# Patent

## Title
Manufacture of microcellular foam tires

## Abstract

This is a division of application Ser. No. 07/699,591 filed May 14, 1991 now U.S. Pat. No. 5,110,644.

## Background
The present invention relates to a silicon nitride sintered material having a high-temperature strength, excellent thermal shock resistance and a low Young's modulus, as well as to a process for producing the sintered material.

With respect to silicon nitride sintered materials containing oxides of IIIa group elements including rare earth elements, for example, Japanese Patent Publication No. 7486/1973 discloses a process for producing a sintered material, which comprises mixing and shaping 85 mole % or more of silicon nitride (Si.sub.3 N.sub.4) and 15 mole % or less of at least one oxide selected from oxides of IIIa group elements and then sintering the shaped material in a non-oxidizing atmosphere; and Japanese Patent Publication No. 21091/1974 discloses a silicon nitride sintered material consisting of 50% by weight of Si.sub.3 N.sub.4, 50% by weight or less of at least one oxide selected from Y.sub.2 O.sub.3 and oxides of La type elements and 0.01-20% by weight of Al.sub.2 O.sub.3.

However, there have been problems that addition of only rare earth elements to silicon nitride fails to provide a sintered material having a high-temperature strength and addition of Al.sub.2 O.sub.3 provides a sintered material which has a higher density but whose grain boundary phase has a lower melting point and gives a very low high-temperature strength.

In order to solve the problem of high-temperature strength, Japanese Patent Application Kokai (Laid-Open) No. 100067/1988 discloses a technique for achieving a high-temperature strength by adding rare earth elements of given composition and given proportion to a Si.sub.3 N.sub.4 powder and sintering the mixture to allow the resulting sintered material to have a specific crystalline phase.

The silicon nitride sintered material disclosed in Japanese Patent Application Kokai (Laid-Open) No. 100067/1988 can achieve a high-temperature strength to some extent but has problems that the Young's modulus is as large as 300 GPa and the thermal shock resistance .DELTA.Tc (.degree.C.) is as small as 1,000.degree. C. This is because the silicon nitride sintered material is homogeneous microscopically, and has a Young's modulus and thermal expansion coefficient characteristic of silicon nitride and, as a result, the thermal shock resistance .DELTA.Tc (.degree.C.) of the silicon nitride sintered material is substantially determined depending upon its strength. The thermal shock resistance .DELTA.Tc (.degree.C.) of a ceramic can be evaluated by the following formula.

[.sigma. is a flexural strength (Pa), .alpha. is a thermal expansion coefficient (1/.degree.C.), and E is a Young's modulus (Pa).]

The object of the present invention is to solve the above-mentioned problems and provide a silicon nitride sintered material having a high-temperature strength about equal to the room temperature thereof and excellent thermal shock resistance, as well as a process for producing the sintered material.

According to the present invention, there is provided a thermal shock-resistant silicon nitride sintered material consisting substantially of silicon nitride and rare earth element compounds, which material contains at least 10 pore groups per mm.sup.2, each pore group consisting of pores of 10 .mu.m or less in diameter and having a diameter of 30-100 .mu.m and which material has a thermal shock resistance .DELTA.Tc (.degree.C.) of 1,000.degree. C. or more.

The present invention further provides a process for producing a thermal shock-resistant silicon nitride sintered material, which process comprises mixing and shaping starting materials consisting of a silicon nitride powder, powders of rare earth element oxides and carbide powders, and then firing the shaped material in a nitrogen atmosphere to (a) react the carbide powders with the silicon oxide present in the silicon nitride to convert the carbide to nitrides or silicides and simultaneously give rise to decomposition gases and (b) thereby form, in the resulting sintered material, pores of 10 .mu.m or less in diameter and pore groups each consisting of said pores and having a diameter of 30-100 .mu.m.

In the present invention, the sintered material obtained can be subjected to a heat treatment of 1,000.degree.-1,500.degree. C. in an oxygen-containing atmosphere to form, on the surface, a surface layer of 5-100 .mu.m in thickness consisting of silicates of rare earth elements and silicon oxide, whereby a silicon nitride sintered material of higher strength and higher thermal shock resistance can be obtained.

FIG. 1 is a schematic illustration showing the microstructure of the silicon nitride sintered material according to the present invention.

FIG. 2 is a micrograph of the silicon nitride sintered material of Example 1 according to the present invention after the polished surface has been oxidized.

