A flat metal plate left outdoors obeys Newton's law of cooling,

PHYSICS · Subjective · Fermi University Physics · Mathematical Methods for Physics · Ordinary differential equations · Ordinary differential equations

Mathematical Methods for Physics, Ch First-order differential equations and physical modelling

Problem

A flat metal plate left outdoors obeys Newton's law of cooling, T˙=−(T−Ta(t))/τ\dot{T} = -(T - T_a(t))/\tau, where T(t)T(t) is the plate's temperature, τ=2.0 h\tau = 2.0\,\mathrm{h} is its (constant) time constant, and the air temperature varies over the day as Ta(t)=15.0∘C+5.0∘Ccos⁡(ωt),ω=π12 rad h−1T_a(t) = 15.0^{\circ}\mathrm{C} + 5.0^{\circ}\mathrm{C}\cos(\omega t), \qquad \omega = \frac{\pi}{12}\,\mathrm{rad\,h^{-1}} (tt in hours, so the period is 24 h24\,\mathrm{h}). At t=0t = 0 the plate's temperature is T(0)=10.0∘CT(0) = 10.0^{\circ}\mathrm{C}. Treat the plate as having a single uniform temperature and τ\tau as fixed (independent of TT). (a) Write the equation in the standard linear form T˙+T/τ=s(t)\dot{T} + T/\tau = s(t) and explain in one line why it cannot be solved by separating variables. (b) Using the integrating factor μ(t)=et/τ\mu(t) = e^{t/\tau} (or, equivalently, treating the oscillating part of s(t)s(t) as the real part of a complex exponential), show that the steady-state part of T(t)T(t) has the form Tss(t)=15.0∘C+5.0∘C1+ω2τ2cos⁡(ωt−φ),φ=arctan⁡(ωτ),T_{\mathrm{ss}}(t) = 15.0^{\circ}\mathrm{C} + \frac{5.0^{\circ}\mathrm{C}}{\sqrt{1+\omega^2\tau^2}}\cos(\omega t - \varphi), \qquad \varphi = \arctan(\omega\tau), and evaluate the amplitude and φ\varphi numerically. (c) Impose T(0)=10.0∘CT(0) = 10.0^{\circ}\mathrm{C} to find the coefficient CC of the transient term Ce−t/τCe^{-t/\tau}, so that T(t)=Tss(t)+Ce−t/τT(t) = T_{\mathrm{ss}}(t) + Ce^{-t/\tau}. (d) Find the time after which the transient has fallen to below 1%1\% of its value at t=0t=0.

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