Two thermistors are calibrated by finding the temperature at which a modelled…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Numerical and computational mathematics · Numerical and computational mathematics

Computational Physics, Ch Where a function vanishes, and what lies between the points

Problem

Two thermistors are calibrated by finding the temperature TT at which a modelled resistance function g(T)g(T) (in Ω\Omega) matches a measured value, using Newton-Raphson on g(T)=0g(T)=0. Near its own root, sensor A's calibration curve is steep, with slope gA′(TA∗)=42.0 Ω ∘C−1g_A'(T_A^*) = 42.0\ \Omega\,{}^{\circ}\mathrm{C}^{-1}. Sensor B is operating near a shallow plateau in its resistance-temperature curve, with slope gB′(TB∗)=6.0×10−3 Ω ∘C−1g_B'(T_B^*) = 6.0\times10^{-3}\ \Omega\,{}^{\circ}\mathrm{C}^{-1}. Both iterations are stopped using the identical residual criterion ∣g(T)∣<3.0×10−3 Ω|g(T)| \lt 3.0\times10^{-3}\ \Omega.An engineer writes: "Since both calibrations were stopped at the same residual tolerance, both temperatures are known to the same accuracy." ((a)) State the approximate relation between a residual ∣g(T)∣|g(T)| and the distance ∣T−T∗∣|T-T^*| to the true root, valid near the root. ((b)) Use it to find the error in TT that the stated stopping criterion actually guarantees for sensor A and for sensor B. ((c)) Say whether the engineer is right, and if not, by how many decades the two guaranteed errors differ.

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