing through the sieve having a nominal aperture size of 1.18 mm and not passing through the sieve having a nominal aperture size of 1 mm were used. 
     (Preparation of Aqueous-Dispersion-Type Acrylic Adhesive) 
     An amount of 40 parts by weight of ion-exchange water was placed in a reaction container equipped with a cooling pipe, a nitrogen introduction pipe, a thermometer, and a stirrer, and was stirred at 60° C. for 1 hour or longer while a nitrogen gas was being introduced thereto for nitrogen purging. To the reaction container was added 0.1 parts by weight of 2,2′-azobis[N-(2-carboxyethyl)-2-methylpropionamidine]n-hydrate (polymerization initiator) to prepare a liquid mixture. A monomer emulsion A was dropped little by little over 4 hours for an emulsion polymerization reaction while this liquid mixture was maintained at 60° C. A reaction solution was thus obtained. The monomer emulsion A used was obtained by adding 98 parts by weight of 2-ethylhexyl acrylate, 1.25 parts by weight of acrylic acid, 0.75 parts by weight of methacrylic acid, 0.05 parts by weight of lauryl mercaptan (chain transfer agent), 0.02 parts by weight of γ-methacryloxypropyltrimethoxysilane (product name “KBM-503” manufactured by Shin-Etsu Chemical Co., Ltd.), and 2 parts by weight of polyoxyethylene sodium lauryl sulfate (emulsifier) to 30 parts by weight of ion-exchange water and emulsifying the mixture. After all the monomer emulsion A was dropped, the reaction solution was further maintained at 60° C. for 3 hours and was then cooled to room temperature. Next, 10% ammonia water was added to the reaction solution, and the pH of the reaction solution was adjusted to 7 to obtain an acrylic polymer emulsion (aqueous-dispersion-type acrylic polymer) A. An amount of 10 parts by weight, on a solids basis, of a resin emulsion (product name “E-865NT” manufactured by ARAKAWA CHEMICAL INDUSTRIES, LTD.) for imparting adhesiveness was added per 100 parts by weight of an acrylic polymer included in the acrylic polymer emulsion A to obtain a mixture. Furthermore, distilled water was added to the mixture so that a weight ratio of the mixture to the distilled water would be 10:5. An aqueous-dispersion-type acrylic adhesive was obtained in this manner. 
     (Sample 1) 
     Commercially-available polystyrene beads (average diameter: 3000 μm) (bulk density: 0.017 g/cm 3 ) and the aqueous-dispersion-type acrylic adhesive were weighed and added to a glass container at a weight ratio of 1:7. The mixture was added to UNIPACK L-4 manufactured by SEISAN NIPPONSHA LTD. The UNIPACK was sealed and shaken for 5 minutes by hand to mix the mixture. Next, scaly boron nitride (UHP-1K; average dimension of principal surfaces: 8 μm; thickness: 0.4 μm) manufactured by SHOWA DENKO K.K. was further added into the UNIPACK so that the polystyrene beads and the boron nitride would be in a weight ratio of 7:24, and thus a mixture was prepared. The UNIPACK was shaken for 5 minutes by hand to produce polystyrene beads coated with boron nitride. 
     A silicone resin (KE-106F) and silicone oil (KF-96-10CS) both manufactured by Shin-Etsu Chemical Co., Ltd. were added at a weight ratio of 10:5. A curing agent (CAT-106) manufactured by Shin-Etsu Chemical Co., Ltd. was further added to the mixture so that the silicone resin and the curing agent would be in a weight ratio of 10:0.85, and thus a thermosetting resin was produced. 
     The polystyrene beads coated with boron nitride were charged in a 95 mm×95 mm×24 mm plastic case, a plain-woven metal mesh (diameter: 0.18 mm; 50-mesh) made of stainless steel and manufactured by YOSHIDA TAKA K.K. was laid on the plastic case, and a perforated metal (diameter: 5 mm; thickness: 1 mm; pitch: 8 mm) made of stainless steel was further laid on the plain-woven metal mesh. The plastic case, the plain-woven metal mesh, and the perforated metal were fixed with a clamp. 
     The above-described thermosetting resin was added into the plastic case and defoamed under reduced pressure. The pressure applied was −0.08 MPa to −0.09 MPa in gauge pressure. This process was repeated three times to impregnate a gap between the polystyrene beads with the thermosetting resin. Next, the silicone resin was cured by heating at 80° C. for 2 hours to obtain a resin molded article including polystyrene beads. The resin molded article was cut to given dimensions. The cut resin molded article was completely immersed in ethyl acetate for 30 minutes to dissolve the polystyrene beads and let the polystyrene beads flow out of the resin molded article. After that, the resin molded article was dried at 90° C. for 3 hours. A composite material according to Sample 1 was produced in this manner. 
     (Samples 2 to 4) 
     Composite materials according to Samples 2 and 4 were each obtained in the same manner as in Sample 1, except that the polystyrene beads and the boron nitride described in Table 1 were used and a mixture was prepared at a ratio described in Table 
     (Sample 5) 
     A composite material according to Sample 5 was obtained in the same manner as in Sample 1, except that the polystyrene beads and the boron nitride described in Table 1 were used, a mixture was prepared at a ratio described in Table 1, and a thermosetting resin including 10 mass % of boron nitride was used instead of the thermosetting resin. 
