A spring's force constant is measured by hanging fifteen different loads and…

PHYSICS · Subjective · Fermi University Physics · Scientific Practice & Experimental Methods · Data analysis and model fitting in the laboratory · Data analysis and model fitting in the laboratory

Computational Physics, Ch Finding the best parameters: minimisation and fitting

Problem

A spring's force constant kk is measured by hanging fifteen different loads and recording the extension xix_i for each applied force, with the model Fi=kxiF_i = k x_i (Hooke's law, taken to hold exactly over the range used). Each force is read with the same uncertainty σF=0.050 N\sigma_F = 0.050\,\mathrm{N}, and the fifteen extensions satisfy ∑i=115xi2=0.980 m2\sum_{i=1}^{15} x_i^2 = 0.980\,\mathrm{m^2}. Because the model is linear in kk, the objective χ2(k)=∑i=115(Fi−kxi)2σF2\chi^2(k) = \sum_{i=1}^{15} \frac{(F_i-kx_i)^2}{\sigma_F^2} is exactly quadratic in kk, so the curvature-based uncertainty σk=σF∑ixi2\sigma_k = \frac{\sigma_F}{\sqrt{\sum_i x_i^2}} is exact rather than approximate. (a) Compute σk\sigma_k from the formula above. (b) A thousand synthetic replicas of the fifteen FiF_i are generated at seed 20242024, each point scattered about the fitted line with the stated σF=0.050 N\sigma_F=0.050\,\mathrm{N}, and each replica is fitted for kk. Predict the standard deviation you expect across the thousand fitted values of kk, and say whether you expect it to agree with σk\sigma_k closely or only roughly, giving a reason tied to the model being linear. (c) A second batch of a thousand replicas is generated with the same seed rule but with the actual scatter of FiF_i doubled to 0.10 N0.10\,\mathrm{N}, while σk\sigma_k is still computed from the formula above using the stated σF=0.050 N\sigma_F=0.050\,\mathrm{N}. Predict the standard deviation of the thousand fitted kk values in this second batch, and compare it with the unchanged σk\sigma_k of part (a).

Browse the problem library