Patent Application
20120264596
1. Field of the Invention
The present invention relates to a honeycomb structure and a method of manufacturing a honeycomb structure.
2. Discussion of the Background
A large number of techniques have been developed in relation to conversion of exhaust gas of automobiles or the like. With an increase in traffic, however, countermeasures taken against exhaust gas have hardly been satisfactory. Not only in Japan but also globally, is emission control of automobiles or the like going to be further tightened.
In order to meet such control of exhaust gas, catalyst supports capable of treating predetermined toxic components contained in exhaust gas are used in exhaust gas converting systems. Further, a honeycomb structure is known as a member for such catalyst supports.
This honeycomb structure has, for example, multiple cells (through holes) extending from one end face to another end face of the honeycomb structure along its longitudinal directions, and these cells are separated from each other by cell walls on which a catalyst is supported. Accordingly, in the case of causing exhaust gas to flow through such a honeycomb structure, substances contained in the exhaust gas, such as HC (a hydrocarbon compound), CO (carbon monoxide), and NOx (nitrogen oxides), are converted (oxidized or reduced) by the catalyst supported on the cell walls, so that these toxic components in the exhaust gas may be treated.
In general, the cell walls (base material) of such a honeycomb structure are formed of cordierite. Further, a catalyst support layer of γ-alumina is formed on the cell walls, and a noble metal catalyst such as platinum and/or rhodium is supported on this catalyst support layer.
Further, a technique has been proposed that, in order to improve conversion performance at exhaust gas temperatures lower than a temperature at which a catalyst becomes active, uses a honeycomb structure of a relatively low electrical resistance, provides this honeycomb structure with electrodes for applying voltage, and supplies the honeycomb structure with electric current, thereby causing the honeycomb structure to perform self-heating (JP 07-80226 A).
For example, JP 07-80226 A discloses that by adding silicon carbide particles and particles of a compound containing nitride to raw material in manufacturing a silicon-carbide-based honeycomb structure, it is possible to reduce the electrical resistivity of a honeycomb structure to be finally obtained.
The entire contents of JP 07-80226 A are incorporated herein by reference.
According to one aspect of the present invention, a honeycomb structure includes a substantially pillar-shaped honeycomb unit having cells defined by cell walls. The cell walls include silicon carbide particles having a nitrogen-containing layer provided on surfaces of the silicon carbide particles.
In addition, according to another aspect of the present invention, a method of manufacturing a honeycomb structure includes preparing paste containing silicon carbide particles. The paste is molded to form a honeycomb molded body. The honeycomb molded body is fired in an inert atmosphere containing no nitrogen to obtain a substantially pillar-shaped honeycomb unit having cells defined by cell walls. The honeycomb unit is heated in an environment containing nitrogen to provide a nitrogen-containing layer on surfaces of the silicon carbide particles forming the cell walls.
A more complete appreciation of the invention and many of the attendant advantages thereof will be readily obtained as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings.
According to the conventional honeycomb structure described in JP 07-80226 A, it is likely to be possible to reduce the finally obtained honeycomb structure in electrical resistivity. Therefore, by supplying the honeycomb structure with electric current via a pair of electrodes, it is likely to be possible to subject the honeycomb structure to resistance heating.
In general, however, the electrical resistivity of a resistor is a function of temperature and tends to change with an increase in temperature. Accordingly, it is believed that in the conventional honeycomb structure described in JP 07-80226 A as well, the electrical resistivity is likely to change with temperature and, in particular, to decrease sharply with an increase in temperature.
On the other hand, in the case of using a honeycomb structure as an exhaust gas converting apparatus, the temperature of the honeycomb structure varies in a wide range from room temperature (for example, approximately 25° C.) to approximately 500° C.
According to an embodiment of the present invention, it is possible to obtain a honeycomb structure in which the temperature change dependence of electrical resistivity is controlled. Further, it is possible to obtain a method of manufacturing such a honeycomb structure.
The embodiments will now be described with reference to the accompanying drawings, wherein like reference numerals designate corresponding or identical elements throughout the various drawings.
As illustrated in
The honeycomb unit 130 includes multiple cells (through holes) 122 and cell walls 124 defining the cells 122. The cells 122 extend from the end face 110A to the end face 110B along the longitudinal directions of the honeycomb unit 130 to be open at the end faces 110A and 110B.