FIG. 3 is a micrograph of the silicon nitride sintered material of Comparative Example 1 after the polished surface has been oxidized.

FIG. 4 is a micrograph of the silicon nitride sintered material of Comparative Example 3 after the polished surface has been oxidized.

In the present invention, a silicon nitride powder containing powders of given rare earth element oxides is mixed with carbide powders and the resulting mixture is fired in a nitrogen atmosphere, whereby is obtained a silicon nitride sintered material which contains at least 10 pore groups per mm.sup.2, each consisting of micropores of 10 .mu.m or less in diameter and having a diameter of 30-100 .mu.m and which accordingly has a unique microstructure. This silicon nitride sintered material has a high-temperature strength about equal to the room temperature thereof strength and excellent thermal shock resistance.

The silicon nitride as a starting material contains oxygen as an impurity, and this oxygen is present in the form of SiO.sub.2. By utilizing the reaction of this SiO.sub.2 with carbides in a nitrogen atmosphere, for example, the following reaction, decomposition gases can be generated in the resulting sintered material.

In the present invention, by adding carbides to silicon nitride and decomposing the carbide as above at a temperature close to the sintering temperature, there can be obtained a silicon nitride sintered material having a unique structure as shown in FIG. 1, containing at least 10 pore groups per mm.sup.2 of sintered material, each consisting of micropores of 10 .mu.m or less in diameter and having a diameter of 30-100 .mu.m. In FIG. 1, the numeral 1 refers to a sintered material; the numeral 2 refers to micropores; and the numeral 3 refers to a pore group.

Such a silicon nitride sintered material containing groups of micropores causes no deterioration in strength, unlike sintered materials containing ordinary pores. The presence of micropore groups is effective for reduction in Young's modulus, making it possible to obtain a silicon nitride sintered material of high strength and low Young's modulus. As is known, the thermal shock resistance of a ceramic can be evaluated by its .DELTA.Tc (.degree.C.), and a larger .DELTA.Tc value gives higher thermal shock resistance. When, for example, a material heated to 1,000.degree. C. is placed into cool water of 0.degree. C. and thereby the material begins to cause cracking, etc. and resultantly reduction in strength, the .DELTA.Tc (.degree.C.) of the material is defined to be 1,000.degree. C. In general, the .DELTA.Tc of a ceramic is given by the following formula

[.sigma. is a flexural strength (Pa), .alpha. is a thermal expansion coefficient (1/.degree.C.), and E is a Young's modulus (Pa)], and is dependent upon the strength, thermal expansion coefficient and Young's modulus of the ceramic. Therefore, when the strength is constant, as the Young's modulus is lower, the .DELTA.Tc is larger and the thermal shock resistance is higher, providing a more useful material.

The silicon nitride sintered material of the present invention is just such a material, and has a reduced Young's modulus without sacrificing the strength and accordingly has significantly improved thermal shock resistance.

In the present invention, the oxygen amount in the silicon nitride used as a starting material is desirably 1-3% by weight. This oxygen amount can be controlled by oxidizing the silicon nitride, or by adding a SiO.sub.2 powder to the silicon nitride.

The total amount of the rare earth element oxides used also as a starting material is preferably 6-21% by weight. When the total amount is less than 6% by weight, it is impossible to obtain a liquid phase necessary for achieving a high density. When the total amount is more than 21% by weight, it tends to be difficult to achieve a high density. As the rare earth element oxides other than Y.sub.2 O.sub.3 and Yb.sub.2 O.sub.3, there can also be used Lu.sub.2 O.sub.3, Tm.sub.2 O.sub.3, Er.sub.2 O.sub.3, etc. The total amount of the rare earth elements in sintered material is the same as that in the starting materials.

The amount of the carbides used also as a starting material is preferably 0.5-10% by weight. An amount of less than 0.5% by weight is not effective to sufficiently form pore groups. An amount of more than 10% by weight hinders the achievement of a high density in some cases. The amount of the carbide is more preferably 1-5% by weight. The C content in sintered material is 1/2 or less of the C content in the starting materials. Incidentally, the type of carbide is not restricted by the crystalline phase; and, in the case of SiC, there can be used any of .alpha. type, .beta. type and amorphous type.

