Question #87071

Obtain the value of the constant c for which the function u(x,t) = cosαcxsinαt is a
solution of the wave equation . 2
2
2
2
2
x

Expert's answer

The one-dimensional wave equation has the form


∂2u∂t2=c2⋅∂2u∂x2\frac{\partial^2 u}{\partial t^2}=c^2\cdot\frac{\partial^2 u}{\partial x^2}

As you can see, you need to calculate the second partial derivatives of the specified function


u(x,t)=cos⁡(αcx)⋅sin⁡(αt)u(x,t)=\cos(\alpha cx)\cdot\sin(\alpha t)

Then,


∂u∂x=∂∂x(cos⁡(αcx)⋅sin⁡(αt))=ddx(cos⁡(αcx))⋅sin⁡(αt)=\frac{\partial u}{\partial x}=\frac{\partial}{\partial x}\left(\cos(\alpha cx)\cdot\sin(\alpha t)\right)=\frac{d}{dx}\left(\cos(\alpha cx)\right)\cdot\sin(\alpha t)==−cα⋅sin⁡(αcx)⋅sin⁡(αt)→=-c\alpha\cdot\sin(\alpha cx)\cdot\sin(\alpha t)\rightarrow∂2u∂x2=∂∂x(∂u∂x)=∂∂x(−cα⋅sin⁡(αcx)⋅sin⁡(αt))=\frac{\partial^2 u}{\partial x^2}=\frac{\partial}{\partial x}\left(\frac{\partial u}{\partial x}\right)=\frac{\partial}{\partial x}\left(-c\alpha\cdot\sin(\alpha cx)\cdot\sin(\alpha t)\right)==ddx(−cα⋅sin⁡(αcx))⋅sin⁡(αt)=−c2α2⋅cos⁡(αcx)⋅sin⁡(αt)=\frac{d}{dx}\left(-c\alpha\cdot\sin(\alpha cx)\right)\cdot\sin(\alpha t)=-c^2\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)

Conclusion,


∂2u∂x2=−c2α2⋅cos⁡(αcx)⋅sin⁡(αt)\boxed{\frac{\partial^2 u}{\partial x^2}=-c^2\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)}

Then,


∂u∂t=∂∂t(cos⁡(αcx)⋅sin⁡(αt))=cos⁡(αcx)⋅ddt(sin⁡(αt))=\frac{\partial u}{\partial t}=\frac{\partial}{\partial t}\left(\cos(\alpha cx)\cdot\sin(\alpha t)\right)=\cos(\alpha cx)\cdot\frac{d}{dt}\left(\sin(\alpha t)\right)==α⋅cos⁡(αcx)⋅cos⁡(αt)→=\alpha\cdot\cos(\alpha cx)\cdot\cos(\alpha t)\rightarrow∂2u∂t2=∂∂t(∂u∂t)=∂∂t(α⋅cos⁡(αcx)⋅cos⁡(αt))=\frac{\partial^2 u}{\partial t^2}=\frac{\partial}{\partial t}\left(\frac{\partial u}{\partial t}\right)=\frac{\partial}{\partial t}\left(\alpha\cdot\cos(\alpha cx)\cdot\cos(\alpha t)\right)==cos⁡(αcx)⋅ddt(α⋅cos⁡(αt))=−α2⋅cos⁡(αcx)⋅sin⁡(αt)=\cos(\alpha cx)\cdot\frac{d}{dt}\left(\alpha\cdot\cos(\alpha t)\right)=-\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)

Conclusion,


∂2u∂t2=−α2⋅cos⁡(αcx)⋅sin⁡(αt)\boxed{\frac{\partial^2 u}{\partial t^2}=-\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)}


Substitute all found derivatives in the specified one-dimensional wave equation equation:


∂2u∂t2=c2⋅∂2u∂x2→\frac{\partial^2 u}{\partial t^2}=c^2\cdot\frac{\partial^2 u}{\partial x^2}\rightarrow−α2⋅cos⁡(αcx)⋅sin⁡(αt)=c2⋅(−c2α2⋅cos⁡(αcx)⋅sin⁡(αt))→-\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)=c^2\cdot\left(-c^2\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)\right)\rightarrow−α2⋅cos⁡(αcx)⋅sin⁡(αt)=−c4α2⋅cos⁡(αcx)⋅sin⁡(αt)→-\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)=-c^4\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)\rightarrowc4α2⋅cos⁡(αcx)⋅sin⁡(αt)−α2⋅cos⁡(αcx)⋅sin⁡(αt)=0→c^4\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)-\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)=0\rightarrow(c4−1)⋅α2⋅cos⁡(αcx)⋅sin⁡(αt)=0→\left(c^4-1\right)\cdot\alpha^2\cdot\cos(\alpha cx)\cdot\sin(\alpha t)=0\rightarrowc4−1=0→(c2−1)(c2+1)=0→(c−1)(c+2)(c2+1)=0→c^4-1=0\rightarrow (c^2-1)(c^2+1)=0\rightarrow (c-1)(c+2)(c^2+1)=0\rightarrowc−1=0orc+1=0orc2+1=0→c-1=0\quad or\quad c+1=0\quad or\quad c^2+1=0\rightarrowc=1orc=−1orc∈∅c=1\quad or\quad c=-1\quad or\quad c\in\varnothing

ANSWER

c=±1\boxed{c=\pm 1}


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