     (Samples 6 and 7) 
     Composite materials according to Samples 6 and 7 were each obtained in the same manner as in Sample 1, except that the polystyrene beads and the boron nitride described in Table 1 were used, a mixture was prepared at a ratio described in Table 1, and a thermosetting resin including 20 mass % of boron nitride was used instead of the thermosetting resin. 
     (Sample 8) 
     A composite material according to Sample 8 was obtained in the same manner as in Sample 1, except that the polystyrene beads and the boron nitride described in Table 1 were used, a mixture was prepared at a ratio described in Table 1, and a thermosetting resin including 50 mass % of boron nitride was used instead of the thermosetting resin. 
     (Samples 9 to 14) 
     Boron nitride, the silicone resin, and ethanol were weighed to amounts described in Table 2 and mixed to prepare a mixture in a slurry state. The mixture was added to a tubular mold having a bottom and having a diameter of 50 mm and a height of 7 mm. Next, the mixture in the mold was heated at 100° C. for 1 hour to foam the silicone resin by the ethanol and cure the foamed silicone resin. Composite materials according to Samples 9 to 14 were obtained in this manner. 
     (Calculation of Amount [Volume %] of Inorganic Particles) 
     The amounts [volume %] of the inorganic particles in the composite materials according to Samples 1 to 14 were determined in the following manner. First, an organic substance was removed from each of the composite materials according to Samples 1 to 14 to extract the inorganic particles. The mass of the extracted inorganic particles was divided by the density (2.3 g/cm 3 ) of boron nitride to calculate the volume A of the inorganic particles. Separately, the volume B of the composite material was calculated from the volume and void ratio of the composite material, the volume B not including the volume of the voids  40 . The amount [volume %] of the inorganic particles in the composite material was determined by (A/B)×100. 
     (Calculation of Amount [Mass %] of Inorganic Particles) 
     The amounts [mass %] of the inorganic particles in the composite materials according to Samples 1 to 14 were determined in the following manner. First, about 10 mg of each of the composite materials according to Samples 1 to 14 was weighed out and added to a fluorine resin container. Hydrofluoric acid was added to the fluorine resin container, which was then sealed. A microwave was applied to the fluorine resin container to perform acid decomposition under pressure at a highest temperature of 220° C. Ultrapure water was added to the resulting solution to adjust the volume to 50 mL. Boron in the solution was quantified using ICP-AES SPS-3520UV manufactured by Hitachi High-Tech Science Corporation to determine the amount [mass %] of the inorganic particles. 
     (Heat Conductivity Measurement) 
     Heat conductivities of the composite materials according to Samples 1 to 14 were measured for one test specimen in a symmetric configuration by a heat flow meter method using a heat conductivity measurement apparatus TCM1001 manufactured by RHESCA Co., LTD. according to the American Society for Testing and Materials (ASTM) standard D5470-01 (steady state longitudinal heat flow method). Specifically, first, each composite material having a thickness t was cut to 20 mm×20 mm to obtain a test piece. A silicone grease (SHC-20; heat conductivity: 0.84 W/(m·K)) manufactured by Sunhayato Corp. was applied to both principal surfaces of the test piece so that each of the resulting silicone grease layers would have a given thickness equal to or less than 300 μm. An upper rod having a heating block (110° C.) and a lower rod having a cooling block (20° C.) were used as standard rods. Blocks made of oxygen-free copper were used as test blocks. The test piece was sandwiched by the blocks made of oxygen-free copper via the silicone grease layers to produce a measurement specimen. The measurement specimen was sandwiched between the upper rod and the lower rod. Heat was allowed to flow in the thickness direction of the test piece. 
     A temperature difference ΔTs between upper and lower surfaces of the test piece was determined by the following equations (3) and (4). In the equations (3) and (4), ΔTc is a temperature difference between the upper surface of the upper block (test block) made of oxygen-free copper and the lower surface of the lower block (test block) made of oxygen-free copper. Additionally, q 1  represents a heat flux [W/m 2 ] determined by a temperature gradient calculated based on temperature differences between a plurality of temperature measurement points on the upper rod, and q 2  represents a heat flux [W/m 2 ] determined by a temperature gradient calculated based on temperature differences between a plurality of temperature measurement points on the lower rod. A symbol t b  represents the sum of the thicknesses of the blocks made of oxygen-free copper. A symbol k b  represents the heat conductivity of the blocks made of oxygen-free copper. 
       Δ Ts=ΔTc −( qs×t   b )/ k   b   Equation (3)
 