The honeycomb unit 130 is formed of, for example, a material having silicon carbide (SiC) as a principal component. The honeycomb unit 130 contains a resistance adjusting component in order to reduce electrical resistivity. The resistance adjusting component is nitrogen atoms (N) with which the silicon carbide is doped. That is, the cell walls 124 of the honeycomb unit 130 contain silicon carbide, and a nitrogen-containing layer is formed on the surface of the silicon carbide. A catalyst is supported on the cell walls 124 of the honeycomb unit 130.
Further, in the case of
The first electrode 160A is provided entirely around a first end part 115A of the honeycomb unit 130. The second electrode 160B is provided entirely around a second end part 115B of the honeycomb unit 130. However, the positions where these electrodes 160A and 160B are provided are examples, and the electrodes 160A and 160B may be provided at other positions in the honeycomb structure 100.
The honeycomb structure 100 may be subjected to resistance heating by externally applying voltage between the electrodes 160A and 160B in the honeycomb structure 100 thus configured.
Here, for example, in the conventional honeycomb structure of a resistance heating type described in JP 07-80226 A, a compound having a low specific resistance value is added to raw material containing silicon carbide particles in order to reduce the electrical resistivity of the honeycomb structure. In this case, a component (low resistance component) contained in the added compound is evenly diffused in the silicon carbide particles during the firing of the raw material, so that it is possible to dispose the low resistance component throughout cell walls in a honeycomb unit to be finally obtained. This is likely to make it possible to reduce the electrical resistivity of the honeycomb unit.
In general, however, the electrical resistivity of a resistor is a function of temperature and tends to change with an increase in temperature. Accordingly, it is believed that in the conventional honeycomb structure described in JP 07-80226 A as well, the electrical resistivity is likely to change with temperature and, in particular, to decrease sharply with an increase in temperature.
On the other hand, in the case of using a honeycomb structure as an exhaust gas converting apparatus, the temperature of the honeycomb structure varies in a wide range from room temperature (for example, approximately 25° C.) to approximately 500° C. Accordingly, even if the honeycomb structure has an electrical resistivity in an appropriate range in a certain temperature region, a change in the temperature of the honeycomb structure is likely to cause a change in the electrical resistivity, so that the electrical resistivity is likely to go out of the appropriate range. Specifically, if a honeycomb structure has an electrical resistivity in an appropriate range in a certain temperature region, an increase in the temperature of the honeycomb structure is likely to cause a decrease in the electrical resistivity. It is believed that as a result, the electrical resistivity is likely to go out of the appropriate range, thus causing a problem in that it is difficult to properly heat the honeycomb structure.
On the other hand, in the honeycomb structure 100 according to the embodiment of the present invention, a layer containing nitrogen atoms (hereinafter referred to as “nitrogen-containing layer”) is present on the surfaces of silicon carbide particles that form the cell walls 124. That is, it is believed that according to the embodiment of the present invention, nitrogen atoms that contribute to the electrical resistivity of a honeycomb unit are present in a concentrated state on the surfaces of silicon carbide particles, so that inside the silicon carbide particles, the nitrogen atoms are absent or present at a lower concentration than on the surfaces of the silicon carbide particles.
By thus disposing nitrogen atoms in a concentrated state on the surfaces of silicon carbide particles, it is likely to be possible to control the temperature dependence of the electrical resistivity of a honeycomb unit.
In
As illustrated in
On the other hand, in the case where the concentration of nitrogen atoms is high, a donor band is formed instead of the donor level. Further, as illustrated in
The donor level represents the energy level of electrons present in a band gap, and the donor band represents a group of electron orbits formed by the density of a large number of electrons present at the donor level in the band gap.
According to the embodiment of the present invention, a “nitrogen-containing layer” is present on the surfaces of silicon carbide particles, that is, nitrogen atoms are concentrated on the surfaces of silicon carbide particles. It is believed that this causes the energy state of nitrogen to be as illustrated in
This principle has been thought out by the inventor of the present invention based on the present knowledge, and it is to be noted that the temperature dependence of the electrical resistivity of a honeycomb unit may also be controlled for other reasons in a configuration of the embodiment of the present invention.
