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	<title>Thermistor - Revision history</title>
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	<updated>2026-04-16T02:06:27Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://pc5271.org/PC5271_AY2425S2/index.php?title=Thermistor&amp;diff=6&amp;oldid=prev</id>
		<title>Christian: Created page with &quot;A common temperature sensor is a Thermistor, which is a device with a temperature-dependent resistance &lt;math&gt;R(T)&lt;/math&gt; and a negative temperature coefficient (NTC), i.e., the Resistance decreases with temperature, or &lt;math&gt;{\partial R(T) \over \partial T} &lt; 0 &lt;/math&gt;. Therefore, thermistors are sometime referenced as NTC sensors.  Their resistances can be described by a Steinhardt-Hart equation, which relates resistance R and absolute temperature T:  &lt;math&gt; {\frac {1}{...&quot;</title>
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		<updated>2024-12-30T10:40:59Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;A common temperature sensor is a Thermistor, which is a device with a temperature-dependent resistance &amp;lt;math&amp;gt;R(T)&amp;lt;/math&amp;gt; and a negative temperature coefficient (NTC), i.e., the Resistance decreases with temperature, or &amp;lt;math&amp;gt;{\partial R(T) \over \partial T} &amp;lt; 0 &amp;lt;/math&amp;gt;. Therefore, thermistors are sometime referenced as NTC sensors.  Their resistances can be described by a Steinhardt-Hart equation, which relates resistance R and absolute temperature T:  &amp;lt;math&amp;gt; {\frac {1}{...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;A common temperature sensor is a Thermistor, which is a device with a temperature-dependent resistance &amp;lt;math&amp;gt;R(T)&amp;lt;/math&amp;gt; and a negative temperature coefficient (NTC), i.e., the Resistance decreases with temperature, or &amp;lt;math&amp;gt;{\partial R(T) \over \partial T} &amp;lt; 0 &amp;lt;/math&amp;gt;. Therefore, thermistors are sometime referenced as NTC sensors.&lt;br /&gt;
&lt;br /&gt;
Their resistances can be described by a Steinhardt-Hart equation, which relates resistance R and absolute temperature T:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {\frac {1}{T}}=a + b \ln R + c (\ln R)^{3} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Usually, the coefficients &amp;lt;math&amp;gt;a,b,c&amp;lt;/math&amp;gt; are not specified in a data sheet of a device. More commonly, three things are quoted/specified:&lt;br /&gt;
* Reference temperature, typically 25 Celsius; sometimes this is not even mentioned explicitly&lt;br /&gt;
* Resistance R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt; at the reference temperature (typically 25 Celsius). Often, R&amp;lt;sub&amp;gt;0&amp;lt;/sub&amp;gt;=10k&amp;amp;Omega;.&lt;br /&gt;
* Characteristic of the exponential, the constant B=1/b in the above expression. Typically around 4000 Kelvin.&lt;br /&gt;
&lt;br /&gt;
These parameters can be used with a simplified Steinhart-Hart equation, which assumes c=0 in the expression above. Then, the equation becomes&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; {\frac {1}{T}}=A+B\ln R&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
or&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;R=R_0 e^{B({1\over T}-{1\over T_0})}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The absoute temperature then can be obtained by inverting the equation above:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;T = \left( {1\over T_0} + {1\over B} \ln {R\over R_0} \right) ^{-1}&amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Christian</name></author>
	</entry>
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