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Consider this matrix transformation:

[[0,-1],[1,0]]
What is the geometric effect of this transformation?
Choose 1 answer:
A A reflection across the 
y axis
B A reflection across the line 
y=x
(c) A rotation about the origin by 
90^(@)
(D) A rotation about the origin by 
180^(@)

Consider this matrix transformation:\newline[0amp;11amp;0] \left[\begin{array}{cc} 0 & -1 \\ 1 & 0 \end{array}\right] \newlineWhat is the geometric effect of this transformation?\newlineChoose 11 answer:\newline(A) A reflection across the y y axis\newline(B) A reflection across the line y=x y=x \newline(C) A rotation about the origin by 90 90^{\circ} \newline(D) A rotation about the origin by 180 180^{\circ}

Full solution

Q. Consider this matrix transformation:\newline[0110] \left[\begin{array}{cc} 0 & -1 \\ 1 & 0 \end{array}\right] \newlineWhat is the geometric effect of this transformation?\newlineChoose 11 answer:\newline(A) A reflection across the y y axis\newline(B) A reflection across the line y=x y=x \newline(C) A rotation about the origin by 90 90^{\circ} \newline(D) A rotation about the origin by 180 180^{\circ}
  1. Identify transformation: Identify the matrix transformation.\newlineThe matrix given is:\newline[0amp;1 1amp;0]\begin{bmatrix} 0 & -1 \ 1 & 0 \end{bmatrix}\newlineThis is a 2×22 \times 2 matrix that can be applied to vectors in the plane.
  2. Effect on basis vectors: Understand the effect of the matrix on basis vectors. To understand the transformation, we can look at what happens to the standard basis vectors i=[1,0]i = [1, 0] and j=[0,1]j = [0, 1]. Applying the matrix to ii: (0amp;1 1amp;0)(1 0)=(0 1)\begin{pmatrix}0 & -1 \ 1 & 0\end{pmatrix} \begin{pmatrix}1 \ 0\end{pmatrix} = \begin{pmatrix}0 \ 1\end{pmatrix} The vector ii is rotated 9090 degrees counterclockwise to become jj.
  3. Apply to basis vectors: Apply the matrix to the second basis vector jj:(0amp;1 1amp;0)(0 1)=(1 0)\begin{pmatrix}0 & -1 \ 1 & 0\end{pmatrix} \begin{pmatrix}0 \ 1\end{pmatrix} = \begin{pmatrix}-1 \ 0\end{pmatrix}The vector jj is rotated 9090 degrees counterclockwise to become i-i.
  4. Conclude geometric effect: Conclude the geometric effect of the transformation. Both basis vectors are rotated 9090 degrees counterclockwise. Therefore, the matrix represents a rotation by 9090 degrees counterclockwise about the origin.

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