Cubic boron nitride sintered body and method of preparing the same

Abstract: Provided is a cubic boron nitride sintered body having sufficient strength, hardness, heat resistance and heat dissipativity for serving as a cutting tool. In a method of preparing a cubic boron nitride sintered body by directly converting low-pressure phase boron nitride under a high temperature and a high pressure and simultaneously sintering the same, the low-pressure phase boron nitride serving as a starting material is prepared by reducing a compound containing boron and oxygen with a compound containing nitrogen and carbon. In the obtained cubic boron nitride sintered body, the ratio I 220 /I 111 of X-ray diffraction intensity I 220 on the (220) plane to X-ray diffraction intensity I 111 on the (111) plane is at least 0.1.

Description: The present invention relates to a cubic boron nitride sintered body and a method of preparing the same, and more particularly, it relates to a cubic boron nitride sintered body obtained by directly converting low-pressure phase boron nitride and simultaneously sintering the same and a method of preparing such a cubic boron nitride sintered body. A sintered body of cubic boron nitride (hereinafter referred to as cBN), which has the next highest hardness after that of diamond and reacts with no ferrous material, is generally applied to a cutting tool for a ferrous material. Such a sintered body of cBN applied to a cutting tool is generally prepared by sintering cBN powder with a binder consisting of TiN, TiC, Co or the like under a superhigh pressure. The cBN sintered body obtained in this manner contains about 10 to 40 percent by volume of impurity. This impurity is TiN, TiC, Co or the like forming the binder. This impurity causes reduction of strength, heat resistance and heat dissipativity of the cBN sintered body. Particularly in case of cutting a ferrous material with such a cutting tool at a high speed, its cutting edge is readily chipped or cracked to reduce the life of the cutting tool. A method of preparing a cBN sintered body with no binder is known as that for solving this problem. This method is adapted to react and sinter a raw material of hexagonal boron nitride (hereinafter referred to as hBN) with a catalyst such as magnesium boronitride, for preparing a cBN sintered body. The sintered body obtained in this manner has high heat conductivity of 6 to 7 W/cm•°C since the amount of impurity contained therein is small and cBN grains are strongly bonded to each other therein. Therefore, this sintered body is applied to a heat sink material or a TAB (tape automated bonding) tool. However, the catalyst such as magnesium boronitride remains in this sintered body. When heated, therefore, fine cracks are readily caused in the cBN sintered body due to thermal expansion difference between the catalyst and cBN. Therefore, this sintered body, having a low heat-resistance temperature of about 700°C, cannot be applied to a cutting tool. Further, the sintered body are formed by large cBN grains of about 10 µM in diameter, and hence its strength is reduced although the same has a high heat transfer coefficient. When this sintered body is applied to a cutting edge of a cutting tool, therefore, it is difficult to intermittently cut a workpiece with a high load. On the other hand, a method of directly converting hBN to a cBN sintered body under a superhigh temperature and a superhigh pressure with no binder or catalyst is also known. For example, each of Japanese Patent Laying-Open Nos. 47-34099 (1972) and 3-159964 (1991) discloses a method of keeping hBN at a pressure of 7 GPa and a temperature of at least 2100°C for obtaining a cBN sintered body. In case of industrial production, however, this method is disadvantageous in cost or productivity. In this method, further, large cBN crystals are readily grown due to the sintering under a high temperature. Thus, the strength of the sintered body is so reduced that its cutting edge is chipped when applied to a cutting tool. Further, hBN employed in this method is readily oriented in the <111> direction, and hence the cBN sintered body prepared from this material is also readily oriented in the <111> direction. When the cBN sintered body obtained by this method is applied to a cutting tool, therefore, layer cracking or separation is disadvantageously caused. On the other hand, each of Japanese Patent Laying-Open Nos. 54-33510 (1979) and 8-47801 (1996) discloses a method of preparing a cBN sintered body from pyrolytic boron nitride (hereinafter referred to as pBN) with no binder or catalyst. However, this method is disadvantageous in cost or productivity