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		<title>Decarburization</title>
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		<summary type="html">&lt;p&gt;71.167.173.50: /* As a secondary effect */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;Steinhart–Hart equation&#039;&#039;&#039; is a model of the [[Electrical resistance|resistance]] of a [[semiconductor]] at different [[temperature]]s. The equation is:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;{1 \over T} = A + B \ln(R) + C (\ln(R))^3 \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where:&lt;br /&gt;
* &amp;lt;math&amp;gt;T&amp;lt;/math&amp;gt; is the temperature (in kelvins)&lt;br /&gt;
* &#039;&#039;R&#039;&#039; is the resistance at &#039;&#039;T&#039;&#039; (in ohms)&lt;br /&gt;
* &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt;, and &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; are the &#039;&#039;&#039;Steinhart–Hart coefficients&#039;&#039;&#039; which vary depending on the type and model of [[thermistor]] and the temperature range of interest. (The most general form of the applied equation contains a &amp;lt;math&amp;gt;(\ln(R))^2&amp;lt;/math&amp;gt; term, but this is frequently neglected because it is typically much smaller than the other coefficients, and is therefore not shown above.)&lt;br /&gt;
&lt;br /&gt;
==Uses of the equation==&lt;br /&gt;
The equation is often used to derive a precise temperature of a thermistor since it provides a closer approximation to actual temperature than simpler equations, and is useful over the entire working temperature range of the sensor.  Steinhart–Hart coefficients are usually published by thermistor manufacturers.&lt;br /&gt;
&lt;br /&gt;
Where Steinhart–Hart coefficients are not available, they can be derived. Three accurate measures of resistance are made at precise temperatures, then the coefficients are derived by solving three [[simultaneous equations]].&lt;br /&gt;
&lt;br /&gt;
==Inverse of the equation==&lt;br /&gt;
To find the resistance of a semiconductor given the temperature the inverse of the Steinhart–Hart equation must be used.  See the [http://www.cornerstonesensors.com/reports/ABC%20Coefficients%20for%20Steinhart-Hart%20Equation.pdf Application Note], &amp;quot;A, B, C Coefficients for Steinhart–Hart Equation&amp;quot;.&lt;br /&gt;
:&amp;lt;math&amp;gt;R = \exp\left(\sqrt[3]{x - y} - \sqrt[3]{x + y}\right),&amp;lt;/math&amp;gt;&lt;br /&gt;
where &lt;br /&gt;
:&amp;lt;math&amp;gt;y = {A - {1 \over T} \over 2C},&amp;lt;/math&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt;x = \sqrt{\left({B \over 3C}\right)^3 + y^2}.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Steinhart–Hart coefficients==&lt;br /&gt;
To find the coefficients of Steinhart–Hart, we need to know at-least three operating points. For this, we use three values of resistance data for three known temperatures.&lt;br /&gt;
:&amp;lt;math&amp;gt;\begin{cases} A + \left(\ln R_1 \right) B + \left(\ln R_1 \right)^3 C=\frac{1}{T_1} \\ A + \left(\ln R_2 \right) B + \left(\ln R_2 \right)^3 C = \frac{1}{T_2} \\ A + \left(\ln R_3 \right) B + \left(\ln R_3 \right)^3 C = \frac{1}{T_3} \end{cases}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
With &amp;lt;math&amp;gt;R_1&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;R_2&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;R_3&amp;lt;/math&amp;gt; values of resistance at the temperatures &amp;lt;math&amp;gt;T_1&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;T_2&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;T_3&amp;lt;/math&amp;gt;, one can express &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;B&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;C&amp;lt;/math&amp;gt; (all calculations):&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;L_1 = \ln\left(R_1\right)&amp;lt;/math&amp;gt;,&amp;amp;nbsp;&amp;amp;nbsp; &amp;lt;math&amp;gt;L_2=\ln\left(R_2\right)&amp;lt;/math&amp;gt; &amp;amp;nbsp;&amp;amp;nbsp;and &amp;amp;nbsp;&amp;amp;nbsp;&amp;lt;math&amp;gt;L_3=\ln\left(R_3\right)&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;Y_1=\frac{1}{T_1}&amp;lt;/math&amp;gt;,&amp;amp;nbsp; &amp;lt;math&amp;gt;Y_2=\frac{1}{T_2}&amp;lt;/math&amp;gt; &amp;amp;nbsp; and &amp;amp;nbsp; &amp;lt;math&amp;gt;Y_3=\frac{1}{T_3}&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;\gamma_2=\frac{Y_2-Y_1}{L_2-L_1}&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;\gamma_3=\frac{Y_3-Y_1}{L_3-L_1}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow C=\left( \frac{ \gamma_3 - \gamma_2 }{ L_3 - L_2} \right) \left(L_1 + L_2 + L_3\right)^{-1}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow B=\gamma_2 - C \left(L_1^2+L_1 L_2+L_2^2\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\Rightarrow A=Y_1 - \left(B+L_1^2 C\right) L_1&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Developers of the equation==&lt;br /&gt;
The equation is named after [[John S. Steinhart]] and [[Stanley R. Hart]] who first published the relationship in 1968.&amp;lt;ref&amp;gt;John S. Steinhart, Stanley R. Hart, Calibration curves for thermistors, Deep Sea Research and Oceanographic Abstracts, Volume 15, Issue 4, August 1968, Pages 497-503, ISSN 0011-7471, {{doi|10.1016/0011-7471(68)90057-0}}.&amp;lt;/ref&amp;gt; Professor Steinhart (1929–2003), a fellow of the [[American Geophysical Union]] and of the [[American Association for the Advancement of Science]], was a member of the faculty of [[University of Wisconsin–Madison]] from 1969 to 1991.[http://www.secfac.wisc.edu/senate/2004/0405/1775(mem_res).pdf] Dr. Hart, a Senior Scientist at [[Woods Hole Oceanographic Institution]] since 1989 and fellow of the [[Geological Society of America]], the American Geophysical Union, the [[Geochemical Society]] and the [[European Association of Geochemistry]], [http://www.whoi.edu/science/GG/people/shart/cv.htm] was associated with Professor Steinhart at the [[Carnegie Institution of Washington]] when the equation was developed.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{DEFAULTSORT:Steinhart-Hart equation}}&lt;br /&gt;
[[Category:Condensed matter physics]]&lt;/div&gt;</summary>
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