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If \(u(x, y)\) satisfies $$ \frac{\partial^{2} u}{\partial x^{2}}-3 \frac{\partial^{2} u}{\partial x \partial y}+2 \frac{\partial^{2} u}{\partial y^{2}}=0 $$ and \(u=-x^{2}\) and \(\partial u / \partial y=0\) for \(y=0\) and all \(x\), find the value of \(u(0,1)\).

Short Answer

Expert verified
Plugging this u(x.y) we have u(0,1)=solve system equations.

Step by step solution

01

Understand the Partial Differential Equation (PDE)

The given PDE is: \[ \frac{\frac{\text{{partial}}^2 u}{\text{{partial}} x^2}}-\frac{3}{\text{{partial}}^2 u}{\text{{partial}} x \text{{partial}}}y + \frac{\text{{2}}}{\text{{partial}}^2 u}{\text{{partial}} y^2} \text{{=}}0 \]. This equation must be satisfied by the potential solution u(x,y).
02

Apply Given Boundary Conditions at y=0

For \(y = 0\), \(u = -x^2\) and \({\frac{\text{{partial}}u}{\text{{partial}} y}}= 0\). This information will help in reducing the PDE to solve for the more specific conditions.
03

Solve for the General Form of u(x,y)

Since \({\frac{\text{{partial}} u}{\text{{partial x^2}}}} = 2\), \({\frac{\text{{partial}} u}{\text{{partial}} x \text{{partial}}}y} - 3 {\text{{partial}}^{2}} n = 2 {\text{{partial}}^{2}} B \text{{partial}}^{2} y^{1.5}} = 0\).
04

Consider u(x,y) = ax^2+bxy+cy^2+d

Plugging this form back into PDE and using boundary conditions solve System of Equations to find a, b, c, and d.
05

Evaluate at given point u(0,1)

To find u(0,1) from the solution derived.

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Key Concepts

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

boundary conditions
Boundary conditions are essential in solving partial differential equations (PDEs). They provide additional constraints that help determine a specific solution from the general solutions of the PDE.

In our example, we have two boundary conditions at y = 0:
  • u = -x^2
  • ∂u/∂y = 0
These conditions specify the function value and its derivative at particular points. Without them, the PDE could have infinite possible solutions. Boundary conditions guide us to the one solution that fits the given physical or geometrical context.

When applying boundary conditions:
  • First, incorporate them into the PDE to reduce complexity.
  • Then, use these simplified forms to solve for specific constants or functions.
general solution of PDE
The general solution of a PDE includes all possible solutions before any boundary conditions are applied. In our case, the PDE is:

$$\frac{\frac{\text{{partial}}^2 u}{\text{{partial}} x^2}}-3 \frac{\frac{\text{{partial}}^2 u}{\text{{partial}} x \text{{partial}} y}}+2 \frac{\frac{\text{{partial}}^2 u}{\text{{partial}} y^2}}=0$$.

To find the general solution, we first need to propose a general form for u(x, y). One common approach is to assume a polynomial form, say u(x, y) = ax^2 + bxy + cy^2 + dx + ey + f. This form includes all possible terms up to the second order, which should encapsulate all potential solutions to our second-order PDE.

Plug this general form back into the PDE, and you will get a system of equations for the coefficients a, b, c, d, e, and f. Solving these equations yields expressions for these coefficients, which gives the general solution.

Next, enforce boundary conditions upon this general solution, which leads us to a specific solution that satisfies both the PDE and the boundary conditions.
method of characteristics
The method of characteristics is a technique to solve certain types of PDEs, particularly useful in first-order linear and quasilinear PDEs. It transforms a PDE into a set of ordinary differential equations (ODEs) by tracing the paths (characteristics) along which the PDE becomes an ODE.

Here's a simplified overview of the technique:
  • Identify characteristic curves in the domain where the PDE can be simplified.
  • Transform the PDE into a set of ODEs along these curves.
  • Solve these ODEs to find the solution of the original PDE.
The method is valuable because it leverages the characteristic directions in the solution space where the problem simplifies, making it easier to solve complex PDEs.

In our given PDE, you might not directly use the method of characteristics since it typically looks for simpler first-order PDEs. However, the underlying principle of transforming a complex problem into simpler forms still holds true and guides the approach in solving higher-order PDEs by reducing them step by step.
boundary value problems
Boundary value problems (BVPs) involve finding a solution to a differential equation that satisfies specific conditions (boundary conditions) at the boundaries of the domain.

In our case, the boundary conditions at y = 0 provided:
  • u = -x^2
  • ∂u/∂y = 0


These constraints must hold true in the solution at the boundaries (in this case, at y = 0 for all x). Solving BVPs typically involves these steps:
  • Formulating the general solution to the PDE without boundary conditions.
  • Applying the boundary conditions to the general solution.
  • Solving the resulting equations to determine all unknown constants or functions.
The given exercise is a typical boundary value problem where we need to find a specific solution that satisfies the overall PDE and the given boundary conditions.

The steps include:
  • Writing the general form of u(x, y).
  • Plugging in the boundary conditions to solve for specific constants a, b, c, etc.
  • Thus, identifying the unique solution that fits the problem context.

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Most popular questions from this chapter

An infinitely long string on which waves travel at speed \(c\) has an initial displacement $$ y(x)= \begin{cases}\sin (\pi x / a), & -a \leq x \leq a \\ 0, & |x|>a\end{cases} $$ It is released from rest at time \(t=0\), and its subsequent displacement is described by \(y(x, t)\). By expressing the initial displacement as one explicit function incorporating Heaviside step functions, find an expression for \(y(x, t)\) at a general time \(t>0\). In particular, determine the displacement as a function of time (a) at \(x=0\), (b) at \(x=a\), and (c) at \(x=a / 2\).

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 $$ 6 \frac{\partial^{2} u}{\partial x^{2}}-5 \frac{\partial^{2} u}{\partial x \partial y}+\frac{\partial^{2} u}{\partial y^{2}}=14 $$ subject to \(u=2 x+1\) and \(\partial u / \partial y=4-6 x\), both on the line \(y=0\).

Consider each of the following situations in a qualitative way and determine the equation type, the nature of the boundary curve and the type of boundary conditions involved. (a) a conducting bar given an initial temperature distribution and then thermally isolated; (b) two long conducting concentric cylinders on each of which the voltage distribution is specified; (c) two long conducting concentric cylinders on each of which the charge distribution is specified; (d) a semi-infinite string the end of which is made to move in a prescribed way.

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.

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