<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-09-19T10:19:05Z</responseDate><request verb="GetRecord" identifier="oai:dspace.mit.edu:1721.1/40933" metadataPrefix="dim">https://dspace.mit.edu/server/oai/request</request><GetRecord><record><header><identifier>oai:dspace.mit.edu:1721.1/40933</identifier><datestamp>2022-01-13T07:54:36Z</datestamp><setSpec>com_1721.1_7582</setSpec><setSpec>com_1721.1_7581</setSpec><setSpec>col_1721.1_131024</setSpec></header><metadata><dim:dim xmlns:dim="http://www.dspace.org/xmlns/dspace/dim" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://www.dspace.org/xmlns/dspace/dim http://www.dspace.org/schema/dim.xsd">
   <dim:field mdschema="dc" element="contributor" qualifier="advisor" lang="en_US">Emanuel M. Sachs.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="author" lang="en_US">Winiarz, Christine Eve</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="other" lang="en_US">Massachusetts Institute of Technology. Dept. of Mechanical Engineering.</dim:field>
   <dim:field mdschema="dc" element="contributor" qualifier="department">Massachusetts Institute of Technology. Department of Mechanical Engineering</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="accessioned">2008-03-27T18:24:57Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="available">2008-03-27T18:24:57Z</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="copyright" lang="en_US">2007</dim:field>
   <dim:field mdschema="dc" element="date" qualifier="issued" lang="en_US">2007</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="uri">http://hdl.handle.net/1721.1/40933</dim:field>
   <dim:field mdschema="dc" element="identifier" qualifier="oclc" lang="en_US">212409308</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Thesis (S.B.)--Massachusetts Institute of Technology, Dept. of Mechanical Engineering, 2007.</dim:field>
   <dim:field mdschema="dc" element="description" lang="en_US">Includes bibliographical references (p. 31).</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="abstract" lang="en_US">Bus bars on solar cells shade silicon from light. When the bus bars are patterned, they can reflect light back onto the silicon using total internal reflection. These patterned bus bars are tin plated and produce 1-2.5% improvement in module efficiency [6]. There is a potential for even greater improvement by using higher reflectivity metal plating on the bus bars. Silver is the most reflective of all metals, but is also very expensive. We tested to see if silver would actually be as reflective as published values and if silver could redirect a substantial amount of light using total internal reflection. We found that silver plating followed the published spectral dependence curve with little deviation, and would reflect 18.4% more light than the published values for tin. Plating 2.24 microns resulted in 94.9% of reflected light undergoing TIR; the most reflected light of any tested material. Finally, given the current cost of silver is $430 per kilogram and the variable cost of a solar cell is $2 per Watt, the maximum allowable thickness we could afford to plate is 44.8 microns. In our testing, plating as little as 0.35 microns produced a very high light capture. The benefit of silver plating patterned bus bars far outweighs the material costs.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="statementofresponsibility" lang="en_US">by Christine Eve Winiarz.</dim:field>
   <dim:field mdschema="dc" element="description" qualifier="degree" lang="en_US">S.B.</dim:field>
   <dim:field mdschema="dc" element="format" qualifier="extent" lang="en_US">31 p.</dim:field>
   <dim:field mdschema="dc" element="language" qualifier="iso" lang="en_US">eng</dim:field>
   <dim:field mdschema="dc" element="publisher" lang="en_US">Massachusetts Institute of Technology</dim:field>
   <dim:field mdschema="dc" element="rights" lang="en_US">M.I.T. theses are protected by &#xd;
copyright. They may be viewed from this source for any purpose, but &#xd;
reproduction or distribution in any format is prohibited without written &#xd;
permission. See provided URL for inquiries about permission.</dim:field>
   <dim:field mdschema="dc" element="rights" qualifier="uri" lang="en_US">http://dspace.mit.edu/handle/1721.1/7582</dim:field>
   <dim:field mdschema="dc" element="subject" lang="en_US">Mechanical Engineering.</dim:field>
   <dim:field mdschema="dc" element="title" lang="en_US">Measurement of light capture in solar cells from silver- and tin-plated patterned bus bars</dim:field>
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   	&lt;Title>Measurement of light capture in solar cells from silver- and tin-plated patterned bus bars&lt;/Title>
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   	&lt;PublicationDate>2007&lt;/PublicationDate>
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        	&lt;DisplayName>Winiarz, Christine Eve&lt;/DisplayName>
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    &lt;Keyword>Mechanical Engineering.&lt;/Keyword>
   	&lt;Abstract>Bus bars on solar cells shade silicon from light. When the bus bars are patterned, they can reflect light back onto the silicon using total internal reflection. These patterned bus bars are tin plated and produce 1-2.5% improvement in module efficiency [6]. There is a potential for even greater improvement by using higher reflectivity metal plating on the bus bars. Silver is the most reflective of all metals, but is also very expensive. We tested to see if silver would actually be as reflective as published values and if silver could redirect a substantial amount of light using total internal reflection. We found that silver plating followed the published spectral dependence curve with little deviation, and would reflect 18.4% more light than the published values for tin. Plating 2.24 microns resulted in 94.9% of reflected light undergoing TIR; the most reflected light of any tested material. Finally, given the current cost of silver is $430 per kilogram and the variable cost of a solar cell is $2 per Watt, the maximum allowable thickness we could afford to plate is 44.8 microns. In our testing, plating as little as 0.35 microns produced a very high light capture. The benefit of silver plating patterned bus bars far outweighs the material costs.&lt;/Abstract>
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