Further, the presence of such a nitrogen-containing layer may be determined by scanning nonlinear dielectric microscopy (SNDM).
SNDM, which is one of the measurement methods based on scanning probe microscopy (SPM), is a technique that measures a change in polarity and a concentration distribution of carriers on the surface of a sample based on the charge sign of a probe and the magnitude of an electric field caused upon application of voltage to the probe brought close to the surface of the sample. SNDM is used in, for example, the measurement of a concentration distribution of semiconductor carriers, etc.
Here, according to the embodiment of the present invention, the thickness of the nitrogen-containing layer is, for example, in the range of approximately 100 nm to approximately 600 nm, preferably in the range of approximately 200 nm to approximately 600 nm, and more preferably, in the range of approximately 200 nm to approximately 400 nm.
If the thickness of the nitrogen-containing layer is more than or equal to approximately 100 nm, the electrical resistivity of a honeycomb unit is less likely to be reduced. As a result, the amount of electric conduction between electrodes is less likely to be reduced, so that it is likely to be possible to heat the honeycomb unit to an appropriate temperature. On the other hand, if the thickness of the nitrogen-containing layer is less than or equal to approximately 600 nm, the electrical resistivity of a honeycomb unit is less likely to have temperature dependence, so that the electrical resistivity of the honeycomb unit is less likely to decrease at the time of high temperatures in particular. Therefore, it is likely to be possible to heat the honeycomb unit to an appropriate temperature.
The nitrogen-containing layer tends to be oxidized by long-term use at high temperatures. Progress in the oxidation of the nitrogen-containing layer is likely to impair the control effect of the nitrogen-containing layer on the temperature dependence of electrical resistivity.
In order to address this problem, it is preferable to provide a silica layer as a protection layer on the surface of the nitrogen-containing layer. This silica layer improves the long-term stability of the nitrogen-containing layer and is likely to make it possible to maintain the control effect on the temperature dependence of electrical resistivity over a long period of time.
The thickness of the silica layer is, for example, in the range of approximately 100 nm to approximately 800 nm, preferably in the range of approximately 100 nm to approximately 500 nm, and more preferably, in the range of approximately 200 nm to approximately 500 nm.
If the thickness of the silica layer is more than or equal to approximately 100 nm, it is easy to sufficiently prevent oxidation of the nitrogen-containing layer, so that the oxidation of the nitrogen-containing layer is less likely to progress. On the other hand, if the thickness of the silica layer is less than or equal to approximately 800 nm, a stress due to a difference in the coefficient of thermal expansion between the silica layer and the silicon carbide particles is less likely to increase, so that the silica layer is less likely to peel off the silicon carbide particles. As a result, the temperature dependence of electrical resistivity is likely to be controlled.
It is possible to form such a silica layer easily by, for example, adding metal Si (silicon) particles to the surfaces of the silicon carbide particles of the cell walls of a honeycomb unit and thereafter oxidizing the metal Si (silicon) by heating the honeycomb unit.
The honeycomb structure 100 illustrated in
As illustrated in
The honeycomb structure 200 is formed by joining multiple honeycomb units by interposing an adhesive layer 250. For example, in the case illustrated in
However, the honeycomb units 230A through 230D contain a resistance adjusting component in order to reduce electrical resistivity. The resistance adjusting component is nitrogen atoms (N) with which the silicon carbide is doped.
As illustrated in
In the case of
The honeycomb unit 230A includes multiple cells 222 and cell walls 224 defining the cells 222. The cells 222 extend from the end face 214A to the end face 214B along the longitudinal directions of the honeycomb unit 230A to be open at the end faces 214A and 214B. A catalyst is supported on the cell walls 224 of the honeycomb unit 230A.
As described above, the cell walls 224 of the honeycomb unit 230A are formed of silicon carbide particles, and a nitrogen-containing layer is formed on the surfaces of the silicon carbide particles. A silica layer may be formed on the surface of the nitrogen-containing layer.
It is clear to a person having ordinary skill in the art that the above-described effects according to the embodiment of the present invention are also produced by the honeycomb structure 200 including this honeycomb unit 230A.