In the process for producing a silicon nitride sintered material according to the present invention, at first there is prepared a mixture of a silicon nitride powder, powders of rare earth element oxides and carbide powders. The mixture is then made into a desired shape to obtain a shaped material. Thereafter, the shaped material is fired at 1,700.degree.-2,100.degree. C., preferably 1,900.degree.-2,000.degree. C., for 3-6 hours in a nitrogen atmosphere of normal pressure to applied pressure corresponding to the firing temperature to (a) react the carbide powders with the silicon oxide present in the silicon nitride to convert the carbide to nitride or silicide and thereby (b) generate the decomposition gases to form pores of 10 .mu.m or less in diameter and simultaneously form groups of said pores, each having a diameter of 30-100 .mu.m, whereby a silicon nitride sintered material of the present invention can be obtained.

It is possible that the thus obtained silicon nitride sintered material itself or after having been subjected to grinding, etc. so as to have a desired shape, is subjected to a heat treatment at 1,000.degree.-1,500.degree. C. in an oxygen-containing atmosphere to form, on the surface, a surface layer of 5-100 .mu.m in thickness consisting of silicates of rare earth elements and silicon oxide and thereby obtain a silicon nitride sintered material further improved in thermal shock resistance.

The present invention is hereinafter described in more detail by way of Examples. However, the present invention is in no way restricted to these Examples.

There were mixed (a) a silicon nitride powder having a purity of 97% by weight, an oxygen content of 2.2% by weight, an average particle diameter of 0.6 .mu.m and a BET specific surface area of 17 m.sup.2 /g, (b) powders of oxides shown in Table 1, having a purity of 99.9% by weight and an average particle diameter of 0.3-2.5 .mu.m and (c) powders of carbides shown in Table 1, such as SiC, WC, Mo.sub.2 C, TiC, NbC, TiC and the like, having a purity of 99% by weight and an average particle diameter of 0.4-3 .mu.m, in proportions shown in Table 1. 200 g of the resulting mixture, 1,800 g of pebbles made of a silicon nitride ceramic and 300 ml of water were placed in a 1.2-l nylon container, and the container was placed in a vibration mill and subjected to vibration of 1,200 times/min for 3 hours to grind the mixture. Then, water was vaporized and the ground mixture was granulated to a particle diameter of 150 .mu.m to obtain a powder for shaping. Thereafter, the powder was subjected to cold isostatic pressing at a pressure of 7 ton/cm.sup.2 to prepare a shaped material of 50.times.40.times.6 mm, and the shaped material was fired under the firing conditions shown in Table 1 to obtain silicon nitride sintered materials of Examples 1-15 of the present invention. The sintered materials of Examples 10-12 were further subjected to a heat treatment.

Separately, there were mixed the same silicon nitride powder as above, powders of oxides shown in Table 2 and a powder of a carbide shown in Table 2, in proportions shown in Table 2; the resulting mixture was subjected to the same grinding, granulation and shaping as above; the resulting shaped material was fired under the firing conditions shown in Table 2 to obtain sintered materials of Comparative Examples 1-6.

Each of the above obtained sintered materials was measured for bulk density, crystalline phase of grain boundary, 4-point flexural strengths at room temperature, 1,000.degree. C. and 1,400.degree. C., Young's modulus at room temperature and thermal shock resistance .DELTA.Tc (.degree.C.). The results are shown in Tables 1 and 2. In Tables 1 and 2, bulk density of the sintered material was measured by the Archimedes' method. This density was expressed in the tables as a value relative to theoretical density, wherein the theoretical density was calculated from the composition of mixed powder and its density. In calculating density of the mixed powder, the following densities were used Si.sub.3 N.sub.4 : 3.2 g/cm.sup.3, Y.sub.2 O.sub.3 : 5.0 g/cm.sup.3, Yb.sub.2 O.sub.3 : 9.2 g/cm.sup.3, Tm.sub.2 O.sub.3 : 8.8 g/cm.sup.3, Lu.sub.2 O.sub.3 : 9.4 g/cm.sup.3, Er.sub.2 O.sub.3 : 8.6 g/cm.sup.3, SiC: 3.2 g/cm.sup.3, WC: 15.6 g/cm.sup.3, Mo.sub.2 C: 8.9 g/cm.sup.3, TiC: 4.9 g/cm.sup.3, TaC: 14.7 g/cm.sup.3, and NbC: 7.8 g/cm.sup.3. 4-Point flexural strength was measured in accordance with JIS R 1601 "Test Method for Flexural Strength (Modulus of Rupture) of High Performance Ceramics". Crystalline phase of grain boundary was determined from the results of X-ray diffraction by CuK .alpha.-rays. In Tables 1 and 2, J is a cuspidine type crystal and gives the same diffraction pattern as Si.sub.3 N.sub.4.4Y.sub.2 O.sub.3.SiO.sub.2 represented by JCPDS card 32-1451, wherein the crystallographic position of Y can be replaced by other rare earth element. H is an apatite type crystal and gives the same diffraction pattern as Si.sub.3 N.sub.4.10Y.sub.2 O.sub.3.9SiO.sub.2 represented by JCPDS card 30-1462, wherein the crystallographic position of Y can be replaced by other rare earth element. K is a wollastonite type crystal and gives the same diffraction pattern as 2Y.sub.2 O.sub.3.SiO.sub.2.Si.sub.3 N.sub.4 represented by JCPDS card 31-1462, wherein the crystallographic position of Y can be replaced by other rare earth element. L is a crystal represented by Re.sub.2 SiO.sub.5 (Re: rare earth element) and gives the same diffraction pattern as any of JCPDS cards 21-1456, 21-1458, 21-1461, 22-992 and 36-1476. S is a crystal represented by Re.sub.2 SiO.sub.7 (Re: rare earth element) and gives the same diffraction pattern as any of JCPDS cards 20-1416, 21-1457, 21-1459, 21-1460, 22-994 and 22-1103. C is a SiO.sub.2 (cristobalite) crystal and gives diffraction patterns represented by JCPDS cards 11-695 and 27-605. The amount of each crystalline phase was determined from the maximum height of the diffraction pattern. In Tables 1 and 2, ">" (inequality sign) refers to "larger" or "smaller" in amount of crystalline phase, and "," refers to "about equal" in amount of crystalline phase.

Young's modulus (room temperature) was measured by a pulse echo overlap method using a columnar sample of 10 mm.phi..times.20 mm (length). Thermal shock resistance .DELTA.Tc (.degree.C.) was measured by an in-water quenching method wherein a test piece heated to a given temperature was placed into water to quench it and the reduction in room temperature strength of the test piece was examined.

Average pore diameter and pore group diameter were measured by subjecting a sintered material to polishing to allow the material to have a mirror surface and subjecting the mirror surface to image analysis using an optical microscope. Pore group density was determined by subjecting a sintered material to the same polishing, subjecting the resulting material to an oxidation treatment in air, and then measuring the number of pore groups per unit area. The oxidation treatment enables easy measurement of the number of pore groups. The size of each pore group looks larger than the actual diameter of each pore group.

FIG. 2 is photomicrograph of the silicon nitride sintered material of Example 1 of the present invention after the polished surface has been oxidized. In the photomicro-graph, white spots are groups of pores.

Meanwhile, FIG. 3 is photomicrograph of the silicon nitride sintered material of Comparative Example 1 after the polished surface has been oxidized, wherein no white spots having a diameter of 30 .mu.m or more are seen.

FIG. 4 is photomicrograph of the silicon nitride sintered material of Comparative Example 3 after the polished surface has been oxidized, wherein pore groups of abnormally large size are seen. __________________________________________________________________________ Example No.                      1   2   3   4   5    6    7   8   9 __________________________________________________________________________ Powders Proportions Y.sub.2 O.sub.3 3.4 3.2 --  2.0 2.0  2.0  9.9 4.2 3.4 mixed   (wt %) Yb.sub.2 O.sub.3 13.9 13.3 14.9 8.9 6.9  4.0   0  16.8 13.5 Other(s) Carbide(s) SiC 1 SiC 5 SiC 0.5 WC 1 Mo.sub.2 C 1 SiC 0.5 TiC 1 NbC SiC 10 Mo.sub.2 C 0.5 Chemical C content (wt %) 0.35 1.55 0.20 0.11 0.10 0.23 0.25 0.13 3.05 analysis O content (wt %) 4.53 4.35 4.55 3.76 3.41 3.02 4.19 4.93 4.28 Sintered Chemical C content (wt %) 0.05 0.75 0.10 0.04 0.04 0.05 0.03 0.02 1.50 material analysis O content (wt %) 3.98 3.24 3.43 3.26 2.95 2.52 3.39 4.43 2.98 Structure Average pore 5   10  2   2   2    3    3   3   10 of    diameter (.mu.m) sintered Pore group diameter 70 100  30  20  20   30   35  30 100 material (.mu.m) Pore group density 30  50  15  10  11   16   20  15 100 (per mm.sup.2) Surface layer --  --  --  --  --   --   --  --  -- thickness (.mu.m) Crystalline phase of --  --  --  --  --   --   --  --  -- surface layer Mechanical Flexural strength properties R.T. (MPa) 820 800 750 850 780  690  790 710 750 1000.degree. C. (MPa) 820 800 750 850 780  690  790 710 750 1400.degree. C. (MPa) 820 800 740 840 750  670  760 700 740 Young's Modulus 260 250 270 270 270  270  270 270 250 R.T. (GPa) Thermal shock 1300 1300 1100 1300 1150 1000 1200 1050 1200 resistance (.degree.C.) Relative density of 99  99  97  97  99   99   99  99  95 sintered material (%) Crystalline phase of J   J   J   H   H > J L > S J   J   J grain be undary Firing        Firing temperature 1900 1900 1700 2100 1900 1900 1950 1900 1900 conditions    (.degree.C.) Firing time (hr) 4   4   6   2   4    4    3   4   6 Nitrogen pressure 10  10  1  100  10   10   50  10  10 (atm) Heat          Heat treatment --  --  --  --  --   --   --  --  -- treatment     temperature (.degree.C.) conditions    Heat treatment --  --  --  --  --   --   --  --  -- time (hr) __________________________________________________________________________ Example No.                      10    11    12    13     14     15 __________________________________________________________________________ Powders Proportions Y.sub.2 O.sub.3 3.4   3.4   3.4   1.9    --     1.9 mixed   (wt %) Yb.sub.2 O.sub.3 13.9  13.9  13.9  --     6.7    -- Other(s)                     Tm.sub.2 O.sub.3 Lu.sub.2 O.sub.3 Er.sub.2 O.sub.3 12.5 Carbide(s) SiC 1 SiC 1 SiC 1 Mo.sub.2 C 4 TaC 4  Mo.sub.2 C 4 Chemical C content (wt %) 0.35  0.35  0.35  0.26   0.30   0.26 analysis O content (wt %) 4.53  4.53  4.53  3.48   3.68   4.01 Sintered Chemical C content (wt %) 0.05  0.05  0.05  0.03   0.09   0.04 material analysis O content (wt %) 3.98  3.98  3.98  2.88   3.14   3.48 Structure Average pore 5     5     5     8      5      4 of    diameter (.mu.m) sintered Pore group diameter 70    70    70    80     70     50 material (.mu.m) Pore group density 30    30     30   50     40     50 (per mm.sup.2) Surface layer 30   100    20   --     --     -- thickness (.mu.m) Crystalline phase of S > L,C S > L,C S > L,C --     --     -- surface layer Mechanical Flexural strength properties R.T. (MPa) 850   850   750   770    780    800 1000.degree. C. (MPa) 850   850   750   770    780    800 1400.degree. C. (MPa) 850   850   740   750    760    780 Young's Modulus 260   260   270   250    250    250 R.T. (GPa) Thermal shock 1350  1350  1100  1200   1200   1300 resistance (.degree.C.) Relative density of 99    99    97    98     98     98 sintered material (%) Crystalline phase of J,H   J,H   J,H   H > L  J      J grain be undary Firing        Firing temperature 1900  1900  1900  2000   1900   1900 conditions    (.degree.C.) Firing time (hr) 4     4     4     3      4      4 Nitrogen pressure 10    10    10   100     10     10 (atm) Heat          Heat treatment 1300  1500  1000  --     --     -- treatment     temperature (.degree.C.) conditions    Heat treatment 1     1     5    --     --     -- time (hr) __________________________________________________________________________ __________________________________________________________________________ Comparative Example 2    3   4    5    6 __________________________________________________________________________ Powders Proportions Y.sub.2 O.sub.3 3.4 2.2  2.0  5   2.9  5.0 mixed   (wt %) Yb.sub.2 O.sub.3 14.0 8.8  8.9 --   11.9 19.0 Other(s)   --  --   --  MgO 3 --   -- ZrO.sub.2 0.3 Carbide(s) SiC 0.1 --   SiC 1 SiC 1 SiC 15 SiC 1 Chemical C content (wt %) 0.08 0.05 0.35 0.35 4.54 0.35 analysis O content (wt %) 3.80 4.53 4.60 3.90 5.40 Sintered Chemical C content (wt %) 0.05 0.05 0.02 0.32 4.04 0.06 material analysis O content (wt %) 3.40 3.70 4.48 3.07 4.50 Structure Average pore 2   2    10  2    15   10 of    diameter (.mu.m) sintered Pore group diameter 20 No pore 250 No pore No pore No pore material (.mu. m) Pore group density 5  group 10 group group group (per mm.sup.2) Surface layer --  --   --  --   --   -- thickness (.mu.m) Crystalline phase of --  --   --  --   --   -- surface layer Mechanical Flexural strength properties R.T. (MPa) 770 700  500 1000 500  600 1000.degree. C. (MPa) 770 650  500 1000 500  -- 1400.degree. C. (MPa) 750 600  500 300  --   -- Young's Modulus 300 300  250 270  250  -- R.T. (GPa) Thermal shock 800 800  500 900  500  -- resistance (.degree.C.) Relative density of 97  96   99  98   80   85 sintered material (%) Crystalline phase of J > H H > S J   J    J > H grain be undary Firing        Firing temperature 1900 1900 1900 1700 1850 1900 conditions    (.degree.C.) Firing time (hr) 2   2    10  1    5    2 Nitrogen pressure 10  10   10  1    5    10 (atm) Heat          Heat treatment --  --   --  --   --   -- treatment     temperature (.degree.C.) conditions    Heat treatment --  --   --  --   --   -- time (hr) __________________________________________________________________________

