Differential Equations and Linear Algebra (4th Edition)

Published by Pearson
ISBN 10: 0-32196-467-5
ISBN 13: 978-0-32196-467-0

Chapter 1 - First-Order Differential Equations - 1.6 First-Order Linear Differential Equations - Problems - Page 59: 25

Answer

$T=C_1e^{-kt}+\alpha(t-k^{-1})+C_2$

Work Step by Step

We are given: $T(t)=\alpha (t-k^{-1})+c_1+c_2e^{-kt}$ Newton’s law of cooling: $\frac{dT}{dt}=k(T_0-T)$ Multiply both sides by $\frac{d}{dt}$: $\frac{d^2T}{dt^2}=k\frac{d}{dt}T_0-k\frac{dT}{dt}$ where $k$ is proportionality constant and $T_0$ is the environment's temperature since $\frac{d}{dt}T_0 = \alpha$ $\rightarrow \frac{d^2}{t^2}T+k\frac{dT}{dt}$ Set $\frac{dT}{dt}=v(t)$ then the equation becomes: $\frac{dv}{dt}+ku=k\alpha$ Intergrating factor: $I=e^{\int kdt}=e^{kt}$ The general solution is: $v=I^{-1}(C_1+\int Ik \alpha)$ $v=C_1e^{-kt}+ \alpha$ Intergrate both sides: $T=-\frac{C_1}{k}e^{-kt}+\alpha t+C_2$ Since $C_1$ and $C_2$ are constants, assume $-\frac{C_1}{k}=C_1$ and $C_2=C_2-\frac{\alpha}{k}$ We get: $T=C_1e^{-kt}+\alpha(t-k^{-1})+C_2$
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