Related Formula
For a uniformly charged spherical shell of radius R$R$ and charge Q$Q$:
- Inside and on the surface of the shell (r ≤ R$r \le R$):
Vᵢₙ = Vsurface = (kQ)/(R)$$V_{\text{in}} = V_{\text{surface}} = \frac{kQ}{R}$$
- Outside the shell (r > R$r > R$):
Vout = (kQ)/(r) = Vsurface ((R)/(r))$$V_{\text{out}} = \frac{kQ}{r} = V_{\text{surface}} \left(\frac{R}{r}\right)$$
Core Logic
Let's calculate the potentials at the specified positions:
- Given surface potential at R = 10~cm$R = 10\mathrm{~cm}$ is 120~V$120\mathrm{~V}$.
- At the center (r = 0$r = 0$):
Since the center lies inside the shell (0 < 10~cm$0 < 10\mathrm{~cm}$), the potential equals the surface potential:
Vcentre = 120~V$$V_{\text{centre}} = 120\mathrm{~V}$$
- At r = 5~cm$r = 5\mathrm{~cm}$:
Since 5~cm$5\mathrm{~cm}$ is also inside the shell (5 < 10~cm$5 < 10\mathrm{~cm}$), the potential remains constant at the surface value:
Vr=5 = 120~V$$V_{r=5} = 120\mathrm{~V}$$
- At r = 15~cm$r = 15\mathrm{~cm}$:
Since 15~cm$15\mathrm{~cm}$ is outside the shell (15 > 10~cm$15 > 10\mathrm{~cm}$), the potential decreases inversely with distance:
Vr=15 = Vsurface ((R)/(r)) = 120 × (10)/(15) = 80~V$$V_{r=15} = V_{\text{surface}} \left(\frac{R}{r}\right) = 120 \times \frac{10}{15} = 80\mathrm{~V}$$
Therefore, the potentials are 120~V$120\mathrm{~V}$, 120~V$120\mathrm{~V}$, and 80~V$80\mathrm{~V}$ respectively.
Pattern Recognition
The electric field inside a uniformly charged conducting spherical shell is zero, meaning that no work is done moving a charge inside it. Consequently, the potential remains absolutely uniform/constant from the surface all the way to the center!
Chapter Mix
Class 12 Physics: Electrostatic Potential and Capacitance