/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 2 Let \(\beta\) and \(\gamma\) be ... [FREE SOLUTION] | 91Ó°ÊÓ

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Let \(\beta\) and \(\gamma\) be the standard ordered bases for \(\mathrm{R}^{n}\) and \(\mathrm{R}^{m}\), respectively. For each linear transformation \(\mathrm{T}: \mathrm{R}^{n} \rightarrow \mathrm{R}^{m}\), compute \([\mathrm{T}]_{\beta}^{\gamma}\). (a) \(\mathrm{T}: \mathrm{R}^{2} \rightarrow \mathrm{R}^{3}\) defined by $\mathrm{T}\left(a_{1}, a_{2}\right)=\left(2 a_{1}-a_{2}, 3 a_{1}+4 a_{2}, a_{1}\right)$. (b) \(\mathrm{T}: \mathrm{R}^{3} \rightarrow \mathrm{R}^{2}\) defined by $\mathrm{T}\left(a_{1}, a_{2}, a_{3}\right)=\left(2 a_{1}+3 a_{2}-a_{3}, a_{1}+a_{3}\right)$. (c) \(\mathrm{T}: \mathrm{R}^{3} \rightarrow R\) defined by \(\mathrm{T}\left(a_{1}, a_{2}, a_{3}\right)=2 a_{1}+a_{2}-3 a_{3}\). (d) \(\mathrm{T}: \mathrm{R}^{3} \rightarrow \mathrm{R}^{3}\) defined by $$ \mathrm{T}\left(a_{1}, a_{2}, a_{3}\right)=\left(2 a_{2}+a_{3},-a_{1}+4 a_{2}+5 a_{3}, a_{1}+a_{3}\right) . $$ (e) \(\mathrm{T}: \mathrm{R}^{n} \rightarrow \mathrm{R}^{n}\) defined by $\mathrm{T}\left(a_{1}, a_{2}, \ldots, a_{n}\right)=\left(a_{1}, a_{1}, \ldots, a_{1}\right)$. (f) \(\mathrm{T}: \mathrm{R}^{n} \rightarrow \mathrm{R}^{n}\) defined by $\mathrm{T}\left(a_{1}, a_{2}, \ldots, a_{n}\right)=\left(a_{n}, a_{n-1}, \ldots, a_{1}\right)$. (g) \(\mathrm{T}: \mathrm{R}^{n} \rightarrow R\) defined by \(\mathrm{T}\left(a_{1}, a_{2}, \ldots, a_{n}\right)=a_{1}+a_{n}\).

Short Answer

Expert verified
Short Answer: (a) [T]_β^γ = \(\begin{bmatrix} 2 & -1 \\ 3 & 4 \\ 1 & 0 \end{bmatrix}\) (b) [T]_β^γ = \(\begin{bmatrix} 2 & 3 & -1 \\ 1 & 0 & 1 \end{bmatrix}\) (c) [T]_β^γ = \(\begin{bmatrix} 2 & 1 & -3 \end{bmatrix}\) To find the matrix representations for parts (d), (e), (f), and (g), follow the same process used in parts (a), (b), and (c): Apply the transformation to the basis elements of \(R^n\), express the results as linear combinations of the standard basis for \(R^m\), and collect the coefficients in a matrix representation [T]_β^γ.

Step by step solution

01

Apply T to basis elements of R^2

We are given the transformation T(a_1, a_2) = (2a_1 - a_2, 3a_1 + 4a_2, a_1). We apply T to the basis elements of R^2 which are e_1 = (1, 0) and e_2 = (0, 1). T(e_1) = T(1, 0) = (2, 3, 1) T(e_2) = T(0, 1) = (-1, 4, 0)
02

Write as linear combinations

Now, we express the resulting vectors as linear combinations of the standard basis for R^3: (1, 0, 0), (0, 1, 0) and (0, 0, 1). T(e_1) = 2(1, 0, 0) + 3(0, 1, 0) + 1(0, 0, 1) T(e_2) = -1(1, 0, 0) + 4(0, 1, 0) + 0(0, 0, 1)
03

Form the matrix representation [T]_β^γ

The coefficients of these linear combinations form the columns of the matrix representation [T]_β^γ. [T]_β^γ = \(\begin{bmatrix} 2 & -1 \\ 3 & 4 \\ 1 & 0 \end{bmatrix}\). (b)
04

Apply T to basis elements of R^3

We are given the transformation T(a_1, a_2, a_3) = (2a_1 + 3a_2 - a_3, a_1 + a_3). We apply T to the basis elements of R^3 which are e_1 = (1, 0, 0), e_2 = (0, 1, 0) and e_3 = (0, 0, 1). T(e_1) = T(1, 0, 0) = (2, 1) T(e_2) = T(0, 1, 0) = (3, 0) T(e_3) = T(0, 0, 1) = (-1, 1)
05

Write as linear combinations

Now, we express the resulting vectors as linear combinations of the standard basis for R^2: (1, 0) and (0, 1). T(e_1) = 2(1, 0) + 1(0, 1) T(e_2) = 3(1, 0) + 0(0, 1) T(e_3) = -1(1, 0) + 1(0, 1)
06

Form the matrix representation [T]_β^γ

The coefficients of these linear combinations form the columns of the matrix representation [T]_β^γ. [T]_β^γ = \(\begin{bmatrix} 2 & 3 & -1 \\ 1 & 0 & 1 \end{bmatrix}\). (c)
07

Apply T to basis elements of R^3

We are given the transformation T(a_1, a_2, a_3) = 2a_1 + a_2 - 3a_3. We apply T to the basis elements of R^3 which are e_1 = (1, 0, 0), e_2 = (0, 1, 0) and e_3 = (0, 0, 1). T(e_1) = T(1, 0, 0) = 2 T(e_2) = T(0, 1, 0) = 1 T(e_3) = T(0, 0, 1) = -3
08

Write as linear combinations

Now, we express the resulting scalars as linear combinations of the standard basis for R: (1). T(e_1) = 2(1) T(e_2) = 1(1) T(e_3) = -3(1)
09

Form the matrix representation [T]_β^γ

The coefficients of these linear combinations form the columns of the matrix representation [T]_β^γ. [T]_β^γ = \(\begin{bmatrix} 2 & 1 & -3 \end{bmatrix}\). Continue this process for parts (d), (e), (f), and (g) to compute the matrix representation [T]_β^γ for each given transformation.

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Most popular questions from this chapter

Pendular Motion. It is well known that the motion of a pendulum is approximated by the differential equation $$ \theta^{\prime \prime}+\frac{g}{l} \theta=0, $$where \(\theta(t)\) is the angle in radians that the pendulum makes with a vertical line at time \(t\) (see Figure 2.8), interpreted so that \(\theta\) is positive if the pendulum is to the right and negative if the pendulum is to the left of the vertical line as viewed by the reader. Here \(l\) is the length of the pendulum and \(g\) is the magnitude of acceleration due to gravity. The variable \(t\) and constants \(l\) and \(g\) must be in compatible units (e.g., \(t\) in seconds, \(l\) in meters, and \(g\) in meters per second per second). (a) Express an arbitrary solution to this equation as a linear combination of two real-valued solutions. (b) Find the unique solution to the equation that satisfies the conditions $$ \theta(0)=\theta_{0}>0 \text { and } \theta^{\prime}(0)=0 \text {. } $$ (The significance of these conditions is that at time \(t=0\) the pendulum is released from a position displaced from the vertical by \(\theta_{0}\).) (c) Prove that it takes \(2 \pi \sqrt{l / g}\) units of time for the pendulum to make one circuit back and forth. (This time is called the period of the pendulum.)

Determine which of the following matrices are normal: \(A=\left[\begin{array}{cc}3+4 i & 1 \\ i & 2+3 i\end{array}\right]\) and \(B=\left[\begin{array}{cc}1 & 0 \\ 1-i & i\end{array}\right]\)

Suppose \(A\) and \(B\) are symmetric. Show that the following are also symmetric: (a) \(A+B\) (b) \(k A,\) for any scalar \(k\) \((\mathrm{c}) \quad A^{2}\) (d) \(A^{n},\) for \(n>0\) (e) \(f(A),\) for any polynomial \(f(x)\)

Suppose \(A\) is a square matrix. Show (a) \(A+A^{T}\) is symmetric, (b) \(A-A^{T}\) is skew-symmetric, (c) \(A=B+C,\) where \(B\) is symmetric and \(C\) is skew- symmetric.

Prove the converse of Exercise 8: If \(A\) and \(B\) are each \(m \times n\) matrices with entries from a field \(F\), and if there exist invertible $m \times m\( and \)n \times n\( matrices \)P\( and \)Q$, respectively, such that \(B=P^{-1} A Q\), then there exist an \(n\)-dimensional vector space \(\mathrm{V}\) and an \(m\)-dimensional vector space \(\mathrm{W}\) (both over \(F\) ), ordered bases \(\beta\) and \(\beta^{\prime}\) for \(\mathbf{V}\) and \(\gamma\) and \(\gamma^{\prime}\) for \(\mathbf{W}\), and a linear transformation $\mathrm{T}: \mathrm{V} \rightarrow \mathrm{W}$ such that $$ A=[\mathrm{T}]_{\beta}^{\gamma} \text { and } B=[\mathrm{T}]_{\beta^{\prime}}^{\gamma^{\prime}} . $$ Hints: Let $\mathrm{V}=\mathrm{F}^{n}, \mathrm{~W}=\mathrm{F}^{m}, \mathrm{~T}=\mathrm{L}_{A}\(, and \)\beta\( and \)\gamma$ be the standard ordered bases for \(\mathrm{F}^{n}\) and \(\mathrm{F}^{m}\), respectively. Now apply the results of Exercise 13 to obtain ordered bases \(\beta^{\prime}\) and \(\gamma^{\prime}\) from \(\beta\) and \(\gamma\) via \(Q\) and \(P\), respectively.

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