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	<id>https://energyeducation.ca/wiki/index.php?action=history&amp;feed=atom&amp;title=Solar_cell_efficiency</id>
	<title>Solar cell efficiency - Revision history</title>
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	<updated>2026-10-07T22:00:10Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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		<id>https://energyeducation.ca/wiki/index.php?title=Solar_cell_efficiency&amp;diff=7339&amp;oldid=prev</id>
		<title>Jmdonev: 1 revision imported</title>
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		<updated>2018-06-25T14:30:28Z</updated>

		<summary type="html">&lt;p&gt;1 revision imported&lt;/p&gt;
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				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;1&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 14:30, 25 June 2018&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-notice&quot; lang=&quot;en&quot;&gt;&lt;div class=&quot;mw-diff-empty&quot;&gt;(No difference)&lt;/div&gt;
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		<author><name>Jmdonev</name></author>
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		<id>https://energyeducation.ca/wiki/index.php?title=Solar_cell_efficiency&amp;diff=7338&amp;oldid=prev</id>
		<title>Jmdonev at 00:28, 9 June 2018</title>
		<link rel="alternate" type="text/html" href="https://energyeducation.ca/wiki/index.php?title=Solar_cell_efficiency&amp;diff=7338&amp;oldid=prev"/>
		<updated>2018-06-09T00:28:51Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;[[Category:Done 2018-06-15]] &lt;br /&gt;
[[File:Silicon_solar_cell_(PERC)_front_and_back.jpg|300px|thumb|Figure 1. A modern crystalline silicon solar cell.&amp;lt;ref&amp;gt;Wikimedia Commons. (May 3, 2018). &amp;#039;&amp;#039;Silicon solar cell (PERC) front and back&amp;#039;&amp;#039; [Online]. Available: https://commons.wikimedia.org/wiki/File:Silicon_solar_cell_(PERC)_front_and_back.jpg&amp;lt;/ref&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
&amp;lt;onlyinclude&amp;gt;Efficiency is the comparison of [[energy]] output to energy input of a given system. For [[photovoltaic cell|solar photovoltaic (PV) cells]], this means the ratio of useful [[electricity|electrical energy]] they produce to the amount of [[solar energy]] incident on the cell under standardized testing conditions. Although some experimental solar cells have achieved efficiencies of close to 50%, most commercial cells are below 30%.&amp;lt;/onlyinclude&amp;gt; Unlike the [[carnot efficiency]] which limits the [[thermal efficiency]] of [[heat engine]]s, the efficiency of solar cells is limited by something called the &amp;quot;band gap energy&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
==Band Gap Energy==&lt;br /&gt;
The physics of [[semiconductor]]s requires a minimum amount of energy to remove an [[electron]] from a crystal structure, known as the [[band gap]] energy. For solar cells, this energy is provided by particles of light called [[photon]]s, which are tiny packets of [[electromagnetic radiation]] released from the [[Sun]]. [[Sunlight]] contains a wide [[Solar spectrum|spectrum]] of photons with different wavelengths and energy. If a photon strikes a solar cell and has less energy than the band gap, it gets absorbed as [[thermal energy]]. If it has sufficient energy it has a chance of &amp;quot;knocking&amp;quot; an electron loose and producing an electrical current. For [[silicon]], the band gap energy is 1.12 [[electron volt]]s.&amp;lt;ref name=Wolfson&amp;gt;R. Wolfson, &amp;quot;Photovoltaic Solar Energy&amp;quot; in &amp;#039;&amp;#039;Energy, Environment, and Climate&amp;#039;&amp;#039;, 2nd ed., New York, NY: W.W. Norton &amp;amp; Company, 2012, ch. 9, sec. 5, pp. 244-252&amp;lt;/ref&amp;gt; The longest [[wavelength]] (which corresponds to the lowest energy) that is capable of removing an electron is 1.1 [[prefixes|µ]][[meter|m]].&amp;lt;ref&amp;gt;&amp;lt;math&amp;gt;\lambda=\frac{hc}{E}=\frac{(6.626kg*m^2/s) \times (3\times10^8 m/s)}{1.12eV}\times \frac{1eV}{1.6\times10^{-19}J}=1.1\mu m&amp;lt;/math&amp;gt;&amp;lt;/ref&amp;gt; From Figure 2 below it can be seen that the visible [[light]] and [[ultraviolet]] light have sufficient energy, but a good portion of [[infrared]] light cannot be used. This means that ~1/4 of the light from the Sun is not sufficient enough to create electricity.&amp;lt;ref name=Wolfson/&amp;gt;&lt;br /&gt;
[[File:PVCELL.png|thumbnail|center|816px|Figure 2. The solar energy received by the Earth, and the corresponding energies of its photons. Efficiency of a PV cell is largely effected by the amount of incoming light that can cause current to flow.&amp;lt;ref&amp;gt;Made internally by member of the Energy Education team, adapted from &amp;#039;&amp;#039;Energy, Environment and Climate&amp;#039;&amp;#039; by R. Wolfson.&amp;lt;/ref&amp;gt;]]&lt;br /&gt;
