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Dielectric Breakdown of Thinned BaO-Al2O3-B2O3-SiO2 Glass
The dielectric breakdown behavior of alkali‐free glass was determined as a function of thickness and surface roughness. The thickness of commercially available glass (as‐received thickness=50 μm) was reduced to a range of thicknesses between 47 and 5 μm by chemical etching. The RMS surface roughness...
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Published in: | Journal of the American Ceramic Society 2010-08, Vol.93 (8), p.2346-2351 |
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creator | Lee, Hoikwan Smith, Nicholas J. Pantano, Carlo G. Furman, Eugene Lanagan, Michael T. |
description | The dielectric breakdown behavior of alkali‐free glass was determined as a function of thickness and surface roughness. The thickness of commercially available glass (as‐received thickness=50 μm) was reduced to a range of thicknesses between 47 and 5 μm by chemical etching. The RMS surface roughness of the as‐received glass was in the range of 0.14–0.47 nm, and the surface roughness increased to up 10 nm after etching; it was also found that agitating the etching solution by ultrasound reduced the overall surface roughness. The evaluation of these samples revealed that the dielectric breakdown strength increased as the thickness decreased. However, the Weibull modulus representing the distribution of dielectric strengths showed a dependence on the surface roughness of the etched glass. A power law dependence, EB∝d−n, where d is the glass thickness and n=0.14 and 0.86, has been found to fit the data in the respective thickness ranges of 5–20 and 25–50 μm. Self‐healing behavior, which allows the dielectric to continue to support a high electric field after breakdown, was found to be more likely as the dielectric layer thickness decreased. The susceptibility to self healing was correlated with the stored electrostatic energy and latent heat of vaporization for the gold electrode material. |
doi_str_mv | 10.1111/j.1551-2916.2010.03749.x |
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The thickness of commercially available glass (as‐received thickness=50 μm) was reduced to a range of thicknesses between 47 and 5 μm by chemical etching. The RMS surface roughness of the as‐received glass was in the range of 0.14–0.47 nm, and the surface roughness increased to up 10 nm after etching; it was also found that agitating the etching solution by ultrasound reduced the overall surface roughness. The evaluation of these samples revealed that the dielectric breakdown strength increased as the thickness decreased. However, the Weibull modulus representing the distribution of dielectric strengths showed a dependence on the surface roughness of the etched glass. A power law dependence, EB∝d−n, where d is the glass thickness and n=0.14 and 0.86, has been found to fit the data in the respective thickness ranges of 5–20 and 25–50 μm. Self‐healing behavior, which allows the dielectric to continue to support a high electric field after breakdown, was found to be more likely as the dielectric layer thickness decreased. The susceptibility to self healing was correlated with the stored electrostatic energy and latent heat of vaporization for the gold electrode material.</description><identifier>ISSN: 0002-7820</identifier><identifier>EISSN: 1551-2916</identifier><identifier>DOI: 10.1111/j.1551-2916.2010.03749.x</identifier><language>eng</language><publisher>Malden, USA: Blackwell Publishing Inc</publisher><subject>Dielectric breakdown ; Dielectric strength ; Electric fields ; Electrode materials ; Electrostatics ; Etching ; Glass ; Surface roughness ; Vaporization</subject><ispartof>Journal of the American Ceramic Society, 2010-08, Vol.93 (8), p.2346-2351</ispartof><rights>2010 The American Ceramic Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27903,27904</link.rule.ids></links><search><creatorcontrib>Lee, Hoikwan</creatorcontrib><creatorcontrib>Smith, Nicholas J.</creatorcontrib><creatorcontrib>Pantano, Carlo G.</creatorcontrib><creatorcontrib>Furman, Eugene</creatorcontrib><creatorcontrib>Lanagan, Michael T.</creatorcontrib><title>Dielectric Breakdown of Thinned BaO-Al2O3-B2O3-SiO2 Glass</title><title>Journal of the American Ceramic Society</title><description>The dielectric breakdown behavior of alkali‐free glass was determined as a function of thickness and surface roughness. The thickness of commercially available glass (as‐received thickness=50 μm) was reduced to a range of thicknesses between 47 and 5 μm by chemical etching. The RMS surface roughness of the as‐received glass was in the range of 0.14–0.47 nm, and the surface roughness increased to up 10 nm after etching; it was also found that agitating the etching solution by ultrasound reduced the overall surface roughness. The evaluation of these samples revealed that the dielectric breakdown strength increased as the thickness decreased. However, the Weibull modulus representing the distribution of dielectric strengths showed a dependence on the surface roughness of the etched glass. A power law dependence, EB∝d−n, where d is the glass thickness and n=0.14 and 0.86, has been found to fit the data in the respective thickness ranges of 5–20 and 25–50 μm. Self‐healing behavior, which allows the dielectric to continue to support a high electric field after breakdown, was found to be more likely as the dielectric layer thickness decreased. The susceptibility to self healing was correlated with the stored electrostatic energy and latent heat of vaporization for the gold electrode material.