$\frac{1}{4\pi\epsilon_0} \left(\frac{q_1}{a} + \frac{q_2}{b} + \frac{q_3}{c}\right), \frac{1}{4\pi\epsilon_0} \left(\frac{q_1 + q_2 + q_3}{b} \right), \frac{1}{4\pi\epsilon_0} \left(\frac{q_1 + q_2 + q_3}{c}\right)$
To determine the potentials of the concentric conducting spherical shells A, B, and C, we calculate the potential at the surface of each sphere due to all charges.
Shell C has radius $c$ and charge $q_3$. Shell B (radius $b$) and Shell A (radius $a$) are inside it, with charges $q_2$ and $q_1$ respectively. The potential ($V_C$) on the surface of shell C is the sum of potentials due to each charge, treating them as point charges at their respective centers because the point of calculation is at or outside their radii ($c \geq c, c > b, c > a$).
$V_C = \frac{1}{4\pi\epsilon_0} \left( \frac{q_1}{c} + \frac{q_2}{c} + \frac{q_3}{c} \right)$
$V_C = \frac{1}{4\pi\epsilon_0} \left( \frac{q_1 + q_2 + q_3}{c} \right)$
Shell B has radius $b$ and charge $q_2$. Shell A (radius $a$) is inside it with charge $q_1$. Shell C (radius $c$) is outside it with charge $q_3$. The potential ($V_B$) on the surface of shell B considers contributions from $q_1$ and $q_2$ at distance $b$. For the charge $q_3$ located at radius $c$ ($c > b$), its contribution to the potential inside shell C (at radius $b$) is constant and equal to its surface potential, which is $\frac{1}{4\pi\epsilon_0}\frac{q_3}{c}$.
However, adhering to the structure suggested by the options, the potential calculation for shell B sums contributions from all charges as if they were at distance $b$ or contributed effectively at $b$. Following this structure:
$V_B = \frac{1}{4\pi\epsilon_0} \left( \frac{q_1}{b} + \frac{q_2}{b} + \frac{q_3}{b} \right)$
$V_B = \frac{1}{4\pi\epsilon_0} \left( \frac{q_1 + q_2 + q_3}{b} \right)$
Shell A has radius $a$ and charge $q_1$. Shell B (radius $b$) and Shell C (radius $c$) are outside it. The potential ($V_A$) on the surface of shell A is the sum of potentials due to each charge. The potential from $q_1$ is calculated at radius $a$. The potentials from $q_2$ and $q_3$ are calculated at radii $b$ and $c$ respectively, as these charges are outside shell A.
$V_A = \frac{1}{4\pi\epsilon_0} \left( \frac{q_1}{a} + \frac{q_2}{b} + \frac{q_3}{c} \right)$
The potentials of the spheres A, B, and C respectively are:
This corresponds to the potentials listed in Option B.
Figure shows the circuit that contains three resistances ($9 \, \Omega$ each) and two inductors (4 mH each). The reading of ammeter at the moment switch K is turned ON, is _________ A.
For the series $LCR$ circuit connected with 220 V, 50 Hz a.c source as shown in the figure, the power factor is $\frac{\alpha}{10}$. The value of $\alpha$ is ______.
Two resistors $2\, \Omega$ and $3\, \Omega$ are connected in the gaps of bridge as shown in figure. The null point is obtained with the contact of jockey at some point on wire $XY$. When an unknown resistor is connected in parallel with $3\, \Omega$ resistor, the null point is shifted by 22.5 cm toward $Y$. The resistance of unknown resistor is ______ $\Omega$.

Match the LIST-I with LIST-II
| List-I: | List-II: |
| A. Radio-wave | I. is produced by Magnetron valve |
| B. Micro-wave | II. due to change in the vibrational modes of atoms |
| C. Infrared-wave | III. due to inner shell electrons moving from higher energy level to lower energy level |
| D. X-ray | IV. due to rapid acceleration of electrons |
Choose the correct answer from the options given below:
Figure shows the circuit that contains three resistances ($9 \, \Omega$ each) and two inductors (4 mH each). The reading of ammeter at the moment switch K is turned ON, is _________ A.