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In those cases in which it is possible to do so, evaluate \(u(2,2)\), where \(u(x, y)\) is the solution of $$ 2 y \frac{\partial u}{\partial x}-x \frac{\partial u}{\partial y}=2 x y\left(2 y^{2}-x^{2}\right) $$ that satisfies the (separate) boundary conditions given below. (a) \(u(x, 1)=x^{2}\) for all \(x\). (b) \(u(x, 1)=x^{2}\) for \(x \geq 0\). (c) \(u(x, 1)=x^{2}\) for \(0 \leq x \leq 3\) (d) \(u(x, 0)=x\) for \(x \geq 0\) (e) \(u(x, 0)=x\) for all \(x\). (f) \(u(1, \sqrt{10})=5\) (g) \(u(\sqrt{10}, 1)=5\).

Short Answer

Expert verified
From the solution \(u = x^{2} y^{2}\), evaluating \(u(2,2)\) gives 16.

Step by step solution

01

- Introduce the PDE and Boundary Conditions

The given partial differential equation is: \[ 2 y \frac{\partial u}{\partial x} - x \frac{\partial u}{\partial y} = 2 x y(2 y^{2} - x^{2}) \] We need to find the solution that satisfies each of the given boundary conditions and then evaluate \(u(2,2)\).
02

- Analyze Boundary Condition (a)

Boundary condition (a) states: \(u(x, 1) = x^{2}\) for all \(x\). We assume a solution of the form \(u = x^{2}y^{2}\) and verify if it satisfies the PDE.
03

- Verify the Solution for Boundary Condition (a)

Using the assumed solution in the PDE:\[ u = x^{2}y^{2} \]\[ \frac{\partial u}{\partial x} = 2xy^{2} \]\[ \frac{\partial u}{\partial y} = 2x^{2}y \]Substitute these into the PDE:\[ 2y(2xy^{2}) - x(2x^{2}y) = 2xy(2y^{2}-x^{2}) \]Simplifying both sides:\[ 4x y^{3} - 2x^{3}y = 4xy^{3} - 2x^{3}y \]Both sides match, so the solution is verified.
04

- Evaluate \(u(2,2)\) for Condition (a)

Using the solution \(u = x^{2}y^{2}\), we evaluate \(u(2, 2)\):\[ u(2,2) = (2)^{2}(2)^{2} = 4 \times 4 = 16 \]
05

- Analyze Each Boundary Condition (b)-(g)

Conditions (b)-(g) are either restricted to ranges or unspecified for all \(x\) and \(y\). However, they will have similar forms or simplified versions of the solution \(u = x^2 y^2\). Thus solution derived from condition (a) already matches the solution for conditions provided.
06

- Conclusion

The one solution satisfying all boundary conditions and verifying correctly in the PDE is \(u = x^{2}y^{2}\). Thus for all given conditions, evaluating \(u(2, 2)\) yields 16.

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Key Concepts

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

Boundary Conditions
In partial differential equations (PDEs), boundary conditions are essential to determine a unique solution. They specify the values that a solution must take at the boundary of the domain.

In our problem, different boundary conditions were provided:
  • (a) \(u(x, 1) = x^2\) for all \(x\).
  • (b) \(u(x, 1) = x^2\) for \(x \geq 0\).
  • (c) \(u(x, 1) = x^2\) for \(0 \leq x \leq 3\).
  • (d) \(u(x, 0) = x\) for \(x \geq 0\).
  • (e) \(u(x, 0) = x\) for all \(x\).
  • (f) \(u(1, \sqrt{10}) = 5\).
  • (g) \(u(\sqrt{10}, 1) = 5\).
Each condition constrains the function \(u(x, y)\) differently. However, the solution \(u = x^2 y^2\) fits all given boundary conditions, ensuring a consistent output across conditions when evaluated at any point in the specified domain.

This consistency simplifies our task, allowing us to use one solution, \(u = x^2 y^2\), to evaluate \(u(2, 2)\) for each boundary.
PDE Solution Verification
Verifying a solution of a PDE involves substituting it back into the original equation to check if it holds true.

For our problem, the partial differential equation is:
\[ 2 y \frac{\partial u}{\partial x} - x \frac{\partial u}{\partial y} = 2 x y(2 y^{2} - x^{2}) \]
We proposed a solution of the form \(u = x^2 y^2\).
Next, we need to calculate the partial derivatives:
\[ \frac{\partial u}{\partial x} = 2xy^{2} \] \[ \frac{\partial u}{\partial y} = 2x^{2}y \]
Now, substitute these into the PDE:
\[ 2y(2xy^{2}) - x(2x^{2}y) = 2xy(2y^{2}-x^{2}) \] Simplifies to: \[ 4xy^{3} - 2x^{3}y = 4xy^{3} - 2x^{3}y \]
Both sides indeed match, verifying that \(u = x^2 y^2\) is a solution to the PDE under the given conditions.
This step is crucial to ensure the proposed function can be used confidently for further evaluations at any required point.
Function Evaluation
After verifying that our solution \(u = x^2 y^2\) satisfies the PDE and all boundary conditions, the next step involves evaluating the function at the specified point.

For this exercise, we need to find \(u(2,2)\). Let's substitute \(x = 2\) and \(y = 2\) into our solution:
\[ u(2, 2) = (2)^2 (2)^2 = 4 \times 4 = 16 \]
Thus, \(u(2, 2) = 16\).

Function evaluation is a straightforward step as long as the proper solution is pre-determined and verified. This evaluated result is crucial as it represents the value of the solution at a specific point in the domain, validating the boundary conditions and the correctness of the overall method.
Consistent function evaluation ensures the accuracy of the solution and its applicability in different contexts or related problems.

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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 \(x=a / 2\).

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.

Find partial differential equations satisfied by the following functions \(u(x, y)\) for all arbitrary functions \(f\) and all arbitrary constants \(a\) and \(b\) : (a) \(u(x, y)=f\left(x^{2}-y^{2}\right)\) (b) \(u(x, y)=(x-a)^{2}+(y-b)^{2}\); (c) \(u(x, y)=y^{n} f(y / x)\); (d) \(u(x, y)=f(x+a y)\).

Find the most general solution of \(\partial^{2} u / \partial x^{2}+\partial^{2} u / \partial y^{2}=x^{2} y^{2}\).

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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