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Test the sets of matrices for linear independence in \(M_{22^{*}}\) For those that are linearly dependent, express one of the matrices as a linear combination of the others. $$\left\\{\left[\begin{array}{rr} 1 & 1 \\ 0 & -1 \end{array}\right],\left[\begin{array}{rr} 1 & -1 \\ 1 & 0 \end{array}\right],\left[\begin{array}{rr} 1 & 0 \\ 3 & 2 \end{array}\right]\right\\}$$

Short Answer

Expert verified
The matrices are linearly dependent.

Step by step solution

01

Understand the problem

We need to determine whether the given set of matrices is linearly independent. If they are linearly dependent, we'll express one matrix as a combination of the others.
02

Define linear independence

Matrices are linearly independent if the only solution to the equation \( c_1A_1 + c_2A_2 + c_3A_3 = 0 \) is \( c_1 = c_2 = c_3 = 0 \), where \( A_1, A_2, \) and \( A_3 \) are the given matrices.
03

Set up the matrix equation

Substitute the matrices: \[ c_1 \begin{bmatrix} 1 & 1 \ 0 & -1 \end{bmatrix} + c_2 \begin{bmatrix} 1 & -1 \ 1 & 0 \end{bmatrix} + c_3 \begin{bmatrix} 1 & 0 \ 3 & 2 \end{bmatrix} = \begin{bmatrix} 0 & 0 \ 0 & 0 \end{bmatrix} \] Combine the matrices terms.
04

Combine matrix equations

Combine corresponding terms: \[ \begin{bmatrix} c_1 + c_2 + c_3 & c_1 - c_2 \ c_2 + 3c_3 & -c_1 + 2c_3 \end{bmatrix} = \begin{bmatrix} 0 & 0 \ 0 & 0 \end{bmatrix} \] Now solve for \(c_1, c_2, c_3\).
05

Solve the system of equations

This gives us the equations: 1. \( c_1 + c_2 + c_3 = 0 \) 2. \( c_1 - c_2 = 0 \) 3. \( c_2 + 3c_3 = 0 \) 4. \( -c_1 + 2c_3 = 0 \)
06

Solve systems for variables

From equation 2: \( c_1 = c_2 \)From equation 3: \( c_2 = -3c_3 \)Substitute into equation 1:\( c_2 - 3c_3 + c_3 = 0 \)
07

Continue solving

Substituting values:\( c_1 = -3c_3 \), \( c_2 = -3c_3 \). Substitute \(c_1 = -3c_3 \) into equation 4: \( -(-3c_3) + 2c_3 = 0 \) gives \( 3c_3 - 2c_3 = 0 \), resulting in \( c_3 = 0 \).
08

Check result consistency

Back-substitute \( c_3 = 0 \): \( c_2 = 0 \) and \( c_1 = 0 \). The solution indicates the set is linearly independent, contrary to previous dependence assumption. The initial matrix combine was incorrect.

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Key Concepts

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

Linear Combinations
Understanding linear combinations is key to grasping the concept of linear independence. A linear combination involves combining multiple elements, such as vectors or matrices, by multiplying each one by a constant and then summing the results. In our exercise, the matrices were combined as follows: \( c_1A_1 + c_2A_2 + c_3A_3 = 0 \).
A linear combination is often used to determine if a set of elements is independent by examining if they can express each other. When matrices, for instance, can be written as a linear combination of others, it indicates dependence. In our example:
  • Matrix 1: \( A_1 = \begin{bmatrix} 1 & 1 \ 0 & -1 \end{bmatrix} \)
  • Matrix 2: \( A_2 = \begin{bmatrix} 1 & -1 \ 1 & 0 \end{bmatrix} \)
  • Matrix 3: \( A_3 = \begin{bmatrix} 1 & 0 \ 3 & 2 \end{bmatrix} \)
The test for independence involves finding if all coefficients \( c_1, c_2, \) and \( c_3 \) are zero in a non-trivial solution. A non-zero solution indicates dependency, showing how one or more elements are redundant and do not add new information to the system.
Matrix Equations
Matrix equations help us express complex relationships between matrices and can aid in testing linear independence. A matrix equation, in general, is an expression where matrices are equal, often used to solve unknowns. In the exercise, matrices \( A_1, A_2, \) and \( A_3 \) were used to form a matrix equation.
Substituting into our equation:\[c_1\begin{bmatrix} 1 & 1 \ 0 & -1 \end{bmatrix} + c_2\begin{bmatrix} 1 & -1 \ 1 & 0 \end{bmatrix} + c_3\begin{bmatrix} 1 & 0 \ 3 & 2 \end{bmatrix} = \begin{bmatrix} 0 & 0 \ 0 & 0 \end{bmatrix}\]This equation describes how combinations of the matrices add to zero when balanced correctly through their coefficients. Such equations are critical in understanding the nature of matrices and their interdependencies. Being able to set up these equations correctly is vital to address problems in linear algebra, offering a foundation to solve for unknown variables and verifying conditions such as linear dependence.
Solution of Systems of Equations
The solution of systems of equations involves finding values that satisfy all given equations simultaneously. In testing for linear independence, this often means evaluating if all coefficients must be zero. From the previous step of combining equations, we derived the system:
1. \( c_1 + c_2 + c_3 = 0 \)
2. \( c_1 - c_2 = 0 \)
3. \( c_2 + 3c_3 = 0 \)
4. \( -c_1 + 2c_3 = 0 \)
Simplifying these equations is essential in understanding the dependence or independence of the system. In our solution:
  • Using equation 2, we solved for \( c_1 \) as \( c_1 = c_2 \).
  • Equation 3 gave us \( c_2 = -3c_3 \).
  • Substituting all knowns back showed \( c_3 = 0 \), resulting in \( c_1 = c_2 = 0 \).
This solution demonstrates that the initial test for dependency was incorrect; in fact, the matrices are linearly independent. Understanding why each variable resolves to zero helps affirm that no matrix in the set can be expressed as a combination of the others.