         qs =( q   1   +q   2 )/2  Equation (4)
 
     A heat conductivity A [W/(m·K)] in the thickness direction of the test piece was determined by the following equation (5). 
       λ= qs×t/ΔTs   Equation (5)
 
     Tables 1 and 2 show the values A of heat conductivities obtained by the above (Heat conductivity measurement) and the values P 1  calculated using the heat conductivity values. The thickness t of each test piece was determined by measurement using a camera. 
     (Composition Analysis) 
     Using an ultra-high-resolution field-emission scanning electron microscope (SU8220) manufactured by Hitachi High-Technologies Corporation, particular regions of each of the composite materials according to Samples 1 to 14 were measured and the proportion of an atom included in the inorganic particle(s) included in each particular region of the composite material was calculated by energy dispersive X-ray spectroscopy. First, a measurement region was determined by the above method for each of the composite materials according to Samples 1 to 14. The proportion of an atom included in the inorganic particle(s) was measured in this measurement region. When the inorganic particle(s) are formed of boron nitride, the measured atom was boron (B). Y/X was calculated, where Y represents the largest proportion [atomic %] of the atom included in the inorganic particle(s) and X represents the smallest proportion [atomic %] of the atom included in the inorganic particle(s) in the measurement region. Additionally, the value Q was calculated by the above method. Tables 1 and 2 show the results. 
     The values P 1  of the composite materials according to Samples 1 to 7 are 6 or more. This reveals that the composite materials according to Samples 1 to 7 are suitable for achieving a high heat conductivity relative to the amount of the inorganic particles. 
     As shown in  FIG.  4   , the composite material according to Sample 1 includes a solid portion including inorganic particles and a resin, and includes a plurality of voids surrounded by the solid portion. In the composite material according to Sample 1, the voids have substantially similar outer shapes to each other. Additionally, the outer shapes of the voids are substantially spherical. Moreover, the plurality of voids are in contact with each other directly or via the inorganic particle. 
     
       
         
           
               
               
               
               
               
               
               
               
               
             
               
                   
                 TABLE 1 
               
               
                   
                   
               
               
                   
                 Sample 1 
                 Sample 2 
                 Sample 3 
                 Sample 4 
                 Sample 5 
                 Sample 6 
                 Sample 7 
                 Sample 8 
               
               
                   
                   
               
             
            
               
                   
               
            
           
           
               
               
               
               
               
               
               
               
               
            
               
                 Polystyrene beads [mass %] 
                 7 
                 7 
                 7 
                 7 
                 7 
                 7 
                 5 
                 7 
               
               
                 Aqueous-dispersion-type acrylic 
                 10 
                 10 
                 10 
                 7 
                 7 
                 7 
                 5 
                 7 
               
               
                 adhesive [mass %] 
               
               
                 Boron nitride [mass %] 
                 24 
                 33 
                 27 
                 14 
                 16 
                 16 
                 34 
                 16 
               
               
                 Resin [mass %] 
                 59 
                 50 
                 56 
                 72 
                 60 
                 52 
                 37 
                 20 
               
               
                 Average diameter [μm] of voids 
                 3000 
                 3000 
                 3000 
                 1000 
                 1000 
                 1000 
                 1000 
                 1000 
               
               
                 Void ratio [volume %] 
                 41 
                 40 
                 41 
                 27 
                 34 
                 27 
                 29 
                 34 
               
            
           
           
               
               
               
               
               
               
               
               
               
               
            
               
                 Inorganic 
                 Aspect ratio 
                 20 
                 7 
                 90 
                 50 
                 20 
                 20 
                 7 
                 20 
               
               
                 particles 
                 Average dimension 
                 8 
                 0.7 
                 18 
                 5 
                 8 
                 8 
                 0.7 
                 8 
               
               
                   
                 [μm] of principal 
               
               
                   
                 surfaces 
               
               
                   
                 Thickness [μm] 
                 0.4 
                 0.1 
                 0.2 
                 0.1 
                 0.4 
                 0.4 
                 0.1 
                 0.4 
               
               
                   
                 Amount [mass %] 
                 12 
                 14 
                 13 
                 12 
                 26 
                 36 
                 52 
                 66 
               
               
                   
                 Amount [volume %] 
                 4 
                 5 
                 4 
                 4 
                 10 
                 15 
                 28 
                 38 
               
            
           
