A Langevin-dynamics simulation of a Brownian particle records its velocity every

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Mathematical Methods for Physics · Uncertainty in measurement

Scientific Computing for Physicists, Ch The uncertainty of a simulated number: inputs, sensitivity and correlated output

Problem

A Langevin-dynamics simulation of a Brownian particle records its velocity every Δt=0.02 s\Delta t = 0.02\,\mathrm{s}, for N=65536N = 65536 samples. The sample variance of the series is σ2=1.5 m2 s−2\sigma^2 = 1.5\,\mathrm{m^2\,s^{-2}}. A one-sided Welch power spectral density estimate of the series (periodogram method, segments averaged as in the spectral-estimation chapter) gives a flat low-frequency plateau S(0)=1.14 m2 s−2 sS(0) = 1.14\,\mathrm{m^2\,s^{-2}\,s}. Separately, a grid-convergence study of the integrator (Richardson extrapolation from runs at two time steps, assuming the integrator's formal order p=2p = 2, following the solution-verification method) gives a numerical uncertainty on the mean velocity of unum=0.0080 m s−1u_{\rm num} = 0.0080\,\mathrm{m\,s^{-1}}. No input parameter of the simulation carries a stated distribution here. ((a)) Using s=S(0)/(2σ2Δt)s = S(0)/(2\sigma^2\Delta t), find the statistical inefficiency ss of the velocity series. ((b)) Find the effective sample size NeffN_{\rm eff} and the statistical uncertainty ustatu_{\rm stat} of the mean velocity. ((c)) Assemble the combined uncertainty usimu_{\rm sim} of the simulated mean velocity from its numerical and statistical contributions, treating them as independent.

Browse the problem library