</description><subject>Dielectric breakdown</subject><subject>Dielectric strength</subject><subject>Electric fields</subject><subject>Electrode materials</subject><subject>Electrostatics</subject><subject>Etching</subject><subject>Glass</subject><subject>Surface roughness</subject><subject>Vaporization</subject><issn>0002-7820</issn><issn>1551-2916</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><recordid>eNqFkF1PwjAUhhujiYj-h93pTWc_1_XKACJq0MU49bLpti4WxqYrBPj3dmC41F6c03P65kn6ABBgFGJ_rmch5hxDInEUEuS3iAomw80R6B0ejkEPIUSgiAk6BWfOzfyIZcx6QN5aU5l82do8GLZGz4tmXQdNGaSftq5NEQx1AgcVSSgcduXVJiSYVNq5c3BS6sqZi9_eB29343R0D6fJ5GE0mEJLhJAwL6kWmsesLDXjkjNecoxMnBWloAL7XWRoFmmuMyoLQ5nOcMao72VOJeG0Dy733K-2-V4Zt1QL63JTVbo2zcqpmEkm_H-YT179mcSRJFQyGtP_oySmkaSMd9SbfXRtK7NVX61d6HarMFKdfzVTnWbVaVadf7XzrzbqcTAa7-6eAPcE65ZmcyDodq4i74Crj-eJSt_Tl5Q8cTWlPwtWhwE</recordid><startdate>201008</startdate><enddate>201008</enddate><creator>Lee, Hoikwan</creator><creator>Smith, Nicholas J.</creator><creator>Pantano, Carlo G.</creator><creator>Furman, Eugene</creator><creator>Lanagan, Michael T.</creator><general>Blackwell Publishing Inc</general><scope>BSCLL</scope><scope>7QF</scope><scope>7QQ</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope></search><sort><creationdate>201008</creationdate><title>Dielectric Breakdown of Thinned BaO-Al2O3-B2O3-SiO2 Glass</title><author>Lee, Hoikwan ; Smith, Nicholas J. ; Pantano, Carlo G. ; Furman, Eugene ; Lanagan, Michael T.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i2779-cf3a7a584ffa459545f510e8bdf7371a456e3b6a5ab39de34ab1b4334afc39253</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>Dielectric breakdown</topic><topic>Dielectric strength</topic><topic>Electric fields</topic><topic>Electrode materials</topic><topic>Electrostatics</topic><topic>Etching</topic><topic>Glass</topic><topic>Surface roughness</topic><topic>Vaporization</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lee, Hoikwan</creatorcontrib><creatorcontrib>Smith, Nicholas J.</creatorcontrib><creatorcontrib>Pantano, Carlo G.</creatorcontrib><creatorcontrib>Furman, Eugene</creatorcontrib><creatorcontrib>Lanagan, Michael T.</creatorcontrib><collection>Istex</collection><collection>Aluminium Industry Abstracts</collection><collection>Ceramic Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</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>Lee, Hoikwan</au><au>Smith, Nicholas J.</au><au>Pantano, Carlo G.</au><au>Furman, Eugene</au><au>Lanagan, Michael T.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dielectric Breakdown of Thinned BaO-Al2O3-B2O3-SiO2 Glass</atitle><jtitle>Journal of the American Ceramic Society</jtitle><date>2010-08</date><risdate>2010</risdate><volume>93</volume><issue>8</issue><spage>2346</spage><epage>2351</epage><pages>2346-2351</pages><issn>0002-7820</issn><eissn>1551-2916</eissn><abstract>The dielectric breakdown behavior of alkali‐free glass was determined as a function of thickness and surface roughness. The thickness of commercially available glass (as‐received thickness=50 μm) was reduced to a range of thicknesses between 47 and 5 μm by chemical etching. The RMS surface roughness of the as‐received glass was in the range of 0.14–0.47 nm, and the surface roughness increased to up 10 nm after etching; it was also found that agitating the etching solution by ultrasound reduced the overall surface roughness. The evaluation of these samples revealed that the dielectric breakdown strength increased as the thickness decreased. However, the Weibull modulus representing the distribution of dielectric strengths showed a dependence on the surface roughness of the etched glass. A power law dependence, EB∝d−n, where d is the glass thickness and n=0.14 and 0.86, has been found to fit the data in the respective thickness ranges of 5–20 and 25–50 μm. Self‐healing behavior, which allows the dielectric to continue to support a high electric field after breakdown, was found to be more likely as the dielectric layer thickness decreased. The susceptibility to self healing was correlated with the stored electrostatic energy and latent heat of vaporization for the gold electrode material.</abstract><cop>Malden, USA</cop><pub>Blackwell Publishing Inc</pub><doi>10.1111/j.1551-2916.2010.03749.x</doi><tpages>6</tpages></addata></record> |
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subjects | Dielectric breakdown Dielectric strength Electric fields Electrode materials Electrostatics Etching Glass Surface roughness Vaporization |
title | Dielectric Breakdown of Thinned BaO-Al2O3-B2O3-SiO2 Glass |
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