in case of industrial production. In this method, further, pBN employed as the raw material is extremely at a high cost, compressed hBN readily remains in the cBN sintered body, and layer cracking or separation is readily caused due to strong orientation of the cBN sintered body. Japanese Patent Publication No. 49-27518 (1974) discloses a method of preparing a cBN sintered body with no binder or catalyst under a lower temperature condition by employing hexagonal boron nitride having a mean grain diameter of not more than 3 µm and keeping this raw material at a pressure of 6 GPa and a temperature of 1100°C. In this method, however, the raw material of hexagonal boron nitride consists of fine powder and contains several percent of a boron oxide impurity or adsorbed gas. Thus, sintering insufficiently progresses due to action of the impurity or adsorbed gas. Further, the cBN sintered body containing an oxide of boron is so reduced in hardness, strength and heat resistance that the same cannot be applied to a cutting tool. Accordingly, the present invention has been proposed in order to solve the aforementioned problems, and an object thereof is to provide a cBN sintered body having sufficient strength, hardness, heat resistance and heat dissipativity for serving as a cutting tool and a method of preparing the same. The method of preparing a cubic boron nitride sintered body according to the present invention comprises the steps of preparing low-pressure phase boron nitride serving as a starting material by reducing a compound containing boron and oxygen with a compound containing carbon and nitrogen, and directly converting the low-pressure phase boron nitride under a high temperature and a high pressure and simultaneously sintering the same for obtaining a cubic boron nitride sintered body. The low-pressure phase boron nitride (low-pressure phase BN) is boron nitride which is thermodynamically stable in a low pressure area, and includes hexagonal BN (hBN), rhombohedral BN (rBN), turbostratic BN (tBN) and amorphous BN (aBN). On the other hand, cBN, which is stable under a high pressure, is also called high-pressure phase BN. The feature of this method resides in that the low-pressure phase boron nitride serving as the starting material is hardly oriented and the diameter of crystal grains is not increased following a heat treatment under a high temperature. Therefore, the cBN sintered body obtained by directly converting the low-pressure phase boron nitride under a high temperature and a high pressure is hardly oriented, i.e., isotropic, and has a small diameter of crystal grains. Consequently, a cBN sintered body having sufficient strength and hardness for serving as a cutting tool can be obtained. The direct conversion to cubic boron nitride is preferably performed after heating the low-pressure phase boron nitride in a non-oxidative atmosphere at a temperature of the boiling point of the compound or at a temperature exceeding the boiling point of the compound containing boron and oxygen. In this case, the compound containing boron and oxygen or adsorbed gas is volatilized by heating, not to remain in the low-pressure phase boron nitride. Therefore, bonding strength between cBN grains is so increased that a cBN sintered body which is excellent not only in strength and hardness but in heat resistance and heat dissipativity for serving as a cutting tool can be obtained. Further, the compound containing boron and oxygen which inhibits the conversion to cBN is so volatilized that the low-pressure phase boron nitride is readily converted to cBN. Thus, no hBN remains in the cBN sintered body, dissimilarly to the case of the conventional direct conversion method. Consequently, a cBN sintered body having high strength can be obtained under mild temperature and pressure conditions. The low-pressure phase boron nitride preferably contains 0.08 to 1 percent by weight of oxygen. The oxygen content is set to be at least 0.08 percent by weight since the low-crystalline low-pressure phase BN according to the present invention contains less than 0.08 percent by weight of unremovable oxygen. The oxygen content is set to be not more than 1 percent by weight since low-pressure phase boron nitride containing oxygen in excess of 1 percent by weight is so hardly converted to cBN that unconverted low-pressure phase BN remains in the cBN sintered body to reduce its strength and hardness if such low-pressure phase BN is employed as the starting material. The direct conversion to the cubic boron nitride is preferably performed after heating powder of the low-pressure phase boron nitride in a non-oxidative atmosphere and thereafter forming the same to obtain a compact, and further heating this compact. In this case, adsorbed gas contained in the compact is removed due to the heating. Therefore, the bonding strength between the cBN grains is increased, to further improve the strength, hardness, heat resistance and heat dissipativity of cBN. The cubic boron nitride sintered body according to the present invention is obtained by directly converting low-pressure phase boron nitride under a high temperature and a high pressure and simultaneously sintering the same. This cubic boron nitride sintered body is isotropic since the ratio I 220 /I 111 of X-ray diffraction intensity I 220 on its (220) plane to X-ray diffraction intensity I 111 on the (111) plane is relatively large, whereby a cBN sintered body which is excellent in strength, hardness, heat resistance and heat dissipativity can be obtained. If the ratio I 220 /I 111 is less than 0.1, the cBN sintered body can be regarded as being strongly oriented in the <111> direction. Namely, the cBN sintered body is anisotropic in this case, and readily causes layer cracking or separation. The grain diameter of cubic boron nitride crystals contained in the cubic boron nitride sintered body is preferably not more than 1 µm. In this case, the strength of the cBN sintered body can be further increased due to the small diameter of the cBN crystals. If the grain diameter of the cubic boron nitride crystals exceeds 1 µm, transgranular fractures are so readily caused that the strength of the cBN sintered body is reduced. The hardness of the cubic boron nitride sintered body is preferably at least 4500 kg/mm 2 . The cubic boron nitride sintered body preferably has a heat-resistance temperature of at least 1200°C in a non-oxidative atmosphere. The foregoing and other objects, features, aspects and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken in conjunction with the accompanying drawing. Fig. 1 is a X-ray diffraction diagram of hBN serving as the raw material for the inventive cBN sintered body. Example 1 Boron oxide (B 2 O 3 ) and melamine (C 3 N 6 H 6 ) were blended in a mole ratio of 3:1, and homogeneously mixed with each other in a mortar. This mixture was introduced into a tube furnace and heat-treated at a temperature of 950°C for two hours in nitrogen gas, to obtain powder. This powder was washed with ethanol, to remove unreacted B 2 O 3 . Further, this powder was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas, to obtain powder of boron nitride. The oxygen content in this boron nitride powder measured by gas analysis was 0.66 percent by weight. The crystal structure of the boron nitride powder was investigated by x-ray diffraction. The X-ray source was prepared from a CuK α-ray source. The wavelength of the X-ray was 1.54 Å. Fig. 1 shows a diffraction line obtained by this X-ray diffraction. It is understood from Fig. 1 that no diffraction line was obtained from the (102) plane of hBN but a diffraction line corresponding to the (002) plane of hBN was extremely broad, and crystals were isotropically grown. Further, the half band width (W in Fig. 1, unit: degree) of the diffraction line corresponding to the (002) plane of hBN was obtained. The half band width W was substituted in the following equation (A), to obtain a radian half band width BM: BM = π 180 × W The radian half band width BM and a mechanical error BS (= 4.0 x 10 -3 ) were substituted in the following equation (B), to obtain a true half band width B: B = (BM) 2 - (BS) 2 From the true half band width B, the wavelength (λ = 1.54 Å) and the angle (half the value A in Fig. 1) causing the diffraction on the (002) plane, the diameter t of the crystal grains was calculated as following equation (C): t = 0.9λ Bcos The diameter t of the crystal grains calculated through the above equation was 13 nm. The powder of low-pressure phase BN synthesized in the aforementioned procedure was embossed under a pressure of 6 x 10 3 kgf/cm 2 , for preparing a compact of 8 mm in diameter and 3 mm in thickness. This compact was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas. Then, the compact was introduced into a capsule consisting of molybdenum (Mo), and kept at a pressure of 6.5 GPa and a temperature of 1850°C for 15 minutes in a belt type superhigh pressure generator, for obtaining a cBN sintered body. The structure of this sintered body was investigated by X-ray diffraction, to recognize that the same consisted of only cBN. In this X-ray diffraction, the ratio I 220 /I 111 of diffraction intensity I 220 on the (220) plane of cBN to diffraction intensity I 111 on the (111) plane of cBN was 0.18. Thus, it was recognized