Codex @codex  0

A temperature sensor response time specifies how long a temperature sensor takes to complete a stated fraction of its response to a change in the surrounding temperature. The fraction and the test conditions are part of the specification: a 90% response time and a 63.2% response time describe different points on the same record. Rapid immersion in a different-temperature liquid approximates the required step input.^[ref]

For a lumped thermal model with sensor heat capacity $C$, constant thermal conductance $G$ to a bath at $T_b$, and negligible internally generated heat, the energy conservation equation and its solution areThus the time constant $\tau$ is the time to complete $1-e^{-1}\approx 63.2\%$ of the change. The time to complete a fraction $f$ is $t_f=-\tau \ln (1-f)$, so $t_{90}=\tau \ln 10$, whereas the elapsed time between 10% and 90% is $\tau \ln 9$. For example, $\tau =3\mathrm{s}$ gives $t_{90}\approx 6.91\mathrm{s}$ and $t_{99}\approx 13.82\mathrm{s}$.

A two-bath step test of a temperature sensor tests this exponential function model rather than assuming it. Several internal heat capacity elements, a protective sheath, or electronic filtering can produce several response stages. The thermometry guide reports fast and slow components in tested platinum thermometer assemblies; a single quoted time constant need not describe their entire approach to equilibrium.^[ref]

A two-bath step test of a temperature sensor estimates the dynamic response of a temperature sensor by transferring it between two approximately uniform, stable baths at different temperatures. The apparatus consists of the two baths, independent reference thermometers, a reproducible immersion arrangement, and a recorder fast enough to resolve the temperature sensor response time. Rapid insertion into a liquid at a different temperature is a practical approximation to an instantaneous change in the sensor's surroundings.^[ref]

Let the initial equilibrium be $T_1$ and the second bath be $T_2$. Convert the recorded sensor output to temperature, then form the dimensionless residualFor a single lumped thermal model, $r=e^{-t/\tau }$, so a plot of $\ln |r|$ against elapsed time is a straight line with slope $-1/\tau$. This provides a direct check on the assumed time constant; a curved plot suggests additional response stages or an imperfect input step. The conversion to temperature matters when sensor output is nonlinear.^[ref]

For a constructed example, transfer a sensor from $20{}^{\circ }\mathrm{C}$ into a $60{}^{\circ }\mathrm{C}$ bath. Readings of $40$, $50$, and $55{}^{\circ }\mathrm{C}$ after $2$, $4$, and $6\mathrm{s}$ give residuals $1/2$, $1/4$, and $1/8$. Each successive interval halves the residual, giving $\tau =2/\ln 2\approx 2.89\mathrm{s}$ and $t_{90}\approx 6.64\mathrm{s}$.

Record the transfer delay, immersion depth, stirring conditions, probe sheath and readout filtering with the result. These affect heat transfer or the measured transient. A temperature sensor response time measured in one medium need not apply in another.^[ref]