Step 1: Identify the given vectors. \\ From the figure, \[ \mathbf{u} = \begin{bmatrix} 4 \\ 3 \end{bmatrix}, \mathbf{v} = \begin{bmatrix} 5 \\ 0 \end{bmatrix}. \] We want a transformation matrix $A$ such that $A \mathbf{u} = \mathbf{v}$.
Step 2: Interpret geometrically. \\ Vector $\mathbf{u} = (4,3)$ has magnitude: \[ |\mathbf{u}| = \sqrt{4^2 + 3^2} = \sqrt{16+9} = \sqrt{25} = 5. \] Vector $\mathbf{v} = (5,0)$ also has magnitude $5$. Thus, $A$ must be a rotation matrix that maps $(4,3)$ onto $(5,0)$.
Step 3: Find the rotation angle. \\ Direction of $\mathbf{u}$: \[ \theta_{u} = \tan^{-1}\!\left(\frac{3}{4}\right) \approx 36.87^\circ. \] Direction of $\mathbf{v}$: \[ \theta_{v} = 0^\circ. \] Therefore, the required rotation is clockwise by $36.87^\circ$.
Step 4: General form of 2D rotation matrix. \\ For a clockwise rotation by angle $\theta$, the rotation matrix is: \[ R(\theta) = \begin{bmatrix} \cos \theta & \sin \theta \\ [6pt] -\sin \theta & \cos \theta \end{bmatrix}. \] Here $\cos \theta = \tfrac{4}{5}$ and $\sin \theta = \tfrac{3}{5}$. So, \[ R = \begin{bmatrix} \tfrac{4}{5} & \tfrac{3}{5} \\ [6pt] -\tfrac{3}{5} & \tfrac{4}{5} \end{bmatrix}. \] But this corresponds to anticlockwise rotation. For clockwise, the correct form is: \[ R = \begin{bmatrix} \tfrac{4}{5} & -\tfrac{3}{5} \\ [6pt] \tfrac{3}{5} & \tfrac{4}{5} \end{bmatrix}. \]
Step 5: Verification. \\ \[ A \mathbf{u} = \begin{bmatrix} \tfrac{4}{5} & -\tfrac{3}{5} \\ [6pt] \tfrac{3}{5} & \tfrac{4}{5} \end{bmatrix} \begin{bmatrix} 4 \\ 3 \end{bmatrix} = \begin{bmatrix} \tfrac{16}{5} - \tfrac{9}{5} \\ [6pt] \tfrac{12}{5} + \tfrac{12}{5} \end{bmatrix} = \begin{bmatrix} \tfrac{7}{5} \\ \tfrac{24}{5} \end{bmatrix}. \] Oops—this does not yield $(5,0)$. Let us carefully check again. Actually, the clockwise rotation matrix is: \[ R(\theta) = \begin{bmatrix} \cos \theta & \sin \theta \\ [6pt] -\sin \theta & \cos \theta \end{bmatrix}. \] Substituting $\cos \theta = 4/5$, $\sin \theta = 3/5$: \[ R = \begin{bmatrix} 4/5 & 3/5 \\ [6pt] -3/5 & 4/5 \end{bmatrix}. \] Now, \[ R \begin{bmatrix} 4 \\ 3 \end{bmatrix} = \begin{bmatrix} \tfrac{16}{5} + \tfrac{9}{5} \\ [6pt] -\tfrac{12}{5} + \tfrac{12}{5} \end{bmatrix} = \begin{bmatrix} 25/5 \\ 0 \end{bmatrix} = \begin{bmatrix} 5 \\ 0 \end{bmatrix}. \] This matches perfectly!
Step 6: Match with options. \\ The correct option is: \[ \begin{bmatrix} \tfrac{4}{5} & \tfrac{3}{5} \\ [6pt] -\tfrac{3}{5} & \tfrac{4}{5} \end{bmatrix}. \] This is option (A). % Final Answer \[ \boxed{\text{Option (A)}} \]
A continuous time periodic signal \( x(t) \) is given by: \[ x(t) = 1 + 2\cos(2\pi t) + 2\cos(4\pi t) + 2\cos(6\pi t) \] If \( T \) is the period of \( x(t) \), then evaluate: \[ \frac{1}{T} \int_0^T |x(t)|^2 \, dt \quad {(round off to the nearest integer).} \]
The maximum percentage error in the equivalent resistance of two parallel connected resistors of 100 \( \Omega \) and 900 \( \Omega \), with each having a maximum 5% error, is: \[ {(round off to nearest integer value).} \]
Consider a distribution feeder, with \( R/X \) ratio of 5. At the receiving end, a 350 kVA load is connected. The maximum voltage drop will occur from the sending end to the receiving end, when the power factor of the load is: \[ {(round off to three decimal places).} \]
In the circuit with ideal devices, the power MOSFET is operated with a duty cycle of 0.4 in a switching cycle with \( I = 10 \, {A} \) and \( V = 15 \, {V} \). The power delivered by the current source, in W, is: \[ {(round off to the nearest integer).} \] 
The induced emf in a 3.3 kV, 4-pole, 3-phase star-connected synchronous motor is considered to be equal and in phase with the terminal voltage under no-load condition. On application of a mechanical load, the induced emf phasor is deflected by an angle of \( 2^\circ \) mechanical with respect to the terminal voltage phasor. If the synchronous reactance is \( 2 \, \Omega \), and stator resistance is negligible, then the motor armature current magnitude, in amperes, during loaded condition is closest to: \[ {(round off to two decimal places).} \]