A pair of electrodes is not illustrated in the honeycomb structure 200 illustrated in
Next, a description is given in more detail of a configuration of each of members of a honeycomb structure according to the embodiment of the present invention. In the following, a description is given principally of members of the honeycomb structure 200 having the aggregated structure illustrated in
The honeycomb unit 230A is formed of an inorganic material based on silicon carbide (SiC), and contains, as a resistance adjusting component, nitrogen atoms (N) with which the silicon carbide (SiC) is doped.
The cross-sectional shape of the honeycomb unit 230A perpendicular to its longitudinal directions is not limited in particular, and may be any shape such as a substantially square shape, a substantially rectangular shape, a substantially hexagonal shape or the like.
Further, the cross-sectional shape of the cells 222 of the honeycomb unit 230A perpendicular to its longitudinal directions is not limited in particular, and may be, for example, a substantially triangular shape, a substantially polygonal shape or the like in addition to a substantially square shape.
The cell density of the honeycomb unit 230A is preferably approximately 15.5 cells/cm2 to approximately 186 cells/cm2 (approximately 100 cpsi to approximately 1200 cpsi), more preferably approximately 31 cells/cm2 to approximately 155 cells/cm2 (approximately 200 cpsi to approximately 1000 cpsi), and still more preferably approximately 46.5 cells/cm2 to approximately 124 cells/cm2 (approximately 300 cpsi to approximately 800 cpsi).
If the cell density of the honeycomb unit 230A is more than or equal to approximately 15.5 cells/cm2, the cell walls 224 are less likely to have a reduced area of contact with exhaust gas, so that sufficient conversion performance is likely to be obtained. On the other hand, if the cell density of the honeycomb unit 230A is less than or equal to approximately 186 cells/cm2, the pressure of a honeycomb structure is less likely to increase.
The porosity of the honeycomb unit 230A may be in the range of approximately 15% to approximately 50%.
If the porosity of the honeycomb unit 230A is more than or equal to approximately 15%, the elastic modulus of the honeycomb unit 230A is less likely to increase, so that the honeycomb unit 230A is less likely to be broken because of a stress generated at the time of its energization. On the other hand, if the porosity of the honeycomb unit 230A is less than or equal to approximately 50%, the strength of the cell walls 224 of the honeycomb unit 230A is less likely to be reduced.
The thickness of the cell walls 224 of the honeycomb unit 230A is not limited in particular. However, a desirable lower limit is approximately 0.05 mm in terms of strength, and a desirable upper limit is approximately 0.3 mm in terms of conversion performance.
The catalyst supported on the cell walls 224 of the honeycomb unit 230A is not limited in particular, and may be, for example, platinum, rhodium, palladium or the like. The catalyst may be supported on the cell walls 224 by interposing an aluminum layer.
The adhesive layer 250 of the honeycomb structure 200 is formed using adhesive layer paste as raw material. The adhesive layer paste may contain inorganic particles, an inorganic binder, inorganic fibers, and/or an organic binder.
Silicon carbide (SiC) is desirable as inorganic particles of the adhesive layer paste. Inorganic sol, a clay-based binder or the like may be used as the inorganic binder. Examples of the inorganic sol include alumina sol, silica sol, titania sol, water glass and the like. Examples of the clay-based binder include clay, kaolin, montmonrillonite, sepiolite, attapulgite and the like. These may be used alone or in combination. Alumina, silica, silicon carbide, silica-alumina, glass, potassium titanate, aluminum borate or the like is preferable as the material of the inorganic fibers. These may be used alone or in combination. Of the above-described materials of the inorganic fibers, silica-alumina is desirable.
The organic binder is not limited in particular, and is, for example, one or more selected from polyvinyl alcohol, methylcellulose, ethylcellulose, carboxymethylcellulose and the like. Of the organic binders, carboxymethylcellulose is desirable.
The thickness of the adhesive layer 250 is preferably in the range of approximately 0.3 mm to approximately 2 mm. If the thickness of the adhesive layer 250 is more than or equal to approximately 0.3 mm, the joining strength of honeycomb units is likely to be sufficient. If the thickness of the adhesive layer 250 is less than or equal to approximately 2 mm, the pressure loss of the honeycomb structure is less likely to increase. The number of honeycomb units to be joined is suitably determined in accordance with the size of the honeycomb structure.
