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Solve the following relations for \(x\) and \(y,\) and compute the Jacobian \(J(u, v)\). $$u=x+y, v=2 x-y$$

Short Answer

Expert verified
In conclusion, given the relations \(u = x + y\) and \(v = 2x - y\), we have found the expressions for \(x(u,v) = \frac{1}{3}(u+v)\) and \(y(u,v) = \frac{2}{3}u - \frac{1}{3}v\). The Jacobian matrix is $$J(u, v) = \begin{bmatrix} \frac{1}{3} & \frac{1}{3} \\ \frac{2}{3} & -\frac{1}{3} \end{bmatrix} $$ with determinant \(\det J(u, v) = -\frac{3}{9}\).

Step by step solution

01

Solve the relations for x and y

Use the given relations to find \(x(u,v)\) and \(y(u,v)\). We have the following system of equations: \[ \begin{cases} u = x+y \\ v = 2x-y \end{cases} \] We can solve this system for \(x\) and \(y\) using any method for solving linear systems, such as substitution or elimination. We will use the elimination method here. Sum the two equations: $$u+v = 3x$$ $$x = \frac{1}{3}(u+v)$$ Substitute this result into the first equation to find the expression for \(y\): $$u = \frac{1}{3}(u+v) + y$$ $$y = u - \frac{1}{3}(u+v) = \frac{2}{3}u - \frac{1}{3}v$$ Now we have the expressions for \(x(u,v)\) and \(y(u,v)\): $$x(u,v) = \frac{1}{3}(u+v), \quad y(u,v) = \frac{2}{3}u - \frac{1}{3}v$$
02

Compute the partial derivatives

Compute the partial derivatives \(\frac{\partial x}{\partial u}\), \(\frac{\partial y}{\partial u}\), \(\frac{\partial x}{\partial v}\), and \(\frac{\partial y}{\partial v}\). Using the expressions for \(x(u,v)\) and \(y(u,v)\), compute the following partial derivatives: $$\frac{\partial x}{\partial u} = \frac{1}{3}, \quad \frac{\partial x}{\partial v} = \frac{1}{3}$$ $$\frac{\partial y}{\partial u} = \frac{2}{3}, \quad \frac{\partial y}{\partial v} = -\frac{1}{3}$$
03

Compute the Jacobian J(u, v)

Form the Jacobian matrix \(J(u, v)\) and compute its determinant. The Jacobian matrix \(J(u, v)\) is given by $$J(u, v) = \begin{bmatrix} \frac{\partial x}{\partial u} & \frac{\partial x}{\partial v} \\ \frac{\partial y}{\partial u} & \frac{\partial y}{\partial v} \end{bmatrix} = \begin{bmatrix} \frac{1}{3} & \frac{1}{3} \\ \frac{2}{3} & -\frac{1}{3} \end{bmatrix} $$ To compute the determinant of \(J(u, v)\), multiply the diagonal entries and subtract the product of the off-diagonal entries: $$\det J(u, v) = \left(\frac{1}{3} \times -\frac{1}{3}\right) - \left(\frac{1}{3} \times \frac{2}{3}\right) = -\frac{1}{9} - \frac{2}{9} = -\frac{3}{9}$$ The Jacobian determinant is given by \(-\frac{3}{9}\).

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Key Concepts

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

Partial Derivatives
In mathematics, partial derivatives are used to measure how a function changes in response to small changes in its input variables. Unlike ordinary derivatives, which apply to functions of a single variable, partial derivatives are applied to functions with multiple variables, like our functions for \(x(u,v)\) and \(y(u,v)\). For these functions, we have two input variables: \(u\) and \(v\).

To find partial derivatives, select one variable to vary while keeping the others constant. For instance, in our solution, when calculating \(\frac{\partial x}{\partial u}\), we keep \(v\) constant and observe how \(x\) changes. Similarly, \(\frac{\partial x}{\partial v}\) involves keeping \(u\) constant.

Partial derivatives help us construct the Jacobian matrix, which provides information about how functions transform input spaces to output spaces. In our solution, these derivatives are:
  • \(\frac{\partial x}{\partial u} = \frac{1}{3}\)
  • \(\frac{\partial x}{\partial v} = \frac{1}{3}\)
  • \(\frac{\partial y}{\partial u} = \frac{2}{3}\)
  • \(\frac{\partial y}{\partial v} = -\frac{1}{3}\)
Linear System of Equations
A linear system of equations consists of multiple linear equations involving the same set of variables. In our scenario, we have a system of two equations:

\[ \begin{cases} u = x+y \ v = 2x-y \end{cases} \]

Often, solving such a system requires methods like substitution or elimination, which simplify the system to find explicit solutions for each unknown variable. Our solution employs the elimination method. By adding and manipulating the given equations, we isolate individual variables.

