The function \( f(z) = \frac{1}{z^2 (z - 2)^3} \) has singularities at \( z = 0 \) and \( z = 2 \). We need to compute the residues of this function at both points.
Step 1: Residue at \( z = 0 \):
At \( z = 0 \), we have a pole of order 2. To find the residue, we use the formula for a second-order pole: \[ {Res}(f, 0) = \lim_{z \to 0} \frac{d}{dz} \left[ z^2 f(z) \right]. \] Now, substitute \( f(z) = \frac{1}{z^2 (z - 2)^3} \): \[ z^2 f(z) = \frac{1}{(z - 2)^3}. \] Differentiating with respect to \( z \): \[ \frac{d}{dz} \left[ \frac{1}{(z - 2)^3} \right] = -3 \cdot \frac{1}{(z - 2)^4}. \] At \( z = 0 \), this becomes: \[ {Res}(f, 0) = \frac{-3}{16}. \] Step 2: Residue at \( z = 2 \):
At \( z = 2 \), we have a pole of order 3. To compute the residue, we use the formula for the residue of a third-order pole: \[ {Res}(f, 2) = \lim_{z \to 2} \frac{1}{2!} \frac{d^2}{dz^2} \left[ (z - 2)^3 f(z) \right]. \] Substitute \( f(z) = \frac{1}{z^2 (z - 2)^3} \): \[ (z - 2)^3 f(z) = \frac{1}{z^2}. \] Differentiating twice with respect to \( z \): \[ \frac{d^2}{dz^2} \left[ \frac{1}{z^2} \right] = \frac{6}{z^4}. \] At \( z = 2 \), this becomes: \[ {Res}(f, 2) = \frac{6}{16} = \frac{3}{16}. \] Thus, the residues are \( {Res}(f, 0) = -\frac{3}{16} \) and \( {Res}(f, 2) = \frac{3}{16} \).
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: