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Consider the conic \(5 x^{2}-4 x y+2 y^{2}=30\) a. Write the left side in matrix form. b. Diagonalize the coefficient matrix, finding the eigenvalues and eigenvectors. c. Construct the rotation matrix from the information in part b. What is the angle of rotation needed to bring the conic into standard form? d. What is the conic?

Short Answer

Expert verified
The given conic’s standard form is an ellipse with the rotation matrix as \[\begin{bmatrix},2/\sqrt{13} & 1\3/\sqrt{13} & 0\end{bmatrix}\]and the angle of rotation as approximately \(56.31^{\circ}\).

Step by step solution

01

Write the Equation in Matrix Form

Firstly, consider the conic equation \(5 x^{2}-4 x y+2 y^{2}=30\). We can write this equation in matrix form as follows:\[\begin{bmatrix}x\y\end{bmatrix}\begin{bmatrix}5 & -2\-2 & 2\end{bmatrix}\begin{bmatrix}x\y\end{bmatrix}= 30\]We have our coefficient matrix as \[A = \begin{bmatrix}5 & -2\-2 & 2\end{bmatrix}\]
02

Diagonalize the Coefficient Matrix

To find the eigenvalues of the matrix A, it is needed to solve the characteristic equation, \(\text{det}(A - \lambda I) = 0\), where I is the identity matrix and \(\lambda\) represent the eigenvalues. We calculate the eigenvalue as follows:\(\text{det}(A - \lambda I) = \text{det}(\begin{bmatrix}5-\lambda & -2\-2 & 2-\lambda\end{bmatrix}) = 0\)This gives the equation \((5 - \lambda)(2 - \lambda) - 4 = 0\), which simplifies to \(\lambda^2 -7\lambda + 10 = 0\). Solving this quadratic equation, we find the roots \(\lambda = 2, 5\), so these are the eigenvalues of matrix A.Next, to find the eigenvectors, we solve the equation \(A v = \lambda v\)For each eigenvalue:For \(\lambda = 2\): We have\(\begin{bmatrix}5-2 & -2\-2 & 2-2\end{bmatrix}v = 0\)which simplifies to \(\begin{bmatrix}3 & -2\-2 & 0\end{bmatrix}v = 0\)Solve this system and one will have \(\mathbf{v}= (2, 3)\) as an eigenvector.Next, for \(\lambda = 5\):This gives\(\begin{bmatrix}5 - 5 & -2\-2 & 2 - 5\end{bmatrix}v = 0\)which simplifies to \(\begin{bmatrix}0 & -2\-2 & -3\end{bmatrix}v = 0\)Solve this system and one will have \(\mathbf{v}= (1, 0)\) as an eigenvector.
03

Construct the rotation matrix and compute the angle of rotation

The rotation matrix can be constructed from the eigenvectors. Since each column of a rotation matrix are just the normalized eigenvectors of the matrix A, we have:\[R = \begin{bmatrix}2/\sqrt{13} & 1\3/\sqrt{13} & 0\end{bmatrix}\]The angle of rotation \(\theta\) can be calculated from the first column of the rotation matrix. Using the formula \(\theta = \arctan\left(\frac{y}{x}\right)\) (where \(x\) and \(y\) are the first and second elements of the first column in the above rotation matrix, respectively), we get \(\theta = \arctan(\frac{3/\sqrt{13}}{2/\sqrt{13}}) = \arccos(2/\sqrt{13})\) which can be simplified to \(\theta \approx 56.31^{\circ}\)
04

Identify the Conic

After rotating the conic by \(\theta\), we obtain the standard form of the conic. Since the eigenvalues are both positive and different from each other, the conic is an ellipse.

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Key Concepts

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

Matrix Diagonalization
Matrix diagonalization is the process of transforming a given matrix into a diagonal form, where all the elements outside the main diagonal are zero. This is incredibly valuable, as diagonal matrices are much easier to work with, particularly in computations involving powers and exponentials.
Here's a simple breakdown of the process:
  • Start with a square matrix, like our coefficient matrix \( A = \begin{bmatrix} 5 & -2 \ -2 & 2 \end{bmatrix} \).
  • Find the eigenvalues by solving the characteristic equation \( \text{det}(A - \lambda I) = 0 \), where \( I \) is the identity matrix.
  • Solve this equation systematically to find \( \lambda \), which are the eigenvalues.
  • With the eigenvalues, proceed to calculate the eigenvectors, which will help us in diagonalizing the matrix.
Once successfully diagonalized, the matrix reveals its intrinsic properties more clearly and can be manipulated or rotated as needed for specific applications, such as conic sections.
Eigenvalues and Eigenvectors
Eigenvalues and eigenvectors are critical concepts in linear algebra, pivotal in various applications like identifying the natural modes of systems or, in our case, rotating conic sections.
Here's what you need to know:
  • An **eigenvalue** \( \lambda \) is a scalar that indicates how a transformation changes the magnitude of a vector, the eigenvector.
  • An **eigenvector** \( \mathbf{v} \) is a non-zero vector that only changes by a scalar factor when a linear transformation is applied.
For our matrix \( A \):
  • The eigenvalues were found to be \( \lambda = 2 \) and \( \lambda = 5 \).
  • With the eigenvalue \( \lambda = 2 \), the eigenvector is \( \mathbf{v} = (2, 3) \).
  • For \( \lambda = 5 \), the eigenvector is \( \mathbf{v} = (1, 0) \).
By applying these, we not only diagonalize the matrix but also understand how the original conic can be transformed into its standard form.
Rotation Matrix
The rotation matrix allows us to rotate a conic section in 2D space so that it can be easier to analyze, often expressing it in its standard form.
The key steps to construct a rotation matrix are:
  • Use the eigenvectors of the matrix \( A \) as the columns of the rotation matrix.
  • Normalize these vectors to maintain the orthogonality and proper statistical properties of a rotation matrix.
In our example:
  • We constructed the rotation matrix \( R \) as \( \begin{bmatrix} 2/\sqrt{13} & 1 \ 3/\sqrt{13} & 0 \end{bmatrix} \).
  • Each eigenvector’s components define the directions for each axis after rotation.
  • The rotation angle \( \theta \) can then be determined using the arctangent or arccosine functions, calculated in our case to be approximately \( 56.31^{\circ} \).
Understanding and utilizing the rotation matrix is crucial for adjusting the orientation of conic sections or any geometric transformations.
Standard Form of Conic
Converting a conic section into its standard form simplifies analysis and interpretation. The standard form is more intuitive and indicates the type and properties of the conic.
Here is how you find and interpret the standard form of a conic:
  • Once the conic equation is rotated using the rotation matrix, it transforms into its standard form with aligned axes.
  • For an equation like ours, with distinct positive eigenvalues, the conic becomes an ellipse.
Recognizing the standard form:
  • An ellipse will have the standard form \( \frac{x^2}{a^2} + \frac{y^2}{b^2} = 1 \).
  • Once identified, properties like axes lengths and orientations are easily derived from the coefficients of the equation.
By transforming the initial equation into standard form, complex geometric problems become much more accessible and understandable.

