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Electrical Properties of Boron Nitride Matrix Composites: I, Analysis of McLachlan Equation and Modeling of the Conductivity of Boron Nitride-Boron Carbide and Boron Nitride-Silicon Carbide Composites
The McLachlan equation, which incorporates both effective medium models and percolation, was used to predict the volume fraction–conductivity relationships of insulator–conductor composites, and results were compared with experimental data. Two composite systems were investigated (BN–B4C and BN–SiC)...
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Published in: | Journal of the American Ceramic Society 2001-07, Vol.84 (7), p.1490-1496 |
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creator | Runyan, Julie Gerhardt, Rosario A. Ruh, Robert |
description | The McLachlan equation, which incorporates both effective medium models and percolation, was used to predict the volume fraction–conductivity relationships of insulator–conductor composites, and results were compared with experimental data. Two composite systems were investigated (BN–B4C and BN–SiC). Both systems are anisotropic, because of the orientation of BN platelets perpendicular to the hot‐pressing direction. For BN–B4C composites, with increasing B4C content, the ac and dc conductivities are relatively constant to ∼40% B4C (the critical volume fraction). At this composition, the conductivity suddenly increases to a value closer to that of B4C and then resumes a gradual increase. Little difference is seen for measurements made perpendicular or parallel to the hot‐pressing direction, i.e., perpendicular or parallel to the BN platelets. Similar results are found for the BN–SiC composites, except that the critical volume fraction is ∼20% SiC in this case. The experimental curves are in good agreement with those predicted by the McLachlan equation. The parameters s and t of the McLachlan equation relate to the morphology of the phases present in the microstructure. The critical volume fraction relates to the connectivity of the phases in the composites. |
doi_str_mv | 10.1111/j.1151-2916.2001.tb00866.x |
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Two composite systems were investigated (BN–B4C and BN–SiC). Both systems are anisotropic, because of the orientation of BN platelets perpendicular to the hot‐pressing direction. For BN–B4C composites, with increasing B4C content, the ac and dc conductivities are relatively constant to ∼40% B4C (the critical volume fraction). At this composition, the conductivity suddenly increases to a value closer to that of B4C and then resumes a gradual increase. Little difference is seen for measurements made perpendicular or parallel to the hot‐pressing direction, i.e., perpendicular or parallel to the BN platelets. Similar results are found for the BN–SiC composites, except that the critical volume fraction is ∼20% SiC in this case. The experimental curves are in good agreement with those predicted by the McLachlan equation. The parameters s and t of the McLachlan equation relate to the morphology of the phases present in the microstructure. 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Two composite systems were investigated (BN–B4C and BN–SiC). Both systems are anisotropic, because of the orientation of BN platelets perpendicular to the hot‐pressing direction. For BN–B4C composites, with increasing B4C content, the ac and dc conductivities are relatively constant to ∼40% B4C (the critical volume fraction). At this composition, the conductivity suddenly increases to a value closer to that of B4C and then resumes a gradual increase. Little difference is seen for measurements made perpendicular or parallel to the hot‐pressing direction, i.e., perpendicular or parallel to the BN platelets. Similar results are found for the BN–SiC composites, except that the critical volume fraction is ∼20% SiC in this case. The experimental curves are in good agreement with those predicted by the McLachlan equation. The parameters s and t of the McLachlan equation relate to the morphology of the phases present in the microstructure. The critical volume fraction relates to the connectivity of the phases in the composites.