Even from the light that &amp;#039;&amp;#039;can&amp;#039;&amp;#039; be absorbed, there is still a problem. Any energy &amp;#039;&amp;#039;above&amp;#039;&amp;#039; the band-gap energy will be transformed into [[heat]]. This also cuts the efficiency because that heat energy is not being used for any useful task.&amp;lt;ref name=Wolfson/&amp;gt; Of the electrons that are made available, not all of them will actually make it to the metal contact and generate electricity. This is because some of them will not be accelerated sufficiently by the [[voltage]] inside the [[semiconductor]]. Because of the reasons listed, the theoretical efficiency of silicon PV cells is about &amp;#039;&amp;#039;&amp;#039;33%&amp;#039;&amp;#039;&amp;#039;.&amp;lt;ref name=Wolfson/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Increasing efficiency==&lt;br /&gt;
There are ways to improve the efficiency of PV cells, all of which come with an increased cost. One way is to decrease the number of semiconductor impurities and crystal structure deformations. This can be achieved through the production of [[Types of PV cells|&amp;#039;&amp;#039;&amp;#039;monocrystalline&amp;#039;&amp;#039;&amp;#039;]], or &amp;quot;single-crystal&amp;quot; cells. A more pure and uniform cell has a higher chance of interacting with incoming photons.&amp;lt;ref name=peake/&amp;gt; Another method is to use a more efficient semiconducting material such as [[Types of PV cells|&amp;#039;&amp;#039;&amp;#039;Gallium Arsenide&amp;#039;&amp;#039;&amp;#039;]]. Although it&amp;#039;s much more rare and expensive than silicon, gallium arsenide has an optimal band-gap of 1.4 [[electron volt]]s, allowing for a higher percentage of the Sun&amp;#039;s energy to be harnessed.&amp;lt;ref name=peake&amp;gt;Stephen Peake. &amp;#039;&amp;#039;Renewable Energy: Power for a Sustainable Future&amp;#039;&amp;#039;, 4th ed. Oxford, UK: Oxford University Press, 2018.&amp;lt;/ref&amp;gt; Multiple layers of semiconductor material called [[p-n junction]]s can also be used to increase cell efficiency. These [[Types of PV cells|&amp;#039;&amp;#039;&amp;#039;multi-junction&amp;#039;&amp;#039;&amp;#039;]] cells harness energy from multiple sections of the solar spectrum as each junction has a different [[band gap]] energy.&amp;lt;ref name=peake/&amp;gt; Efficiency can also be increased through &amp;#039;&amp;#039;&amp;#039;[[concentrated photovoltaics]]&amp;#039;&amp;#039;&amp;#039;. This method involves concentrating the Sun&amp;#039;s energy through various methods to increase the intensity of energy hitting the solar cell. For more information about the different types of solar cells, [[Types of PV cells|click here]]. Figure 3 below shows the evolution of solar cell technologies and efficiencies from 1976 to 2017.&lt;br /&gt;
[[File:Best_Research-Cell_Efficiencies.png|thumbnail|center|800px|Figure 3. Conversion efficiencies of best research solar cells worldwide for various photovoltaic technologies since 1976.&amp;lt;ref&amp;gt;Wikimedia Commons. (April 15, 2018). &amp;#039;&amp;#039;Best Research-Cell Efficiencies&amp;#039;&amp;#039; [Online]. Available: https://commons.wikimedia.org/wiki/File:Best_Research-Cell_Efficiencies.png&amp;lt;/ref&amp;gt;]]&lt;br /&gt;
&lt;br /&gt;
==Power Degradation==&lt;br /&gt;
Efficiency of solar cells and [[solar panel]]s are known to decrease over time, outputting less energy every year. This is due to a variety of factors including UV exposure and weather cycles. A comprehensive report from the National Renewable Energy Laboratory (NREL) states that the median degradation rate is 0.5% per year.&amp;lt;ref&amp;gt;Dirk C. Jordan and Sarah R. Kurtz. &amp;#039;&amp;#039;Photovoltaic Degradation Rates — An Analytical Review&amp;#039;&amp;#039;, National Renewable Energy Laboratory, USA, 2012. Accessed April 24, 2018. [Online] Available at https://www.nrel.gov/docs/fy12osti/51664.pdf&amp;lt;/ref&amp;gt; This means that after 25 years of operation a solar panel originally rated for 300 watts of power output will only produce about 260 watts on average. Degradation in the first year of operation can also be much more profound, at around 2.5%.&lt;br /&gt;
&lt;br /&gt;
==For Further Reading==&lt;br /&gt;
*[[Sun]]&lt;br /&gt;
*[[Types of PV cells]]&lt;br /&gt;
*[[Photovoltaic effect]]&lt;br /&gt;
*[[Thermal efficiency]]&lt;br /&gt;
*Or explore a [[Special:Random|random page]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
==References==&lt;/div&gt;</summary>
		<author><name>Jmdonev</name></author>
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