Thermistor: Difference between revisions

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<math>R=R_0 e^{B({1\over T}-{1\over T_0})}</math>.
<math>R=R_0 e^{B({1\over T}-{1\over T_0})}</math>.
The absoute temperature then can be obtained by inverting the equation above:
<math>T = \left( {1\over T_0} + {1\over B} \ln {R\over R_0} \right) ^{-1}</math>

Latest revision as of 13:04, 9 April 2024

A common temperature sensor is a Thermistor, which is a device with a temperature-dependent resistance R(T) and a negative temperature coefficient (NTC), i.e., the Resistance decreases with temperature, or ∂R(T)∂T<0. 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:

1T=a+bln⁡R+c(ln⁡R)3

Usually, the coefficients a,b,c are not specified in a data sheet of a device. More commonly, three things are quoted/specified:

  • Reference temperature, typically 25 Celsius; sometimes this is not even mentioned explicitly
  • Resistance R0 at the reference temperature (typically 25 Celsius). Often, R0=10kΩ.
  • Characteristic of the exponential, the constant B=1/b in the above expression. Typically around 4000 Kelvin.

These parameters can be used with a simplified Steinhart-Hart equation, which assumes c=0 in the expression above. Then, the equation becomes

1T=A+Bln⁡R

or

R=R0eB(1T−1T0).

The absoute temperature then can be obtained by inverting the equation above:

T=(1T0+1Bln⁡RR0)−1