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Solve the following partial differential equations for \(u(x, y)\) with the boundary conditions given: (a) \(x \frac{\partial u}{\partial x}+x y=u, \quad u=2 y\) on the line \(x=1\) (b) \(1+x \frac{\partial u}{\partial y}=x u, \quad u(x, 0)=x\).

Short Answer

Expert verified
(a) Solution: \(u(x,y)=2ye^{-x}\)(b) Solution: \(u(x,y)=x e^y\)

Step by step solution

01

Identify the Type of PDE

Both equations are first-order linear partial differential equations.
02

Rewrite Equation (a) in Standard Form

Rewrite equation (a): \[ x \frac{\partial u}{\partial x} + xy = u \] Divide both sides by x: \[ \frac{\partial u}{\partial x} + y = \frac{u}{x} \]
03

Solve the Homogeneous Part of (a)

Solve the homogeneous part \(\frac{du}{dx} + u = 0\): \[ \frac{du}{dx} = -u \] Integrate to get: \[ u = Ce^{-x} \]
04

Solve the Non-Homogeneous Part of (a)

For the non-homogeneous term, use variation of parameters: \[ u = Ce^{-x} + e^{-x} \int e^x y dx \] Evaluate the integral and solve to find the constant.
05

Apply Boundary Condition for (a)

Apply the boundary condition \(u = 2y\) when \(x = 1\): \[ u(1, y) = 2y = Ce^{-1} + e^{-1} \int_0^y e^{1} y dy \] Solve for the constant \(C\) and find the solution.
06

Rewrite Equation (b) in Standard Form

Rewrite equation (b): \[ 1 + x \frac{\partial u}{\partial y} = x u \] Divide both sides by x: \[ \frac{1}{x} + \frac{\partial u}{\partial y} = u \]
07

Solve the Homogeneous Part of (b)

Solve the homogeneous part \(\frac{\partial u}{\partial y} = u\): \[ \frac{du}{dy} = u \] Integrate to get: \[ u = C e^y \]
08

Solve the Non-Homogeneous Part of (b)

For the non-homogeneous term, use variation of parameters: \[ u = C e^y + e^y \int (\frac{1}{x}) e^{-y} dy \] Evaluate the integral and solve to find the constant.
09

Apply Boundary Condition for (b)

Apply the boundary condition \(u(x, 0) = x\): \[ u(x, 0) = x = C e^0 + e^0 \int (1/x) x dx \] Solve for the constant \(C\) and find the solution.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

first-order linear PDE
A first-order linear partial differential equation (PDE) has the general form: A first-order linear partial differential equation (PDE) has the general form: \[ a(x,y) \frac{\partial u}{\partial x} + b(x,y) \frac{\partial u}{\partial y} = c(x,y,u) \] The equation involves first-order partial derivatives of the unknown function, \(u\), with respect to the variables \(x\) and \(y\). In simpler terms, it tells how the function \(u\) changes as we move along the \(x\) and \(y\) directions.
boundary conditions
Boundary conditions specify values or behaviors of the solution at specific points or along specific lines. These are critical for finding a unique solution to a PDE. For example, in our exercise:
  • For equation (a), the boundary condition is \(u = 2y\) on the line \(x = 1\).
  • For equation (b), the boundary condition is \(u(x, 0) = x\).
These conditions help us determine integration constants and finalize our solutions.
variation of parameters
Variation of Parameters is a technique used to solve non-homogeneous PDEs. It extends the solution of a homogeneous equation to include the non-homogeneous part. For the exercise:
  • In equation (a), we find the general solution of the homogeneous part and then adjust it by introducing an additional function to account for the non-homogeneous term.
  • For equation (b), similarly, we define the general solution of the homogeneous part and vary the parameters to include the non-homogeneous term.
Mathematically, if the solution to the homogeneous equation is \(u_h\), then for the non-homogeneous equation, we look for a solution of the form \(u = u_h + u_p\).
homogeneous and non-homogeneous equations
A homogeneous PDE has no term that is only a function of the independent variables; it usually has the form: \[ L(u) = 0 \] where \(L\) represents some differential operator applied to \(u\). For example:
  • \( \frac{\text{d}u}{\text{d}x} + u = 0 \ \frac{\text{d}u}{\text{d}y} = u \)
A non-homogeneous PDE contains additional terms that are functions of the independent variables, making the equation look like: \[ L(u) = f(x, y) \] , where \( \ L (u) = u_p \) is a particular solution of the non-homogeneous problem.
integration
Integration is critical in solving PDEs, especially for finding the particular solutions. For instance in our exercise:
  • For equation (a), after isolating the homogeneous component, integrate with respect to \(x\) to find the general solution \( u = Ce^{-x} \).
  • For the non-homogeneous part, we integrate the non-homogeneous term: \( e^{-x} \int e^x y dx \).
  • For equation (b), after solving the homogeneous part and obtaining \( u = Ce^y \), integrate the non-homogeneous part by solving \( e^y \int (\frac{1}{x}) e^{-y} dy \).
In both cases, integrating involves finding the antiderivatives to determine the constants.

