(a) Radius of the spherical conductor, r = 12 cm = 0.12 m Charge is uniformly distributed over the conductor, q = 1.6 × 10−7 C Electric field inside a spherical conductor is zero. This is because if there is field inside the conductor, then charges will move to neutralize it.
(b) Electric field E just outside the conductor is given by the relation,
\(E = \frac{1}{4πεº} . \frac{q}{r^2}\)
Where, εo = Permittivity of free space and \(\frac{1}{4πε_o}\) = 9 × 109 Nm2 C-2
Therefore, \(E = \frac{9×10^9×1.6×10-7}{( 0.12)^2} =10^5NC^{-1}\)
Therefore, the electric field just outside the sphere is 105 NC-1.
(c) Electric field at a point 18 m from the centre of the sphere = E1
Distance of the point from the centre, d = 18 cm = 0.18 m
\(E_1 = \frac{1}{4πε_o}.\frac{q}{d_2} = \frac{9×109×1.6×10-7}{(1.8×10-2)2}=4.4×10^4 NC^{-1}\)
Therefore, the electric field at a point 18 cm from the centre of the sphere is 4.4 × 104 NC-1 .
(a) Electric Field Inside the Sphere
For a conductor in electrostatic equilibrium, the electric field inside the conductor is zero because the charges reside on the surface, and the field inside cancels out.
\(E_{\text{inside}} = 0 \, \text{N/C}\)
(b) Electric Field Just Outside the Sphere
To find the electric field just outside the surface of the sphere, we use Gauss's law. Consider a Gaussian surface just outside the sphere with radius \(R = 12 \, \text{cm} = 0.12 \, \text{m}\). The charge enclosed by this surface is \(Q = 1.6 \times 10^{-7} \, \text{C}\).
Gauss's law states:
\(\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\epsilon_0}\)
For a spherical surface, the electric field E is uniform and radial, so:
\(E \cdot 4 \pi R^2 = \frac{Q}{\epsilon_0}\)
Solving for E:
\(E = \frac{Q}{4 \pi \epsilon_0 R^2}\)
Plugging in the values:
\(E = \frac{1.6 \times 10^{-7}}{4 \pi (8.85 \times 10^{-12}) (0.12)^2}\)
Let's calculate this:
\(E = \frac{1.6 \times 10^{-7}}{4 \pi \times 8.85 \times 10^{-12} \times 0.0144}\)
\(E = \frac{1.6 \times 10^{-7}}{1.601 \times 10^{-12}}\)
\(E =1.00 \times 10^{5} \, \text{N/C}\)
So the electric field just outside the sphere is:
\(E_{\text{outside}} = 10^{5} \, \text{N/C}\)
(c) Electric Field at a Point 18 cm from the Centre of the Sphere
For a point outside the sphere at a distance \(r = 18 \, \text{cm} = 0.18 \, \text{m}\) from the center, the charge enclosed is still \(Q = 1.6 \times 10^{-7} \, \text{C}\)We can treat the sphere as if all its charge were concentrated at its center.
The electric field at distance r is given by:
\(E = \frac{Q}{4 \pi \epsilon_0 r^2}\)
Plugging in the values:
\(E = \frac{1.6 \times 10^{-7}}{4 \pi (8.85 \times 10^{-12}) (0.18)^2}\)
Let's calculate this:
\(E = \frac{1.6 \times 10^{-7}}{4 \pi \times 8.85 \times 10^{-12} \times 0.0324}\)
\(E = \frac{1.6 \times 10^{-7}}{3.601 \times 10^{-12}}\)
\(E = 4.44 \times 10^{4} \, \text{N/C}\)
So the electric field at a point 18 cm from the center of the sphere is: \(E_{18\text{cm}} = 4.44 \times 10^{4} \, \text{N/C}\)
Find work done in bringing charge q = 3nC from infinity to point A as shown in the figure : 
Two capacitors \( C_1 \) and \( C_2 \) are connected in parallel to a battery. Charge-time graph is shown below for the two capacitors. The energy stored with them are \( U_1 \) and \( U_2 \), respectively. Which of the given statements is true? 
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Choke coil is simply a coil having a large inductance but a small resistance. Choke coils are used with fluorescent mercury-tube fittings. If household electric power is directly connected to a mercury tube, the tube will be damaged.
Reason (R): By using the choke coil, the voltage across the tube is reduced by a factor \( \frac{R}{\sqrt{R^2 + \omega^2 L^2}} \), where \( \omega \) is the frequency of the supply across resistor \( R \) and inductor \( L \). If the choke coil were not used, the voltage across the resistor would be the same as the applied voltage.
In light of the above statements, choose the most appropriate answer from the options given below:

The electrostatic potential is also known as the electric field potential, electric potential, or potential drop is defined as “The amount of work that is done in order to move a unit charge from a reference point to a specific point inside the field without producing an acceleration.”
SI unit of electrostatic potential - volt
Other units - statvolt
Symbol of electrostatic potential - V or φ
Dimensional formula - ML2T3I-1
The electric potential energy of the system is given by the following formula:
U = 1/(4πεº) × [q1q2/d]
Where q1 and q2 are the two charges that are separated by the distance d.