Question #51339

Separate the following partial differential equation into a set of three ODEs by the method of separation of variables :
d^2 u/dt^2 = c^2 [d^2 u/dr^2 + 1/r * du/dr + 1/r^2 * d^2/d(thita)^2 ]

Expert's answer

Answer on Question #51339 – Math – Differential Calculus | Equations

Separate the following partial differential equation into a set of three ODEs by the method of separation of variables :


d2u/dt2=c2[d2u/dr2+1rur+1r22uθ2]\mathrm{d}^2 \mathrm{u} / \mathrm{dt}^2 = \mathrm{c}^2 \left[ \mathrm{d}^2 \mathrm{u} / \mathrm{dr}^2 + \frac{1}{r} \cdot \frac{\partial u}{\partial r} + \frac{1}{r^2} \cdot \frac{\partial^2 u}{\partial \theta^2} \right]


Solution


2ut2=c2[2ur2+1rur+1r22uθ2]\frac{\partial^2 u}{\partial t^2} = c^2 \left[ \frac{\partial^2 u}{\partial r^2} + \frac{1}{r} \frac{\partial u}{\partial r} + \frac{1}{r^2} \frac{\partial^2 u}{\partial \theta^2} \right]


Assume that u(r,θ,t)=R(r)Θ(θ)T(t)u(r, \theta, t) = R(r) \Theta(\theta) T(t)

So R(r)Θ(θ)T(t)=c2[(R+1rR)Θ(θ)T(t)+1r2Θ(θ)R(r)T(t)]R(r) \Theta(\theta) T''(t) = c^2 \left[ \left( R'' + \frac{1}{r} R' \right) \Theta(\theta) T(t) + \frac{1}{r^2} \Theta''(\theta) R(r) T(t) \right] → divide both sides by c2R(r)Θ(θ)T(t)c^2 R(r) \Theta(\theta) T(t) \rightarrow

1c2TT=(R+1rR)1R+1r2ΘΘ\rightarrow \frac{1}{c^2} \frac{T''}{T} = \left( R'' + \frac{1}{r} R' \right) \frac{1}{R} + \frac{1}{r^2} \frac{\Theta''}{\Theta}


The right side of this equation does not depend on TT, hence the left side of this equation must be constant.

Thus, 1c2TT=(R+1rR)1R+1r2ΘΘ=λ\frac{1}{c^2} \frac{T''}{T} = \left( R'' + \frac{1}{r} R' \right) \frac{1}{R} + \frac{1}{r^2} \frac{\Theta''}{\Theta} = \lambda.


(R+1rR)1R+1r2ΘΘ=λΘΘ=(R+1rR)r2Rλr2\left( R'' + \frac{1}{r} R' \right) \frac{1}{R} + \frac{1}{r^2} \frac{\Theta''}{\Theta} = \lambda \rightarrow -\frac{\Theta''}{\Theta} = \left( R'' + \frac{1}{r} R' \right) \frac{r^2}{R} - \lambda r^2


Because each side only depends on one independent variable, both sides of this equation must be constant. This gives the second separation constant, which we call μ\mu.

The equation with respect to Θ\Theta can then be written as


Θ+μΘ=0\Theta'' + \mu \Theta = 0


And equation with respect to RR:


(R+1rR)r2Rλr2=μr2R+rR(λr2+μ)R=0\left(R ^ {\prime \prime} + \frac {1}{r} R ^ {\prime}\right) \frac {r ^ {2}}{R} - \lambda r ^ {2} = \mu \rightarrow r ^ {2} R ^ {\prime \prime} + r R ^ {\prime} - (\lambda r ^ {2} + \mu) R = 0


Finally we have 3 ODEs:


Tλc2T=0;Θ+μΘ=0;r2R+rR(λr2+μ)R=0.\begin{array}{l} T ^ {\prime \prime} - \lambda c ^ {2} T = 0; \\ \boldsymbol {\Theta} ^ {\prime \prime} + \mu \boldsymbol {\Theta} = \mathbf {0}; \\ r ^ {2} R ^ {\prime \prime} + r R ^ {\prime} - (\lambda r ^ {2} + \mu) R = 0. \end{array}


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