A particle of mass moves in an unspecified central potential about a fixed centre

PHYSICS · Subjective · Fermi University Physics · Mechanics & Dynamical Systems · Lagrangian mechanics · Lagrangian mechanics

Action and Symmetry, Ch Symmetry, Noether's theorem and what is conserved

Problem

A particle of mass m=0.25 kgm=0.25\ \mathrm{kg} moves in an unspecified central potential about a fixed centre, subject also to a linear drag force −bv-b\mathbf v with b=0.040 kg s−1b=0.040\ \mathrm{kg\,s^{-1}}, represented by the Rayleigh dissipation function F=12b(r˙2+r2θ˙2)\mathcal F=\tfrac12 b(\dot r^2+r^2\dot\theta^2). At t=0t=0 its angular momentum about the centre is pθ(0)=0.60 kg m2 s−1p_\theta(0)=0.60\ \mathrm{kg\,m^2\,s^{-1}}. Find pθp_\theta at t=8.0 st=8.0\ \mathrm{s}.

Related theory

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