A honeycomb structure according to the embodiment of the present invention may have any shape. For example, in addition to a substantially circular-pillar shape illustrated in
Next, a description is given of a method of manufacturing a honeycomb structure according to the embodiment of the present invention. The following description is given, taking the case of manufacturing the honeycomb structure 100 illustrated in
(a) the step of preparing paste containing silicon carbide particles (step S110);
(b) the step of forming a honeycomb molded body by molding the paste (step S120);
(c) the step of obtaining a substantially pillar-shaped honeycomb unit having cells defined by cell walls by firing the molded body in an inert atmosphere containing no nitrogen (step S130);
(d) the step of forming a nitrogen-containing layer on the surfaces of the silicon carbide particles forming the cell walls by heating the honeycomb unit in an environment containing nitrogen (step S140);
(e) the step of forming a silica layer on the nitrogen-containing layer (step S150); and
(f) the step of causing a catalyst to be supported on the cell walls (step S160).
Step S150 of (e) and/or step S160 of (f) may be omitted.
Further, the method of manufacturing a honeycomb structure according to the embodiment of the present invention may have the step of joining multiple honeycomb units by interposing an adhesive layer.
A description is given below of each of the steps.
First, raw material paste having silicon carbide (SiC) as a principal component is prepared.
Apart from silicon carbide (SiC) particles, an organic binder, a dispersion medium, a molding aid (for example, molding lubricant, molding plasticizer or the like) and the like may be suitably added to the raw material paste.
The organic binder is not limited in particular, and may be one or more kinds of organic binders selected from, for example, methylcellulose, carboxymethylcellulose, hydroxyethylcellulose, polyethylene glycol, phenolic resin, epoxy resin and the like. The amount of the organic binder blended is preferably approximately 1 part by weight to approximately 10 parts by weight to the total of 100 parts by weight of the inorganic particles.
The dispersion medium is not limited in particular, and may be, for example, water, an organic solvent (such as benzene), alcohol (such as methanol) or the like.
The molding aid is not limited in particular, and may be, for example, ethylene glycol, dextrin, a fatty acid, fatty acid soap, polyalcohol or the like, where two or more kinds of molding aids may be blended. Of these molding aids, a fatty acid is desirable. Further, the fatty acid is preferably an unsaturated fatty acid, and more desirably a higher fatty acid. The higher fatty acid desirably has a carbon number more than or equal to 15 and less than 65.
The raw material paste is not limited to this, and is preferably subjected to mixing and kneading. For example, the raw material paste may be mixed using a mixer, an attritor or the like, and may be well kneaded with a kneader or the like.
Next, a honeycomb molded body is formed by molding the raw material paste prepared in step S110.
The method of molding a honeycomb molded body is not limited in particular. For example, a honeycomb molded body having multiple cells is molded from the raw material paste by extrusion molding or the like.
Thereafter, the obtained honeycomb molded body is preferably dried. The drying apparatus used for drying is not limited in particular, and may be a microwave drying apparatus, a hot air drying apparatus, a dielectric drying apparatus, a reduced-pressure drying apparatus, a vacuum drying apparatus, a freeze drying apparatus or the like. Further, the obtained dried honeycomb molded body is preferably degreased. The conditions for degreasing, which are not limited in particular and are suitably selected in accordance with the kind and amount of the organic matter included in the molded body, are preferably approximately 400° C. and approximately 2 hours in the rough.
Next, the obtained dried honeycomb molded body is fired (first heat treatment). The conditions for firing are not limited in particular. It is preferable to perform firing for approximately 1 hour to approximately 5 hours at approximately 2000° C. to approximately 2200° C.
The atmosphere for firing needs to be an inert atmosphere containing no nitrogen, such as an argon atmosphere or the like. This is because if firing is performed in an environment containing nitrogen, a nitrogen component in the environment is likely to be captured through gas phase diffusion into sintered silicon carbide particles during the sintering of the silicon carbide particles, which makes it difficult to cause nitrogen to be present only on the surfaces of silicon carbide particles forming cell walls in a honeycomb unit to be finally obtained.