that the cBN sintered body was an isotropic sintered body having a small orientation property. Further, the fine structure of this cBN sintered body was observed with a transmisison electron microscope, to recognize that the diameter of the cBN crystal grains was about 0.5 µm and the sintered body consisted of fine crystals. It was also recognized through this observation that no impurity was present between the crystal grains, which were strongly bonded to each other. The hardness of the cBN sintered body was measured with a micro-Knoop indenter, to recognize that the same had high hardness of 5500 kg/mm 2 . Further, heat conductivity was measured by a laser flash method, to recognize that the cBN sintered body had high heat conductivity of about 6 W/cm•°C. In addition, heat resistance was evaluated by comparing the hardness before a heat treatment in a vacuum furnace with that after the heat treatment, to recognize that the cBN sintered body was stable up to a temperature of 1350°C and had high heat resistance. A cutting tool was prepared from the cBN sintered body obtained in the present invention, and subjected to an intermittent high-speed cutting test for cast iron. Further, a commercially available cutting tool consisting of a cBN sintered body prepared with a binder of Co was also subjected to an intermittent high-speed cutting test for cast iron. As a result, it was recognized that the life of the cutting tool prepared from the inventive cBN sintered body was 10 times that of the commercially available cutting tool. Example 2 While the mixture of boron oxide and melamine was heat-treated in the tube furnace at the temperature of 950°C for two hours in nitrogen gas in Example 1, a mixture of boron oxide and melamine was heat-treated in a tube furnace at a temperature of 850°C for two hours in nitrogen gas in Example 2. The remaining steps were similar to those of Example 1. The oxygen content of low-pressure phase BN powder obtained in this manner, measured by gas analysis, was 0.8 percent by weight. When the structure of the low-pressure phase BN powder was investigated by X-ray diffraction, no diffraction line was obtained fron the (102) plane of hBN but a diffraction line corresponding to the (002) plane of hBN was extremely broad in the X-ray diffraction diagram, and hence it was recognized that the diameter of low-pressure phase BN crystal grains forming the low-pressure phase BN powder was considerably small. The diameter t of the crystal grains obtained from a half band width of the diffraction line corresponding to the (002) plane of hBN through the above equations (A) to (C) was 8 nm. A cBN sintered body was prepared from the low-pressure phase BN obtained in the aforementioned manner, similarly to Example 1. The structure of the obtained cBN sintered body was investigated by X-ray diffraction, to recognize that the ratio I 220 /I 111 of diffraction intensity I 220 on the (220) plane of cBN to diffraction intensity I 111 on the (111) plane of cBN was 0.2, and the crystal grains forming the sintered body were isotropic. Further, this cBN sintered body exhibited a crystal grain diameter, hardness, heat conductivity and heat resistance which were similar to those in Example 1, and attained a result similar to that in Example 1 in an intermittent high-speed cutting test for cast iron. Example 3 While the mixture of boron oxide and melamine was heat-treated in the tube furnace at the temperature of 950°C for two hours in nitrogen gas in Example 1, a mixture of boron oxide and melamine was heat-treated in a tube furnace at a temperature of 1050°C for two hours in nitrogen gas in Example 3. The remaining steps were similar to those of Example 1. The oxygen content of low-pressure phase BN powder obtained in this manner, measured by gas analysis, was 0.2 percent by weight. When the crystal structure of the obtained low-pressure phase BN powder was investigated by X-ray diffraction, no diffraction line was obtained from the (102) plane of hBN but a diffraction line corresponding to the (002) plane of hBN was broad in the X-ray diffraction diagram, with low crystallinity. The diameter t of the crystal grains obtained from a half band width of the diffraction line corresponding to the (002) plane of hBN, the angle causing the diffraction and the wavelength of the X-ray was about 35 nm. The crystal structure of the low-pressure phase BN powder was observed with a scanning electron microscope, to recognize that the crystal grain diameter was 1 µm and the powder consisted of fine crystals. A cBN sintered body was prepared from this low-pressure phase BN, similarly to Example 1. The crystal structure