Introduction & Context

A thermocouple produces a small open-circuit voltage that is a monotonic function of the temperature difference between its measuring junction and the reference junction. In process engineering this voltage is measured by a data-acquisition system; converting it to a meaningful temperature is essential for control loops, safety interlocks, custody transfer calculations, and regulatory reporting. The linear segment model shown here is valid for Type K (Chromel–Alumel) thermoelements between 0 °C and 500 °C and is routinely embedded in PLCs, DCSs, and micro-controller firmware where computational resources are limited and a fast, deterministic result is required.

Methodology & Formulas

  1. Reference-junction compensation
    When the reference junction is held at \(T_{\text{ref}}\) the effective (compensated) voltage that corresponds to the measuring-junction temperature is \[ V_{\text{net}} = V_{\text{meas}} \quad \text{if} \quad T_{\text{ref}} = 0\,^{\circ}\text{C}. \] For \(T_{\text{ref}} \neq 0\,^{\circ}\text{C}\) add the Seebeck voltage generated over the interval \([0, T_{\text{ref}}]\) obtained from the NIST tables or polynomials; the code shown assumes an ice-point reference so this step is bypassed.
  2. Linear conversion
    Inside the monotonic region the temperature is approximated by a straight-line fit \[ T = m\,V_{\text{net}} + b \] where \(m\) is the slope (°C mV–1) and \(b\) is the offset (°C) that forces the curve through the mid-range calibration point.
  3. Validity regime
    The linear coefficients are valid only inside the following bounds:
    Parameter Lower limit Upper limit Remark
    Voltage, \(V_{\text{net}}\) \(V_{\min}\) \(V_{\max}\) Outside this interval the NIST polynomial must be used.
    Temperature, \(T\) \(T_{\min}\) \(T_{\max}\) Same as above.