</description><subject>boron nitride</subject><subject>ceramic matrix composites</subject><subject>Composite materials</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>conductivity</subject><subject>Conductivity of specific materials</subject><subject>Conductivity phenomena in semiconductors and insulators</subject><subject>electrical properties</subject><subject>Electronic transport in condensed matter</subject><subject>Exact sciences and technology</subject><subject>Physics</subject><issn>0002-7820</issn><issn>1551-2916</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqVUdFu0zAUjRCTKIN_sBDiiXR2nNjJnuii0g21A2lDSHux7hybuaRxZ7us_cN91pylgiFewC9XV-fcc3zvSZI3BI9JfEfLWAqSZhVh4wxjMg7XGJeMjbfPkhEp9tDzZIQxzlJeZvhF8tL7ZWxJVeaj5H7aKhmckdCiL86ulQtGeWQ1OrHOdujcRLBRaAGxblFtV2vrTVD-GJ29R5MO2p03j_yFnIO8aaFD09sNBBOHoWvQwjaqNd33nhJuVFTomo0M5qcJu79s0qGrwV33pv38n_iFaY18wvj9n1fJgYbWq9f7eph8_Ti9rE_T-efZWT2ZpzLPOU4JyxhVmOeswhyKeINcM86AKmiwUg3nlEOZQcEIyWnJK011obSGkua6qYAeJu8G3bWztxvlg1gZL1UbF1d240XGOMcMs38hsoLSLBKPB6J01nuntFg7swK3EwSLPmWxFH3Koo9S9CmLfcpiG4ff7l3Axwy1g04a_0SBxSV6jw8D7c60avcfBuLTpJ6SvMJRIh0kjA9q-0sC3A_B4tEK8e18Jsrs6gJfnl6JGX0AUU7ODQ</recordid><startdate>200107</startdate><enddate>200107</enddate><creator>Runyan, Julie</creator><creator>Gerhardt, Rosario A.</creator><creator>Ruh, Robert</creator><general>American Ceramics Society</general><general>Blackwell</general><scope>BSCLL</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7SR</scope><scope>JG9</scope></search><sort><creationdate>200107</creationdate><title>Electrical Properties of Boron Nitride Matrix Composites: I, Analysis of McLachlan Equation and Modeling of the Conductivity of Boron Nitride-Boron Carbide and Boron Nitride-Silicon Carbide Composites</title><author>Runyan, Julie ; Gerhardt, Rosario A. ; Ruh, Robert</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4470-16263e0746907a59844f676a3ead0eed7737a82a561143879f3f5effa834fd9a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>boron nitride</topic><topic>ceramic matrix composites</topic><topic>Composite materials</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>conductivity</topic><topic>Conductivity of specific materials</topic><topic>Conductivity phenomena in semiconductors and insulators</topic><topic>electrical properties</topic><topic>Electronic transport in condensed matter</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Runyan, Julie</creatorcontrib><creatorcontrib>Gerhardt, Rosario A.</creatorcontrib><creatorcontrib>Ruh, Robert</creatorcontrib><collection>Istex</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Engineered Materials Abstracts</collection><collection>Materials Research Database</collection><jtitle>Journal of the American Ceramic Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Runyan, Julie</au><au>Gerhardt, Rosario A.</au><au>Ruh, Robert</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electrical Properties of Boron Nitride Matrix Composites: I, Analysis of McLachlan Equation and Modeling of the Conductivity of Boron Nitride-Boron Carbide and Boron Nitride-Silicon Carbide Composites</atitle><jtitle>Journal of the American Ceramic Society</jtitle><date>2001-07</date><risdate>2001</risdate><volume>84</volume><issue>7</issue><spage>1490</spage><epage>1496</epage><pages>1490-1496</pages><issn>0002-7820</issn><eissn>1551-2916</eissn><coden>JACTAW</coden><abstract>The McLachlan equation, which incorporates both effective medium models and percolation, was used to predict the volume fraction–conductivity relationships of insulator–conductor composites, and results were compared with experimental data. Two composite systems were investigated (BN–B4C and BN–SiC). Both systems are anisotropic, because of the orientation of BN platelets perpendicular to the hot‐pressing direction. For BN–B4C composites, with increasing B4C content, the ac and dc conductivities are relatively constant to ∼40% B4C (the critical volume fraction). At this composition, the conductivity suddenly increases to a value closer to that of B4C and then resumes a gradual increase. Little difference is seen for measurements made perpendicular or parallel to the hot‐pressing direction, i.e., perpendicular or parallel to the BN platelets. Similar results are found for the BN–SiC composites, except that the critical volume fraction is ∼20% SiC in this case. The experimental curves are in good agreement with those predicted by the McLachlan equation. The parameters s and t of the McLachlan equation relate to the morphology of the phases present in the microstructure. The critical volume fraction relates to the connectivity of the phases in the composites.</abstract><cop>Westerville, Ohio</cop><pub>American Ceramics Society</pub><doi>10.1111/j.1151-2916.2001.tb00866.x</doi><tpages>7</tpages></addata></record> |
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subjects | boron nitride ceramic matrix composites Composite materials Condensed matter: electronic structure, electrical, magnetic, and optical properties conductivity Conductivity of specific materials Conductivity phenomena in semiconductors and insulators electrical properties Electronic transport in condensed matter Exact sciences and technology Physics |
title | Electrical Properties of Boron Nitride Matrix Composites: I, Analysis of McLachlan Equation and Modeling of the Conductivity of Boron Nitride-Boron Carbide and Boron Nitride-Silicon Carbide Composites |
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