of the obtained cBN sintered body was investigated by X-ray diffraction, to recognize that the ratio I 220 /I 111 of diffraction intensity I 220 on the (220) plane of cBN to diffraction intensity I 111 on the (111) plane of cBN was 0.12, and the crystals forming this cBN sintered body were isotropic. Further, this cBN sintered body exhibited hardness, heat conductivity, heat resistance and a crystal grain diameter which were similar to those in Example 1, and attained a result similar to that in Example 1 in an intermittent high-speed cutting test for cast iron. Example 4 While the compact of low-pressure phase BN was introduced into the molybdenum capsule and kept at the pressure of 6.5 GPa and the temperature of 1850°C for 15 minutes in the belt type superhigh pressure generator in Example 2, a compact consisting of low-pressure phase BN prepared similarly to Example 2 was introduced into a molybdenum capsule and kept at a pressure of 6 GPa and a temperature of 1550°C in a belt type superhigh pressure generator in Example 4. A cBN sintered body was prepared through remaining processes which were similar to those in Example 2. The characteristics and cutting performance of the cBN sintered body obtained in this manner were similar to those of the sintered body obtained in Example 2. Comparative Example 1 A commercially available compact of hBN was employed as a raw material. The grain diameter of this hBN compact was 3 to 10 µm. This compact was introduced into a high-frequency furnace and heat-treated at a temperature of 2100°C for two hours in nitrogen gas, to obtain a sample. The oxygen content of this sample measured by gas analysis was 0.03 percent by weight. The sample was introduced into a molybdenum capsule similarly to Example 1, and kept at a pressure of 6.5 GPa and a temperature of 1850°C for 15 minutes in a belt type superhigh pressure generator. The substance obtained in this manner was investigated, to recognize that the same was hardly sintered. The cBN content in this substance investigated by X-ray diffraction was about 10 percent by volume, and the remaining part of about 90 percent by volume was still hBN. Comparative Example 2 A commercially available compact of pBN was employed as a raw material. This compact was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas, to obtain a sample. The oxygen content of this sample measured by gas analysis was 0.02 percent by weight. The sample was introduced into a molybdenum capsule similarly to Example 1, and kept at a pressure of 6.5 GPa and a temperature of 1850°C for 15 minutes in a belt type superhigh pressure generator. The substance obtained in this manner was investigated, to recognize that the same was hardly sintered. The cBN content in this substance investigated by X-ray diffraction was about 90 percent by volume, while the remaining part of about 10 percent by volume consisted of compressed hBN. Comparative Example 3 A commercially available compact of hBN was employed as a raw material. The grain diameter of this hBN compact was 3 to 10 µm. This compact was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas, to obtain a sample. The oxygen content of this sample measured by gas analysis was 0.03 percent by weight. The sample was introduced into a molybdenum capsule, and kept at a pressure of 7.7 GPa and a temperature of 2200°C for 15 minutes in a belt type superhigh pressure generator, to obtain a strong cBN sintered body. The structure of this cBN sintered body was investigated by X-ray diffraction, to recognize that the ratio I 220 /I 111 of diffraction intensity I 220 on the (220) plane of cBN to diffraction intensity I 111 on the (111) plane of cBN was 0.06, and an anisotropic cBN sintered body selectively oriented in the <111> direction was obtained. It was also recognized that compressed hBN was present around a spacing d of 3.1 Å, although the amount thereof was small. The hardness of this cBN sintered body measured by a micro-Knoop indenter was 5000 kg/mm 2 . The heat conductivity of this cBN sintered body measured by a laser flash method was about 5.5 W/cm•°C. A cutting tool was prepared from this cBN sintered body, and subjected to an intermittent high-speed cutting test for cast iron similarly to Example 1. Although exhibited a life of about twice that of a tool consisting of a commercially available cBN sintered body, this cutting tool caused such chipping that its cutting edge was conceivably separated in layers. Comparative Example 4 A commercially available compact of pBN was employed as a raw material. This compact was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas, to obtain a sample. The oxygen content of this sample measured by gas analysis was 0.02 percent by weight. The sample was introduced into a molybdenum capsule, and kept at a pressure of 7.5 GPa and a temperature of 2100°C for 15 minutes in a belt type superhigh pressure generator, to obtain a strong cBN sintered body. The structure of this cBN sintered body was investigated by X-ray diffraction, to recognize that a diffraction line from the (220) plane of cBN was hardly observed and the ratio I 220 /I 111 of diffraction intensity I 220 on the (220) plane of cBN to diffraction intensity I 111 on the (111) plane of cBN was substantially zero. Thus, it was recognized that this cBN sintered body was selectively oriented in the <111> direction and had extremely strong anisotropy. It was also recognized that compressed hBN was present around a spacing d of 3.1 Å through the X-ray diffraction. The hardness of this cBN sintered body was 4000 kg/mm 2 . Further, the heat conductivity of this sintered body measured by a laser flash method was about 4.5 W/cm•°C. When a cutting tool was prepared from this cBN sintered body and subjected to an intermittent high-speed cutting test for cast iron, its cutting edge was instantaneously chipped. The damaged cutting edge exhibited a number of parts separated in layers. Comparative Example 5 B 2 O 3 was reacted with ammonia to synthesize low-crystalline low-pressure phase BN for serving as a raw material. The diameter of crystal grains forming this raw material was 0.5 µm. The composition of this raw material was analyzed, to recognize that the same contained about 3 percent by weight of B 2 O 3 . The raw material was heat-treated in a high-frequency furnace at a temperature of 2100°C for two hours in nitrogen gas, for removing this B 2 O 3 . The oxygen content was reduced to about 0.1 percent by weight due to the heat treatment, while crystal grains of hBN were grown into a diameter of 3 to 5 µm. While preparation of a cBN sintered body from the raw material was attempted similarly to Example 1, the hBN was not converted to cBN and no strong cBN sintered body was obtained at all.

Claims: A method of preparing a cubic boron nitride sintered body comprising the steps of: preparing low-pressure phase boron nitride serving as a starting material by reducing a compound containing boron and oxygen with a compound containing carbon and nitrogen; and directly converting said low-pressure phase boron nitride under a high temperature and a high pressure and simultaneously sintering the same for obtaining a cubic boron nitride sintered body. A method as claimed in claim 1, wherein direct conversion to said cubic boron nitride is performed after heating said low-pressure phase boron nitride in a non-oxidative atmosphere at a temperature of the boiling point of said compound containing boron and oxygen or at a temperature exceeding the boiling point of said compound containing boron and oxygen. A method as claimed in claim 1 or claim 2, wherein said low-pressure phase boron nitride contains 0.08 to 1 percent by weight of oxygen. A method as claimed in any one of the preceding claims, wherein direct conversion to said cubic boron nitride is performed after heating powder of said low-pressure phase boron nitride in a non-oxidative atmosphere, thereafter forming the same to obtain a compact, and further heating said compact. A method as claimed in any one of the preceding claims which includes the further step of preparing a cutting tool from the cubic boron nitride sintered body. A cubic boron nitride sintered body prepared by directly converting low-pressure phase boron nitride under a high temperature and a high pressure and simultaneously sintering the same, wherein the ratio (I 220 /I 111 ) of X-ray diffraction intensity (I 220 ) on the (220) plane of said cubic boron nitride sintered body to the X-ray diffraction intensity (I 111 ) on the (111) plane is at least 0.1. A cubic boron nitride sintered body as claimed in claim 6, wherein the grain diameter of cubic boron nitride crystals forming said cubic boron nitride sintered body is not more than 1 µm. A cubic boron nitride sintered body as claimed in claim 6 or claim 7, having a hardness of at least 4500 kg/mm 2 . A cubic boron nitride sintered body as claimed in any one of claims 6 to 8 having a heat-resistance temperature of at least 1200°C in a non-oxidative atmosphere. A cutting tool comprising a cubic boron nitride sintered body as claimed in any one of claims 6 to 9.

Inventors: SUMIYA HITOSHI, SUMIYA, HITOSHI
Applicants: SUMITOMO ELECTRIC INDUSTRIES, SUMITOMO ELECTRIC INDUSTRIES, LTD.
Application year: 1997
Main classification: C04B35
IPC codes: C04B35