           
               
               
               
               
               
               
               
               
               
            
               
                 Heat conductivity λ [W/(m · K)] 
                 0.59 
                 0.62 
                 0.81 
                 0.89 
                 1.21 
                 1.25 
                 1.81 
                 2.17 
               
               
                 P 0   
                 154 
                 1714 
                 68 
                 54 
                 43 
                 34 
                 414 
                 43 
               
               
                 P 1   
                 15.1 
                 12.4 
                 20.3 
                 22.8 
                 12.7 
                 8.3 
                 6.5 
                 5.7 
               
               
                 Y/X 
                 5.7 
                 5.0 
                 5.3 
                 5.9 
                 2.8 
                 2.5 
                 2.8 
                 1.8 
               
               
                 Q 
                 85.0 
                 83.3 
                 84.2 
                 85.5 
                 73.7 
                 71.7 
                 73.5 
                 64.2 
               
               
                   
               
            
           
         
       
     
     
       
         
           
               
               
               
               
               
               
               
             
               
                   
                 TABLE 2 
               
               
                   
                   
               
               
                   
                 Sample 9 
                 Sample 10 
                 Sample 11 
                 Sample 12 
                 Sample 13 
                 Sample 14 
               
               
                   
                   
               
             
            
               
                   
               
            
           
           
               
               
               
               
               
               
               
            
               
                 Boron nitride [mass %] 
                 14 
                 20 
                 20 
                 20 
                 34 
                 60 
               
               
                 Silicone resin [mass %] 
                 84 
                 78 
                 78 
                 78 
                 64 
                 38 
               
               
                 Ethanol [mass %] 
                 2 
                 2 
                 2 
                 2 
                 2 
                 2 
               
               
                 Average diameter [μm] of voids 
                 200 
                 200 
                 200 
                 200 
                 200 
                 200 
               
               
                 Void ratio [volume %] 
                 50 
                 50 
                 50 
                 50 
                 50 
                 50 
               
            
           
           
               
               
               
               
               
               
               
               
            
               
                 Inorganic 
                 Aspect ratio 
                 50 
                 20 
                 7 
                 50 
                 7 
                 20 
               
               
                 particles 
                 Average dimension 
                 5 
                 8 
                 0.7 
                 5 
                 0.7 
                 8 
               
               
                   
                 [μm] of principal 
               
               
                   
                 surfaces 
               
               
                   
                 Thickness [μm] 
                 0.1 
                 0.4 
                 0.1 
                 0.1 
                 0.1 
                 0.4 
               
               
                   
                 Amount [mass %] 
                 14 
                 20 
                 20 
                 20 
                 34 
                 60 
               
               
                   
                 Amount [volume %] 
                 6 
                 7 
                 7 
                 7 
                 12 
                 32 
               
            
           
           
               
               
               
               
               
               
               
            
               
                 Heat conductivity λ [W/(m · K)] 
                 0.12 
                 0.13 
                 0.12 
                 0.13 
                 0.38 
                 1.24 
               
               
                 P 0   
                 20 
                 13 
                 143 
                 20 
                 143 
                 13 
               
               
                 P 1   
                 2.0 
                 1.9 
                 1.7 
                 1.9 
                 3.2 
                 3.9 
               
               
                 Y/X 
                 1.3 
                 1.5 
                 1.3 
                 1.4 
                 1.3 
                 1.2 
               
               
                 Q 
                 55.7 
                 60.5 
                 55.9 
                 57.6 
                 56.8 
                 55.3 
               
               
                   
               
            
           
         
       
     
     The method for producing the composite material of Example 1-1 described in Patent Literature 1 and the method for producing the composite material of Sample 14 of the present embodiment are similar. From this fact, the structure of the composite material of Example 1-1 of Patent Literature 1 and the structure of the composite material of Sample 14 of the present embodiment can be considered similar. According to the paragraph 0055 of Patent Literature 1, the heat conductivity of the composite material described in Patent Literature 1 is measured by a flash method, which is an unsteady-state method. On the other hand, the heat conductivity of the composite material according to the present embodiment is measured by the steady state longitudinal heat flow method including a surface resistance of the composite material. Therefore, the heat conductivity (3.85 W/m·K) of the composite material described in Example 1-1 of Patent Literature 1 and the heat conductivity of the composite material of Sample 14 according to the present embodiment are greatly different. The composite material of Example 1-1 of Patent Literature 1 has the greatest heat conductivity relative to the filling amount of fillers. According to the technique described in Patent Literature 1, P 1  is 3.9 or less. The values P 1  of the composite materials according to Samples 1 to 7 are 6 or more. These reveal that the composite material according to the present embodiment is suitable for achieving a higher heat conductivity relative to the amount of the inorganic particles.