Radiative Temperature Measurement

Chapter 26 - Signal Characterization in Control Systems

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Temperature measurement devices may be classified into two broad types: contact and non-contact. Contact-type temperature sensors detect temperature by directly touching the material to be measured, and there are several varieties in this category. Non-contact temperature sensors work by detecting light emitted by hot objects.

Energy radiated in the form of electromagnetic waves (photons, or light) relates to object temperature by an equation known as the Stefan-Boltzmann equation, which tells us the rate of heat lost by radiant emission from a hot object is proportional to the fourth power of its absolute temperature:

\[P = e \sigma A T^4\]

Where,

\(P\) = Radiated energy power (watts)

\(e\) = Emissivity factor (unitless)

\(\sigma\) = Stefan-Boltzmann constant (5.67 \(\times\) \(10^{-8}\) W / m\(^{2}\) \(\cdot\) K\(^{4}\))

\(A\) = Surface area (square meters)

\(T\) = Absolute temperature (Kelvin)

Solving for temperature (\(T\)) involves the use of the fourth root, to “un-do” the fourth power function inherent to the original function:

\[T = \root 4 \of {P \over {e \sigma A}}\]

Any optical temperature sensor measuring the emitted power (\(P\)) must “characterize” the power measurement using the above equation to arrive at an inferred temperature. This characterization is typically performed inside the temperature sensor by a microcomputer.