As is seen from Tables 1 and 2, the sintered materials of Examples 1-15 of the present invention using rare earth element oxides as a sintering aid and carbides, have a high relative density of 95% or more, a low Young's modulus of 270 GPa or less and a high thermal shock resistance .DELTA.Tc (.degree.C.) of 1,000.degree. C. or more. Meanwhile, the sintered materials of Comparative Examples 1 and 2 using a carbide in an amount of less than 0.5% by weight, have pore groups of less than 30 .mu.m in diameter and accordingly have a high Young's modulus of 300 GPa and a low thermal shock resistance .DELTA.Tc (.degree.C.) of less than 1,000.degree. C. although they have about the same strength as the sintered materials of the present invention.

The sintered material of Comparative Example 5 having an average pore diameter of more than 10 .mu.m and the sintered material of Comparative Example 3 having pore groups of more than 100 .mu.m in diameter, have a low strength and accordingly a low thermal shock resistance .DELTA.Tc (.degree.C.) although they have a low Young's modulus.

Further, as appreciated from Examples 10-12, when the sintered material of the present invention is heat-treated at 1,000-1,500.degree. C. in air, a surface layer consisting of silicates of rare earth elements and silicon oxide is formed on the surface of the sintered material, and such a sintered material has a higher strength and higher thermal shock resistance.

## Claims

1. A process for producing a thermal shock-resistant silicon nitride sintered material containing at least 10 pore groups per mm.sup.2, wherein each pore group has a diameter of 30 to 100 .mu.m and consists of pores having diameters of 10 .mu.m or less, said process comprising: oxide powders and 0.5-5 wt % carbide powders; C. for 3-6 hours in a nitrogen atmosphere to decompose the carbide powders to form said pore groups in the resulting sintered material.

2. The process of claim 1, further comprising the step of subjecting the sintered material to a heat treatment at 1000.degree.-1500.degree. C. in an oxygen-containing atmosphere to obtain a thermal shock-resistant silicon nitride sintered material having a surface layer of 5-100 .mu.m in thickness and consisting of silicates of rare earth elements and silicon oxide.

3. A process for producing a thermal shock-resistant silicon nitride sintered material containing at least 10 pore groups per mm.sup.2, wherein each pore group has a diameter of 30 to 100 .mu.m and consists of pores having diameters of 10 .mu.m or less, said process comprising: oxide powders, and 0.5-5 wt % carbide powders having an average particle diameter of 0.4-3 .mu.m; carbide powders to obtain said thermal shock-resistant silicon nitride sintered material; sintered material is less than half the carbon content in said starting materials.

4. The process of claim 3, wherein said shaped material is fired at a temperature ranging from 1700.degree. C.-2100.degree. C. for 3-6 hours.

5. The process of claim 3, wherein an amount of said rare earth oxide powders in said starting materials is 6-21 wt. %.