2.
Measurement Process Characterization
2.3. Calibration 2.3.4. Catalog of calibration designs


Measurement sequence  Calibration of liquid in glass thermometers is usually carried out in a controlled bath where the temperature in the bath is increased steadily over time to calibrate the thermometers over their entire range. One way of accounting for the temperature drift is to measure the temperature of the bath with a standard resistance thermometer at the beginning, middle and end of each run of K test thermometers. The test thermometers themselves are measured twice during the run in the following time sequence: $$ R_1, \, T_1, \, T_2, \, \ldots, \, T_K, \, R_2, \, T_K', \, \ldots, \, T_2', \, T_1', \, R_3 $$ where \( R_1, \, R_2, \, R_3 \) represent the measurements on the standard resistance thermometer and \( T_1, \, T_2, \, \ldots, \, T_K \) and \( T_1', \, T_2', \, \ldots, \, T_K' \) represent the pair of measurements on the K test thermometers.  
Assumptions regarding temperature 
The assumptions for the analysis are that:


Indications for test thermometers  It can be shown (Cameron and Hailes) that the average reading for a test thermometer is its indication at the temperature implied by the average of the three resistance readings. The standard deviation associated with this indication is calculated from difference readings where $$ d_i = T_i  T_i' $$ is the difference for the ith thermometer. This difference is an estimate of \( \phi + 2(Ki)\Delta \).  
Estimates of drift 
The estimates of the shift due to the resistance
thermometer and temperature drift are given by:


Standard deviations  The residual variance is given by $$ {\large s}^2 = \frac{1}{(K2)} \sum_{i=1}^K \left( d_i  \widehat{\phi} 2(Ki)\widehat{\Delta} \right) ^2 \, . $$ The standard deviation of the indication assigned to the ith test thermometer is $$ {\large s}_{test} = \frac{{\large s}}{\sqrt{2}} $$ and the standard deviation for the estimates of shift and drift are $$ {\large s}_\phi = \frac{\sqrt{2} (2K1)}{K(K+1)} {\large s} $$ and $$ {\large s}_\Delta = \frac{\sqrt{3}}{K(K^2 1)} {\large s} \, , $$ respectively. 