Next, in order to form a nitrogen-containing layer on the surfaces of the silicon carbide particles, the honeycomb fired body obtained in step S130 is subjected to heat treatment (second heat treatment).
This second heat treatment is performed in an environment containing nitrogen. The second heat treatment is preferably performed in the temperature range of approximately 1800° C. to approximately 2200° C., and more preferably, in the range of approximately 1800° C. to approximately 2000° C. The second heat treatment is preferably performed for approximately 2 hours to approximately 8 hours.
If the temperature of the second heat treatment is more than or equal to approximately 1800° C., nitrogen atoms (N) are likely to diffuse onto the surfaces of the silicon carbide particles, so that a nitrogen-containing layer is likely to be formed. If the temperature of the second heat treatment is less than or equal to approximately 2200° C., the sintering of the silicon carbide particles is less likely to progress. Therefore, nitrogen atoms (N) are less likely to diffuse into sintered silicon carbide particles through gas phase diffusion, so that it is possible to have nitrogen atoms (N) present only on the surfaces of the silicon carbide particles.
Through the above-described processes, it is possible to obtain a honeycomb unit having a nitrogen-containing layer on the surfaces of silicon carbide particles.
Next, if needed, a silica layer is further formed on the surfaces of the silicon carbide particles of the honeycomb unit obtained in step S140.
The method of forming a silica layer is not limited in particular. The silica layer may be formed by, for example, coating the surface of the nitrogen-containing layer with silicon by adding metal Si (silicon) particles to the surface of the honeycomb unit and oxidizing the metal Si (silicon) by heating the honeycomb unit.
The method of adding metal Si (silicon) particles to the surface of the honeycomb unit is, for example, immersing the honeycomb unit in molten silicon, or the like. Further, the method of oxidizing metal Si (silicon) particles added to the surfaces of the silicon carbide particles of the honeycomb unit is, for example, subjecting the honeycomb unit to heat treatment in an oxidizing atmosphere, or the like. In this case, the temperature of heat treatment is preferably in the range of approximately 1000° C. to approximately 1400° C., and the time of heat treatment is preferably in the range of approximately 1 hour to approximately 10 hours.
If the temperature of heat treatment is more than or equal to approximately 1000° C., the metal Si (silicon) particles are likely to be sufficiently oxidized, so that it is possible to have a silica layer formed on the surfaces of the silicon carbide particles. On the other hand, if the temperature of heat treatment is less than or equal to approximately 1400° C., the metal Si (silicon) particles are less likely to melt, so that it is possible to have a silica layer formed on the surfaces of the silicon carbide particles.
Through the above-described process, it is possible to manufacture a honeycomb unit having a silica layer further formed on the nitrogen-containing layer.
In the case of using the honeycomb unit as a honeycomb structure of a resistance heating type, the honeycomb unit is provided with a pair of electrodes. This process is preferably performed before the above-described step (e) (step S150) after the above-described step (d) (step S140). Alternatively, this process may be performed after cutting the silica layer where the electrodes are to be provided after the above-described step (e) (step S150).
The positions where electrodes are provided are not limited in particular. The electrodes are preferably provided one on each end portion of the honeycomb unit entirely around the end portion or at least on the curved side so as to facilitate attachment of terminals and supply of electric current.
The electrodes are formed of metal or the like. Further, the electrodes may be provided by, for example, metal spraying, metal sputtering, metal vapor deposition or the like.
In the method of manufacturing a honeycomb structure according to the embodiment of the present invention, the step of causing a catalyst to be supported on the cell walls of the honeycomb unit may be further performed after the above-described step (d) (step S140) or the above-described step (e) (step S150).
In particular, in the case of using the honeycomb unit as a honeycomb structure for a catalyst support, a catalyst is supported on the cell walls of the honeycomb unit.
For example, platinum, rhodium, palladium or the like may be used as the catalyst. The method of causing a catalyst to be supported is not limited in particular. The catalyst may be supported by interposing an alumina layer.
The method of manufacturing a honeycomb structure according to the embodiment of the present invention may have the step of joining multiple honeycomb units by interposing an adhesive layer (joining process).
For example, in the case of manufacturing a honeycomb structure of the aggregated structure, multiple honeycomb units obtained with the above-described method are joined by interposing an adhesive layer.