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Most popular questions from this chapter

A pendulum consists of a mass, called a bob, that is affixed to the end of a string of length \(L\) (see Figure 6.26 . When the bob is moved from its rest position and released, it swings back and forth. The time it takes the pendulum to swing from its farthest right position to its farthest left position and back to its next farthest right position is called the period of the pendulum. (Figure can't copy) Let \(\theta=\theta(t)\) be the angle of the pendulum from the vertical. It can be shown that if there is no resistance, then when \(\theta\) is small it satisfies the differential equation \\[ \theta^{\prime \prime}+\frac{g}{L} \theta=0 \\] where \(g\) is the constant of acceleration due to gravity, approximately \(9.7 \mathrm{m} / \mathrm{s}^{2} .\) Suppose that \(L=1 \mathrm{m}\) and that the pendulum is at rest (i.e., \(\theta=0\) ) at time \(t=0\) second. The bob is then drawn to the right at an angle of \(\theta_{1}\) radians and released. (a) Find the period of the pendulum. (b) Does the period depend on the angle \(\theta_{1}\) at which the pendulum is released? This question was posed and answered by Galileo in \(1638 .\) [Galileo Galilei \((1564-1642)\) studied medicine as a student at the University of Pisa, but his real interest was always mathematics. In \(1592,\) Galileo was appointed professor of mathematics at the University of Padua in Venice, where he taught primarily geometry and astronomy. He was the first to use a telescope to look at the stars and planets, and in so doing, he produced experimental data in support of the Copernican view that the planets revolve around the sun and not the earth. For this, Galileo was summoned before the Inquisition, placed under house arrest, and forbidden to publish his results. While under house arrest, he was able to write up his research on falling objects and pendulums. His notes were smuggled out of Italy and published as Discourses on Two New Sciences in \(1638 .\)

Is \(\mathscr{P}_{2}\) spanned by \(1+x, x+x^{2}, 1+x^{2} ?\)

Let \(T: V \rightarrow W\) be a linear transformation between finite-dimensional vector spaces \(V\) and \(W\). Let \(\mathcal{B}\) and \(\mathcal{C}\) be bases for \(V\) and \(W\), respectively, and let \(A=[T]_{C+B}\). If \(V\) is a vector space, then the dual space of \(V\) is the vector space \(V^{*}=\mathscr{L}(V, \mathbb{R}) .\) Prove that if \(V\) is finitedimensional, then \(V^{*} \cong V\)

Determine whether \(\mathrm{V}\) and \(\mathrm{W}\) are isomorphic. If they are, give an explicit isomorphism \(T: V \rightarrow W\) \(V=S_{3}(\text { symmetric } 3 \times 3 \text { matrices }), W=S_{3}^{\prime}(\) skew symmetric \(3 \times 3\) matrices\()\)

Which of the codes in Exercises are linear codes? $$C=\left\\{\left[\begin{array}{l} 0 \\ 0 \\ 0 \end{array}\right],\left[\begin{array}{l} 1 \\ 0 \\ 1 \end{array}\right],\left[\begin{array}{l} 1 \\ 1 \\ 0 \end{array}\right],\left[\begin{array}{l} 0 \\ 1 \\ 0 \end{array}\right]\right\\}$$

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