Step 1: The integral involves a rational function in \( z \) and is taken over a unit circle. To solve it, we can use the residue theorem to compute the integral by identifying the poles inside the unit circle.
Step 2: The poles of the integrand occur where the denominators are zero. These are the points where \( z^4 - 1 = 0 \), and where \( z - \frac{a}{b} = 0 \) and \( z - \frac{b}{a} = 0 \).
Step 3: After identifying the poles and applying the residue theorem, we find that the correct values for \( I \) are \( \frac{5}{8} \) when \( a = 1, b = 2 \) and when \( a = 2, b = 1 \), and the corresponding answer options are (A) and (C).
Evaluate $\displaystyle \oint_C \frac{dz}{z^2(z-4)}$ where $C$ is the rectangle with vertices $(-1-j), (3-j), (3+j), (-1+j)$ traversed counter-clockwise.
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is:
In the transistor circuit shown in the figure, \( V_{BE} = 0.7 \, {V} \) and \( \beta_{DC} = 400 \). The value of the base current in \( \mu A \) (rounded off to one decimal place) is: