Optimum Shapes for Inductors
The concept of optimum shape of inductors is discussed. The optimum shape is defined to be that of the inductor which has the smallest volume for a given set of electrical specifications. This definition has the widest application and can be used to calculate the optimum shape. A dimensionless funct...
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Veröffentlicht in: | IEEE transactions on parts, materials, and packaging materials, and packaging, 1969-03, Vol.5 (1), p.3-15, Article 3 |
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creator | Astle, B. |
description | The concept of optimum shape of inductors is discussed. The optimum shape is defined to be that of the inductor which has the smallest volume for a given set of electrical specifications. This definition has the widest application and can be used to calculate the optimum shape. A dimensionless function of the proportions of the inductor is related to the definition and is used to calculate the optimum shapes of three types of core: toroidal, E, and pot cores. Equations are developed to help the reader calculate the optimum shapes of other types of core. |
doi_str_mv | 10.1109/TPMP.1969.1136053 |
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The optimum shape is defined to be that of the inductor which has the smallest volume for a given set of electrical specifications. This definition has the widest application and can be used to calculate the optimum shape. A dimensionless function of the proportions of the inductor is related to the definition and is used to calculate the optimum shapes of three types of core: toroidal, E, and pot cores. Equations are developed to help the reader calculate the optimum shapes of other types of core.</description><identifier>ISSN: 0018-9502</identifier><identifier>EISSN: 1558-2655</identifier><identifier>DOI: 10.1109/TPMP.1969.1136053</identifier><language>eng</language><publisher>IEEE</publisher><subject>Conducting materials ; Conductors ; Equations ; Frequency ; Inductors ; Inorganic materials ; Magnetic cores ; Permeability ; Shape ; Transformer cores</subject><ispartof>IEEE transactions on parts, materials, and packaging, 1969-03, Vol.5 (1), p.3-15, Article 3</ispartof><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c265t-5bcc98028d845316fddfb8074e43816000a8a8489665a9ce32227f01c92c7d123</citedby><cites>FETCH-LOGICAL-c265t-5bcc98028d845316fddfb8074e43816000a8a8489665a9ce32227f01c92c7d123</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1136053$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/1136053$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Astle, B.</creatorcontrib><title>Optimum Shapes for Inductors</title><title>IEEE transactions on parts, materials, and packaging</title><addtitle>T-CPM</addtitle><description>The concept of optimum shape of inductors is discussed. The optimum shape is defined to be that of the inductor which has the smallest volume for a given set of electrical specifications. This definition has the widest application and can be used to calculate the optimum shape. A dimensionless function of the proportions of the inductor is related to the definition and is used to calculate the optimum shapes of three types of core: toroidal, E, and pot cores. Equations are developed to help the reader calculate the optimum shapes of other types of core.</description><subject>Conducting materials</subject><subject>Conductors</subject><subject>Equations</subject><subject>Frequency</subject><subject>Inductors</subject><subject>Inorganic materials</subject><subject>Magnetic cores</subject><subject>Permeability</subject><subject>Shape</subject><subject>Transformer cores</subject><issn>0018-9502</issn><issn>1558-2655</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1969</creationdate><recordtype>article</recordtype><recordid>eNp9j11LwzAUhoMoWKc_QPSif6DznKRJk0sZfgwmGzivQ5YmWFnXkmQX_ntbVhC88Orwcnjel4eQW4Q5IqiH7eZtM0cl1BCZAM7OSIacy4IKzs9JBoCyUBzoJbmK8QuAlgogI_frPjXtsc3fP03vYu67kC8P9dGmLsRrcuHNPrqb6c7Ix_PTdvFarNYvy8XjqrBDeyr4zlolgcpalpyh8HXtdxKq0pVMogAAI40spRKCG2Udo5RWHtAqaqsaKZsRPPXa0MUYnNd9aFoTvjWCHvX0qKdHPT3pDUz1h7FNMqnpDimYZv8veXciG-fc79L0_QET_FtY</recordid><startdate>196903</startdate><enddate>196903</enddate><creator>Astle, B.</creator><general>IEEE</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>196903</creationdate><title>Optimum Shapes for Inductors</title><author>Astle, B.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c265t-5bcc98028d845316fddfb8074e43816000a8a8489665a9ce32227f01c92c7d123</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1969</creationdate><topic>Conducting materials</topic><topic>Conductors</topic><topic>Equations</topic><topic>Frequency</topic><topic>Inductors</topic><topic>Inorganic materials</topic><topic>Magnetic cores</topic><topic>Permeability</topic><topic>Shape</topic><topic>Transformer cores</topic><toplevel>online_resources</toplevel><creatorcontrib>Astle, B.</creatorcontrib><collection>CrossRef</collection><jtitle>IEEE transactions on parts, materials, and packaging</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Astle, B.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optimum Shapes for Inductors</atitle><jtitle>IEEE transactions on parts, materials, and packaging</jtitle><stitle>T-CPM</stitle><date>1969-03</date><risdate>1969</risdate><volume>5</volume><issue>1</issue><spage>3</spage><epage>15</epage><pages>3-15</pages><artnum>3</artnum><issn>0018-9502</issn><eissn>1558-2655</eissn><abstract>The concept of optimum shape of inductors is discussed. The optimum shape is defined to be that of the inductor which has the smallest volume for a given set of electrical specifications. This definition has the widest application and can be used to calculate the optimum shape. A dimensionless function of the proportions of the inductor is related to the definition and is used to calculate the optimum shapes of three types of core: toroidal, E, and pot cores. Equations are developed to help the reader calculate the optimum shapes of other types of core.</abstract><pub>IEEE</pub><doi>10.1109/TPMP.1969.1136053</doi><tpages>13</tpages></addata></record> |
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source | IEEE Electronic Library (IEL) |
subjects | Conducting materials Conductors Equations Frequency Inductors Inorganic materials Magnetic cores Permeability Shape Transformer cores |
title | Optimum Shapes for Inductors |
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