This joining process is performed after the above-described step (d) (step S140). In particular, considering the heat resistance of the inorganic fibers contained in the adhesive layer, the joining process is performed after the above-described step (e) (step S150) if the method of manufacturing a honeycomb structure according to the embodiment of the present invention includes the above-described step (e) (step S150) (silica layer forming process). Further, if the method of manufacturing a honeycomb structure according to the embodiment of the present invention includes the above-described step (f) (step S160) (catalyst supporting process), the joining process is performed before the above-described step (f) (step S160). Further, if the method of manufacturing a honeycomb structure according to the embodiment of the present invention includes the above-described step (e) (step S150) (silica layer forming process) and the above-described step (f) (step S160) (catalyst supporting process), the joining process is performed between the above-described step (e) (step S150) and the above-described step (f) (step S160).
Next, a description is given of examples according to the embodiment of the present invention.
A honeycomb unit was manufactured in the following manner, and a change in the electrical resistivity of the honeycomb unit due to temperature was evaluated.
First, raw material paste for molding a honeycomb unit was prepared. The raw material paste was prepared by mixing 690 g of an organic binder (methylcellulose), 115 g of a molding lubricant (UNILUB), 115 g of a molding plasticizer (glycerin), and 1600 g of ion-exchanged water with 1000 g of silicon carbide particles.
Next, the obtained raw material paste was subjected to extrusion molding using a screw molding machine, thereby manufacturing a honeycomb molded body of 10 mm square and 50 mm long. The cell walls of the honeycomb molded body were 0.2 mm in thickness, and the cell density of the honeycomb molded body was 600 cpsi.
Next, the obtained honeycomb molded body was fired at 2200° C. for 3 hours in an argon atmosphere, so that a honeycomb fired body was obtained (first heat treatment). The obtained honeycomb fired body (also referred to as honeycomb unit) has an average porosity of 45% and an average pore size of 11 μm.
Next, this honeycomb fired body was subjected to heat treatment at 1900° C. for 8 hours in a nitrogen atmosphere (second heat treatment).
The honeycomb unit thus obtained is referred to as “honeycomb unit according to Example 1.”
The surfaces of silicon carbide particles contained in the cell walls of the honeycomb unit according to Example 1 were observed by SNDM.
Specifically, silicon carbide particles were observed with a voltage of 4 V applied to a probe, and such an image as to allow determination of the variation of carrier concentration was captured.
As a result of the measurement, the thickness of the nitrogen-containing layer was 300 nm.
A honeycomb unit according to Example 2 was manufactured in the same manner as in Example 1. In Example 2, however, the honeycomb unit obtained in Example 1 (hereinafter referred to as “honeycomb unit having a nitrogen-containing layer”) was further subjected to the following treatment, so that a silica layer was formed on the surfaces of the silicon carbide particles.
First, the entire “honeycomb unit having a nitrogen-containing layer” was immersed in a bath of aqueous liquid containing metal Si (silicon) particles, so that the metal Si (silicon) particles were added to the surfaces of the silicon carbide particles.
Next, this “honeycomb unit having a nitrogen-containing layer” was dried and was thereafter heated at 1200° C. for 1 hour in the atmosphere.
As a result, a silica layer was formed on the surfaces of the silicon carbide particles (technically, the surface of the nitrogen-containing layer). The silica layer was 500 nm in thickness. The thickness of the nitrogen-containing layer hardly changed through this heat treatment, and was 300 nm.
The thickness of the silica layer was measured with a transmission electron microscope.
A honeycomb unit according to Comparative Example 1 was manufactured in the same manner as in Example 1. In Comparative Example 1, however, the “first heat treatment” was performed at 2200° C. for 3 hours in a nitrogen atmosphere. Further, the “second heat treatment” was not performed in Comparative Example 1.
The surfaces of silicon carbide particles contained in the cell walls of the honeycomb unit according to Comparative Example 1 were observed by SNDM. As a result, no nitrogen-containing layer was formed on the surfaces of the silicon carbide particles.
The configurations (the presence or absence of a nitrogen-containing layer and the presence or absence of a silica layer) of the honeycomb units according to Example 1, Example 2, and Comparative Example 1 are collectively illustrated in Table 1.
