Chapter 10: Problem 17
\(f(x, y)=y\)
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These are the key concepts you need to understand to accurately answer the question.
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Chapter 10: Problem 17
\(f(x, y)=y\)
These are the key concepts you need to understand to accurately answer the question.
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\(f(x)=e^{-x}\) \(0<\) \(x<\) 1
$$ \frac{\partial^{2} u}{\partial t^{2}} $$ \(=\frac{\partial^{2} u}{\partial x^{2}}+x \sin t\), \(0\)<\(x\)<\(\pi\), \(t>0\) $$ u(0, t) $$ \(=u(\pi, t)=0\) \(t>0\), $$ u(x, 0)=0 $$, \(0\)<\(x\)<\(\pi\), $$ \frac{\partial u}{\partial t}(x, 0) $$ \(=0\), \(0\)<\(x\)<\(\pi\)
\(f(x)=x(\pi-x)\)
Fluid Flow Around a Corner. The stream lines that describe the fluid flow around a corner (see Figure 10.28\()\) are given by \(\phi(x, y)=k,\) where \(k\) is a constant and \(\phi\) the stream function, satisfies the boundary value problem (a) Using the results of Problem \(22,\) show that this problem can be reduced to finding the flow above a flat plate (see Figure 10.29 ). That is, show that the problem reduces to finding the solution to \(\frac{\partial^{2} \psi}{\partial u^{2}}+\frac{\partial^{2} \psi}{\partial v^{2}}=0, \quad v>0, \quad-\infty< u <\infty,\) \(\psi(u, 0)=0, \quad-\infty< u <\infty,\) where \(\quad \psi \quad\) and \(\quad \phi \quad\) are related as follows: \(\psi(u, v)=\phi(x(u, v), y(u, v)) \quad\) with the \(\quad\) mapping between \((u, v)\) and \((x, y)\) given by the analytic function \(f(z)=z^{2} .\) (b) Verify that a nonconstant solution to the problem in part (a) is given by \(\psi(u, v)=v.\) (c) Using the result of part (b), find a stream function \(\phi(x, y)\) for the original problem.
$$\frac{\partial u}{\partial t}=3 \frac{\partial^{2} u}{\partial x^{2}}+x, 0<\mathcal{x}<\pi,t>0,$$ $$u(0, t)=u(\pi, t)=0, \quad t>0,$$ $$u(x, 0)=\sin x,0<\mathcal{x}<\pi$$
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