(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: \(E_{18\text{cm}} = 4.44 \times 10^{4} \, \text{N/C}\)
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
Arrange the following in the ascending order of wavelength (\( \lambda \)):
(A) Microwaves (\( \lambda_1 \))
(B) Ultraviolet rays (\( \lambda_2 \))
(C) Infrared rays (\( \lambda_3 \))
(D) X-rays (\( \lambda_4 \))
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.