Self Heating Effect Thermistors

Please click on the section below to view your area of interest:

bullet Introduction   bullet Thermal Time Constant (T.C.)
bullet Chip Configuration   bullet Thermal Dissipation Constant (D.C.)
bullet Volume Resistivity   bullet Voltage–Current Characteristics
bullet Resistance   bullet Tolerance of Thermistors
bullet Slope (Resistance Ratio)   bullet BetaCURVE and BetaCHIP Products
bullet Alpha (Temperature Coefficient)   bullet Stability & reliability of thermistors
bullet Modelling of Conduction in Thermistors   bullet Specification of thermistors for applications
bullet Mathematical Modelling of Thermistors   bullet Application Notes
bullet Exponential Model of NTC Thermistors Beta Value,ß , or Sensitivity Index   bullet Circuit Notes
bullet The Steinhart-Hart Thermistor Equation   bullet Technical Note from Analog Devices
www.analog.com/adn8830
bullet Steinhart Coefficients for BetaTHERM standard part numbers    
bullet Factors affecting measured resistance value of thermistors      
bullet Self heating effect of thermistors      
bullet Zero-power resistance characteristic      
         

Self Heating effect of Thermistors:

To fully avail of the information in the published tables of Resistance versus temperature for thermistors and to optimize the accuracy of the Steinhart-Hart Equation it is essential to consider the electrical power levels in the thermistor during measurements. When the resistance of a thermistor is being measured there is a voltage across it and a current passing through it (from Ohm’s Law ).
Ohms Law states that for a resistive component: V = IxR where,
V is the voltage across the component in Volts,
I is the current through the component in Amps
R is the resistance of the component in Ohms.
The power in the component is defined as the product of the current and voltage:
P = I x V

where P is the power in Watts, I is in Amps,V is in Volts.

This power is dissipated in the component, and for a thermistor the power causes heating of the thermistor. The heating effect in turn causes the resistance of the thermistor to decrease. This power dissipation is known as self-heating of the thermistor.

If the power levels are moderate (of the order of several milli-Watts (mW), the self-heating will not continue indefinitely, because the thermistor will reach thermal equilibrium with it’s environment. The stage at which this equilibrium is reached depends on the thermal characteristics of the system.

It should be noted that when this "steady" state is reached, the resistance of the thermistor will not accurately represent the temperature of it’s environment. Instead, the resistance of the thermistor will be lower than expected, because of the self heating effect. To obtain a resistance reading from the thermistor that accurately represents the temperature of it’s environment it is critical that the power levels (essentially the current levels) associated with the measurement are low enough not to cause appreciable self heating.

The self heating effect should be considered in all thermistor applications and even in basic resistance measurements using a digital ohm-meter (multi-meter). Most manufactures of measuring instruments specify the magnitude of current used on the various resistance measuring ranges and it is important to be aware of these values in performing resistance measurements on thermistors.

The self-heating effect is a disadvantage in attempting to make accurate resistance measurements, but it is the basis of other applications. These applications are discussed in a later section of the catalog.

Because the self-heating effect can influence the measured resistance value of a thermistor it is important to quantify it in some manner. This is done by using the concept of "Zero-power resistance characteristic."

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