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Most popular questions from this chapter

Consider the following systems. For each system, determine the coefficient matrix. When possible, solve the eigenvalue problem for each matrix and use the eigenvalues and eigenvectors to provide solutions to the given systems. Finally, in the common cases that you investigated in Problem 2.31, make comparisons with your previous answers, such as what type of eigenvalues correspond to stable nodes. a. $$ \begin{aligned} &x^{\prime}=3 x-y \\ &y^{\prime}=2 x-2 y \end{aligned} $$ b. $$ \begin{aligned} &x^{\prime}=-y_{t} \\ &y^{\prime}=-5 x \end{aligned} $$ c. $$ \begin{aligned} &x^{\prime}=x-y_{r} \\ &y^{\prime}=y \end{aligned} $$ d. $$ \begin{aligned} &x^{\prime}=2 x+3 y \\ &y^{\prime}=-3 x+2 y \end{aligned} $$ e. $$ \begin{aligned} x^{\prime} &=-4 x-y \\ y^{\prime} &=x-2 y \end{aligned} $$ \(\mathrm{f}\). $$ \begin{aligned} x^{\prime} &=x-y \\ y^{\prime} &=x+y \end{aligned} $$

The Pauli spin matrices in quantum mechanics are given by the following matrices: \(\sigma_{1}=\left(\begin{array}{ll}0 & 1 \\ 1 & 0\end{array}\right), \sigma_{2}=\left(\begin{array}{cc}0 & -i \\ i & 0\end{array}\right)\), and \(\sigma_{3}=\left(\begin{array}{cc}1 & 0 \\ 0 & -1\end{array}\right) .\) Show that a. \(\sigma_{1}^{2}=\sigma_{2}^{2}=\sigma_{3}^{2}=I\). b. \(\left\\{\sigma_{i}, \sigma_{j}\right\\} \equiv \sigma_{i} \sigma_{j}+\sigma_{j} \sigma_{i}=2 \delta_{i j} I\), for \(i, j=1,2,3\) and \(I\) the \(2 \times 2\) identity matrix. \(\\{,\),\(} is the anti-commutation operation.\) c. \(\left[\sigma_{1}, \sigma_{2}\right] \equiv \sigma_{1} \sigma_{2}-\sigma_{2} \sigma_{1}=2 i \sigma_{3}\) and similarly for the other pairs. \([,\), is the commutation operation. d. Show that an arbitrary \(2 \times 2\) matrix \(M\) can be written as a linear combination of Pauli matrices, \(M=a_{0} I+\sum_{j=1}^{3} a_{j} \sigma_{j}\), where the \(a_{j}^{\prime}\) s are complex numbers.

You make 2 quarts of salsa for a party. The recipe calls for 5 teaspoons of lime juice per quart, but you had accidentally put in 5 tablespoons per quart. You decide to feed your guests the salsa anyway. Assume that the guests take a quarter cup of salsa per minute and that you replace what was taken with chopped tomatoes and onions without any lime juice. [ 1 quart = 4 cups and \(1 \mathrm{~Tb}=3\) tsp.] a. Write the differential equation and initial condition for the amount of lime juice as a function of time in this mixture-type problem. b. Solve this initial value problem. c. How long will it take to get the salsa back to the recipe's suggested concentration?

Express the vector \(\mathbf{v}=(1,2,3)\) as a linear combination of the vectors \(\mathbf{a}_{1}=(1,1,1), \mathbf{a}_{2}=(1,0,-2)\), and \(\mathbf{a}_{3}=(2,1,0)\)

Consider the matrix $$ A=\left(\begin{array}{ccc} \frac{1}{2} & \frac{1}{\sqrt{2}} & \frac{1}{2} \\ -\frac{1}{\sqrt{2}} & 0 & \frac{1}{\sqrt{2}} \\ \frac{1}{2} & -\frac{1}{\sqrt{2}} & \frac{1}{2} \end{array}\right) $$ a. Verify that this is a rotation matrix. b. Find the angle and axis of rotation. c. Determine the corresponding similarity transformation using the results from part b.

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