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Most popular questions from this chapter

Find the most general solutions \(u(x, y)\) of the following equations consistent with the boundary conditions stated: (a) \(y \frac{\partial u}{\partial x}-x \frac{\partial u}{\partial y}=3 x, \quad u=x^{2}\) on the line \(y=0\); (b) \(y \frac{\partial u}{\partial x}-x \frac{\partial u}{\partial y}=3 x, \quad u(1,0)=2\); (c) \(y^{2} \frac{\partial u}{\partial x}+x^{2} \frac{\partial u}{\partial y}=x^{2} y^{2}\left(x^{3}+y^{3}\right)\), no boundary conditions.

A function \(u(x, y)\) satisfies $$ 2 \frac{\partial u}{\partial x}+3 \frac{\partial u}{\partial y}=10 $$ and takes the value 3 on the line \(y=4 x\). Evaluate \(u(2,4)\).

The non-relativistic Schrödinger equation (18.7) is similar to the diffusion equation in having different orders of derivatives in its various terms; this precludes solutions that are arbitrary functions of particular linear combinations of variables. However, since exponential functions do not change their forms under differentiation, solutions in the form of exponential functions of combinations of the variables may still be possible. Consider the Schrödinger equation for the case of a constant potential, i.e. for a free particle, and show that it has solutions of the form \(A \exp (l x+m y+n z+\lambda t\) ) where the only requirement is that $$ -\frac{\hbar^{2}}{2 m}\left(l^{2}+m^{2}+n^{2}\right)=i \hbar \lambda $$ In particular, identify the equation and wavefunction obtained by taking \(\lambda\) as \(-i E / \hbar\), and \(l, m\) and \(n\) as \(i p_{x} / \hbar, i p_{y} / \hbar\) and \(i p_{z} / \hbar\) respectively, where \(E\) is the energy and \(p\) the momentum of the particle; these identifications are essentially the content of the de Broglie and Einstein relationships.

Like the Schrödinger equation of the previous question, the equation describing the transverse vibrations of a rod, $$ a^{4} \frac{\partial^{4} u}{\partial x^{4}}+\frac{\partial^{2} u}{\partial t^{2}}=0 $$ has different orders of derivatives in its various terms. Show, however, that it has solutions of exponential form \(u(x, t)=A \exp (\lambda x+i \omega t)\) provided that the relation \(a^{4} \lambda^{4}=\omega^{2}\) is satisfied. Use a linear combination of such allowed solutions, expressed as the sum of sinusoids and hyperbolic sinusoids of \(\lambda x\), to describe the transverse vibrations of a rod of length \(L\) clamped at both ends. At a clamped point both \(u\) and \(\partial u / \partial x\) must vanish; show that this implies that \(\cos (\lambda L) \cosh (\lambda L)=1\), thus determining the frequencies \(\omega\) at which the rod can vibrate.

Solve $$ \sin x \frac{\partial u}{\partial x}+\cos x \frac{\partial u}{\partial y}=\cos x $$ subject to (a) \(u(\pi / 2, y)=0\), (b) \(u(\pi / 2, y)=y(y+1)\).

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