The following evaluation of a change in electrical resistivity due to temperature was performed using the honeycomb units of Example 1, Example 2, and Comparative Example 1 manufactured in the above-described manner.
A change in the electrical resistivity of each honeycomb unit due to temperature was measured. The measurement was performed through the following steps.
First, silver paste was applied entirely around each end portion (10 mm in width) of each of the honeycomb units of Example 1 and Comparative Example 1 as electrodes. Further, a platinum line was connected to each of the electrodes.
On the other hand, the silica layer was cut off entirely around each end portion (10 mm in width) of the honeycomb unit of Example 2 using sandpaper, and thereafter, silver paste was applied as electrodes to where the silica layer had been cut off. Further, in Example 2 as well, a platinum line was connected to each of the electrodes the same as in Example 1 and Comparative Example 1.
As described above, samples for evaluating a change in electrical resistivity due to temperature with respect to Example 1, Example 2, and Comparative Example 1 (hereinafter referred to as evaluation samples) were manufactured.
Next, a constant-voltage power supply unit was connected between the electrodes of each of the evaluation samples, and a voltage of 200 V was applied between the electrodes. In this state, the electrical resistivities of the evaluation samples were measured. Thereafter, the evaluation samples were heated to temperatures (up to 550° C.), and the electrical resistivities of the evaluation samples were measured in the same manner.
The measurement results of the evaluation samples of the honeycomb unit according to Example 1 and the honeycomb unit according to Comparative Example 1 are collectively illustrated in
This graph of
Thus, it has been confirmed that the temperature dependence of electrical resistivity is likely to be significantly controlled in the honeycomb unit manufactured with the method of manufacturing a honeycomb structure according to the embodiment of the present invention.
In Table 1 described above, the results (the results of the evaluation of a change in electrical resistivity due to temperature) obtained in the honeycomb units according to Example 1, Example 2, and Comparative Example 1 are collectively illustrated.
Next, changes in electrical resistivity over time in an environment closer to actual installation in vehicles were measured using the honeycomb units according to Example 1 and Example 2. In the case of the honeycomb unit according to Comparative Example 1, it was confirmed in “Evaluation of Changes in Electrical Resistivity due to Temperature” described above that the electrical resistivity presents high temperature dependence. Therefore, this evaluation was not performed with respect to the honeycomb unit according to Comparative Example 1. Further, the electrical resistivity was measured using evaluation samples the same as in the case of “Evaluation of Changes in Electrical Resistivity due to Temperature” described above.
The measurement was performed at 1000° C. in the atmosphere, and the electrical resistivity was measured for up to 100 hours.
The results of the evaluation of changes in electrical resistivity in an accelerated environment are illustrated in
The results of the evaluation of changes in electrical resistivity in an accelerated environment are illustrated in Table 1.
As illustrated in the graph of
Accordingly, in the case of using a honeycomb structure for a long period of time at high temperatures, the durability of the nitrogen-containing layer is believed to be further improved by further forming a silica layer on the nitrogen-containing layer. Further, this is likely to make it possible to control the temperature dependence of electrical resistivity over a long period of time.
The electrical resistivity of Example 1 in the accelerated environment presents a sharp change. The accelerated environment implemented in this test is believed to have severe conditions of high temperature and high oxygen concentration compared with those of a practical usage environment. Therefore, it is believed that even the configuration of Example 1 is sufficiently usable for practical applications.
Further, the evaluation of changes in electrical resistivity due to temperature and the evaluation of changes in electrical resistivity in an accelerated environment were performed using evaluation samples. It is believed, however, that substantially the same results are obtained as well with evaluations using honeycomb structures according to the embodiment of the present invention.
Obviously, numerous modifications and variations of the present invention are possible in light of the above teachings. It is therefore to be understood that within the scope of the appended claims, the invention may be practiced otherwise than as specifically described herein.
| Number | Date | Country | Kind |
|---|---|---|---|
| PCT/JP2011/059211 | Apr 2011 | JP | national |
The present application is based upon and claims priority under 35 U.S.C. §119 to PCT International Application No. PCT/JP2011/059211, filed on Apr. 13, 2011, the entire contents of which are incorporated herein by reference.
