A quantity , measured in metres, obeys y - 2 t y + 2 t^2 y = g, t t_0, with constant…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Ordinary differential equations · Ordinary differential equations

Mathematical Methods for Physics, Ch Higher-order linear equations, the Wronskian and variation of parameters

Problem

A quantity y(t)y(t), measured in metres, obeys y¨−2ty˙+2t2y=g,t≥t0,\ddot{y} - \frac{2}{t}\dot{y} + \frac{2}{t^2}y = g, \qquad t \ge t_0, with g=2.0 m s−2g = 2.0\ \mathrm{m\,s^{-2}} constant and t0=1.0 st_0 = 1.0\ \mathrm{s}. It is at rest at t0t_0: y(t0)=0y(t_0) = 0 and y˙(t0)=0\dot{y}(t_0) = 0. Substitution shows that y=ty = t solves the undriven equation; no other solution is given. ((a)) Find y(t)y(t) for t≥t0t \ge t_0, and evaluate y(2.0 s)y(2.0\ \mathrm{s}) to three significant figures. ((b)) Say which tools the answer needed, and why Chapter 8's route (an auxiliary equation for the undriven solutions, then a trial form guessed from the drive) is not available here, even though the drive is a constant.

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