{"id":709,"date":"2026-03-22T19:13:49","date_gmt":"2026-03-22T19:13:49","guid":{"rendered":"https:\/\/www.parthasarathimishra.com\/wordpress\/?p=709"},"modified":"2026-03-22T19:25:36","modified_gmt":"2026-03-22T19:25:36","slug":"capacitance-of-an-asymmetric-capacitor","status":"publish","type":"post","link":"https:\/\/www.parthasarathimishra.com\/wordpress\/capacitance-of-an-asymmetric-capacitor\/","title":{"rendered":"Capacitance of an Asymmetric Capacitor"},"content":{"rendered":"\n<p>Capacitors which were formerly called condensers, were always build with plates of same physical dimensions in order to satisfy Maxwellian electrodynamics and predictable outcome. But asymmetric capacitors are not much discussed in mainstream due to no direct benefit in existing technologies as well as design complexities.<br><br>This post derives the capacitance of the asymmetric parallel plate capacitor.<\/p>\n\n\n\n<p>Let there be and parallel plate asymmetric capacitor as shows below in fig 1. The dielectric material be increasing in width like a cone as shown guiding the electric displacement expanding from one plate to another.<br><\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"489\" height=\"524\" src=\"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-content\/uploads\/2026\/03\/asymmetric_capacitor.png\" alt=\"\" class=\"wp-image-710\" srcset=\"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-content\/uploads\/2026\/03\/asymmetric_capacitor.png 489w, https:\/\/www.parthasarathimishra.com\/wordpress\/wp-content\/uploads\/2026\/03\/asymmetric_capacitor-280x300.png 280w\" sizes=\"(max-width: 489px) 100vw, 489px\" \/><figcaption class=\"wp-element-caption\">Fig 1<\/figcaption><\/figure><\/div>\n\n\n<p>The area of two plates be<strong> A<sub>1<\/sub><\/strong> and <strong>A<sub>2<\/sub><\/strong>. Let\u2019s assume them to be squares with sides 2h<sub>1<\/sub> and 2h<sub>2<\/sub> respectively, separated by a distance d. The areas of the two plates are:<\/p>\n\n\n\n<p><\/br><span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} A_{1} = 4 h_{1}^{2} \\end{aligned}\\end{equation}<\/span><\/br><span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} A_{2} = 4 h_{2}^{2} \\end{aligned}\\end{equation}<\/span><\/p>\n\n\n\n<p>To calculate the capacitance, let\u2019s take a small section of the dielectric at distance <em>x<\/em> from A<sub>1<\/sub> with its height y from the horizontal line making the imaginary plate size as <em>2y<\/em> and the separation between them as <em>dx<\/em>. The area of the abstract symmetric parallel plate capacitor as A<sub>x<\/sub>.<br><br>We need to calculated the capacitance of the imaginary small subtract capacitance element and add all of them in series in order to get the actual capacitance.<\/p>\n\n\n\n<p>From similarity we have,<\/p>\n\n\n\n<p><span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} \\frac{h_{2} - h_{1}}{d} = \\frac{y - h_{1}}{x} \\end{aligned}\\end{equation}<\/span>\nor, <span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned}y = h_{1} + \\frac{x}{d}\\left( h_{2} - h_{1} \\right)\\end{aligned}\\end{equation}<\/span>\n<\/p>\n\n\n\n<p>Now area A<sub>x<\/sub> is:<\/p>\n\n\n\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} A_{x} = 4 y^{2} \\end{aligned}\\end{equation}<\/span>\n<p>\nor, <span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned}A_{x} = 4 \\left[ h_{1} + \\frac{x}{d}\\left( h_{2} - h_{1} \\right) \\right]^{2} \\end{aligned}\\end{equation}<\/span>\n<\/p>\n\n\n\n<p>So, capacitance <em>dC<sub>x<\/sub><\/em> of the parallel plate capacitor is:<\/p>\n\n\n\n<p><span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} dC_{x} = \\frac{\\epsilon A_{x}}{dx} \\end{aligned}\\end{equation}<\/span><\/br>\nor, <span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} dC_{x} = \\frac{4 \\epsilon \\left[ h_{1} + \\frac{x}{d}\\left( h_{2} - h_{1} \\right) \\right]^{2}}{dx} \\end{aligned}\\end{equation}<\/span><\/p>\n\n\n\n<p>So total capacitance C in series becomes:<\/p>\n\n\n\n<p>\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} \\frac{1}{C} =\\int_{0}^{d}\\frac{1}{dC_{x}} = \\int_{0}^{d}\\frac{dx}{4 \\epsilon \\left[ h_{1} + \\frac{x}{d}\\left( h_{2} - h_{1} \\right) \\right]^{2}}\\end{aligned}\\end{equation}<\/span>\n<\/pr>\n\n\n\n<p>Now replacing,<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} h_{1} + \\frac{x}{d}\\left( h_{2} - h_{1} \\right)  = u\\end{aligned}\\end{equation}<\/span><\/br>\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned}dx  = \\frac{d}{\\left( h_{2} - h_{1} \\right)} du\\end{aligned}\\end{equation}<\/span><\/br>\nThe integral becomes<\/br>\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} \\frac{1}{C} &amp; = \\frac{d}{4\\epsilon}\\int_{h_{1}}^{h_{2}} \\frac{du}{\\left( h_{2} - h_{1} \\right) u^{2}} \\\\&amp; =\\frac{d}{4\\epsilon \\left( h_{2} - h_{1} \\right)} \\left[ \\frac{1}{h_{1}}  -\\frac{1}{h_{2}}\\right] \\\\&amp;  =\\frac{d}{4\\epsilon h_{1} h_{2}}  \\end{aligned}\\end{equation}\n<\/span>\n<\/p>\n\n\n\n<p><\/br>Hence,<\/br>\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned}C &amp; = \\frac{4\\epsilon h_{1} h_{2}}{d} \\\\&amp; = \\frac{\\epsilon \\sqrt{A_{1}A_{2}}}{d} \\end{aligned}\\end{equation} <\/span><\/br>\n<\/p>\n\n\n\n<p>So as you can see, for a parallel plate capacitor, A<sub>1<\/sub> = A<sub>2<\/sub> and the above equation becomes<\/p>\n\n\n\n<span class=\"katex-eq\" data-katex-display=\"true\">\\begin{equation}\\begin{aligned} C = \\frac{\\epsilon A}{d} \\end{aligned}\\end{equation}<\/span>\n","protected":false},"excerpt":{"rendered":"<p>Capacitors which were formerly called condensers, were always build with plates of same physical dimensions in order to satisfy Maxwellian electrodynamics and predictable outcome. But asymmetric capacitors are not much discussed in mainstream due to no direct benefit in existing technologies as well as design complexities. This post derives the capacitance of the asymmetric parallel [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"_links":{"self":[{"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/posts\/709"}],"collection":[{"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/comments?post=709"}],"version-history":[{"count":10,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/posts\/709\/revisions"}],"predecessor-version":[{"id":720,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/posts\/709\/revisions\/720"}],"wp:attachment":[{"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/media?parent=709"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/categories?post=709"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.parthasarathimishra.com\/wordpress\/wp-json\/wp\/v2\/tags?post=709"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}