The elimination method helps us efficiently find expressions for \(x\) and \(y\) in terms of \(u\) and \(v\):
  • \(x(u,v) = \frac{1}{3}(u+v)\)
  • \(y(u,v) = \frac{2}{3}u - \frac{1}{3}v\)
These solutions form the foundation for evaluating the Jacobian matrix and its determinant.
Determinant of a Matrix
The determinant of a matrix is a special number that gives important insights into the properties of the matrix. Specifically, for a 2x2 matrix (like our Jacobian matrix), the determinant is calculated using the formula:

\[ \det J = ad - bc \]

where \(a\), \(b\), \(c\), and \(d\) are the elements of the matrix:

\[ J = \begin{bmatrix} a & b \ c & d \ \end{bmatrix} \]

In our particular case, the Jacobian matrix is:

\[ J(u, v) = \begin{bmatrix} \frac{1}{3} & \frac{1}{3} \ \frac{2}{3} & -\frac{1}{3} \end{bmatrix} \]

Calculating the determinant using the provided formula gives:

\[ \det J(u, v) = \left(\frac{1}{3} \times -\frac{1}{3}\right) - \left(\frac{1}{3} \times \frac{2}{3}\right) = -\frac{1}{9} - \frac{2}{9} = -\frac{3}{9} \]

The determinant value, \(-\frac{3}{9}\), signifies the scaling factor of the transformation represented by the Jacobian matrix, influencing how areas and volumes change under the mapping.

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Most popular questions from this chapter

Use polar coordinates to find the centroid of the following constant-density plane regions. The region bounded by the limaçon \(r=2+\cos \theta\)

Use polar coordinates to find the centroid of the following constant-density plane regions. The semicircular disk \(R=\\{(r, \theta): 0 \leq r \leq 2,0 \leq \theta \leq \pi\\}\)

The Jacobian is a magnification (or reduction) factor that relates the area of a small region near the point \((u, v)\) to the area of the image of that region near the point \((x, y)\) a. Suppose \(S\) is a rectangle in the \(u v\) -plane with vertices \(O(0,0)\) \(P(\Delta u, 0),(\Delta u, \Delta v),\) and \(Q(0, \Delta v)\) (see figure). The image of \(S\) under the transformation \(x=g(u, v), y=h(u, v)\) is a region \(R\) in the \(x y\) -plane. Let \(O^{\prime}, P^{\prime},\) and \(Q^{\prime}\) be the images of O, P, and \(Q,\) respectively, in the \(x y\) -plane, where \(O^{\prime}\) \(P^{\prime},\) and \(Q^{\prime}\) do not all lie on the same line. Explain why the coordinates of \(\boldsymbol{O}^{\prime}, \boldsymbol{P}^{\prime}\), and \(Q^{\prime}\) are \((g(0,0), h(0,0))\) \((g(\Delta u, 0), h(\Delta u, 0)),\) and \((g(0, \Delta v), h(0, \Delta v)),\) respectively. b. Use a Taylor series in both variables to show that $$\begin{aligned} &g(\Delta u, 0) \approx g(0,0)+g_{u}(0,0) \Delta u\\\ &g(0, \Delta v) \approx g(0,0)+g_{v}(0,0) \Delta v\\\ &\begin{array}{l} h(\Delta u, 0) \approx h(0,0)+h_{u}(0,0) \Delta u \\ h(0, \Delta v) \approx h(0,0)+h_{v}(0,0) \Delta v \end{array} \end{aligned}$$ where \(g_{u}(0,0)\) is \(\frac{\partial x}{\partial u}\) evaluated at \((0,0),\) with similar meanings for \(g_{v}, h_{u}\) and \(h_{v}\) c. Consider the vectors \(\overrightarrow{O^{\prime} P^{\prime}}\) and \(\overrightarrow{O^{\prime} Q^{\prime}}\) and the parallelogram, two of whose sides are \(\overrightarrow{O^{\prime} P^{\prime}}\) and \(\overrightarrow{O^{\prime} Q^{\prime}}\). Use the cross product to show that the area of the parallelogram is approximately \(|J(u, v)| \Delta u \Delta v\) d. Explain why the ratio of the area of \(R\) to the area of \(S\) is approximately \(|J(u, v)|\)

Find the center of mass of the region in the first quadrant bounded by the circle \(x^{2}+y^{2}=a^{2}\) and the lines \(x=a\) and \(y=a,\) where \(a > 0\).

The following table gives the density (in units of \(\mathrm{g} / \mathrm{cm}^{2}\) ) at selected points of a thin semicircular plate of radius 3. Estimate the mass of the plate and explain your method. $$\begin{array}{|c|c|c|c|c|c|} \hline & \boldsymbol{\theta}=\mathbf{0} & \boldsymbol{\theta}=\boldsymbol{\pi} / \boldsymbol{4} & \boldsymbol{\theta}=\boldsymbol{\pi} / \boldsymbol{2} & \boldsymbol{\theta}=\boldsymbol{3} \pi / \boldsymbol{4} & \boldsymbol{\theta}=\boldsymbol{\pi} \\ \hline \boldsymbol{r}=\mathbf{1} & 2.0 & 2.1 & 2.2 & 2.3 & 2.4 \\ \hline \boldsymbol{r}=\mathbf{2} & 2.5 & 2.7 & 2.9 & 3.1 & 3.3 \\ \hline \boldsymbol{r}=\mathbf{3} & 3.2 & 3.4 & 3.5 & 3.6 & 3.7 \\ \hline \end{array}$$

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