Step 1: Understanding the Concept of a Spherical Shell
According to Gauss's Law, the electric potential inside a charged conducting spherical shell is constant and equal to the potential on its surface. However, for an insulating spherical shell, the potential follows a different equation.
Step 2: Given Data
- Radius of the charged shell: \( R = 10 \) cm
- Potential on the surface: \( V_s = 100 \) V
- Distance from the center where potential is to be found: \( r = 2 \) cm
Step 3: Applying the Concept
For a conducting spherical shell, the potential inside the shell remains constant and is equal to the surface potential: \[ V_{{inside}} = V_{{surface}} \] Thus, at \( r = 2 \) cm (inside the shell), \[ V = V_{{surface}} = 100 { V} \] However, if the shell is non-conducting, then the potential at any point inside is given by: \[ V = \frac{kQ}{R} \] Since inside a conducting shell, the charge is distributed on the outer surface, the electric field inside is zero, leading to a constant potential.
Step 4: Conclusion
Since the given problem is based on a charged conducting spherical shell, the potential inside is constant. Thus, the potential at \( r = 2 \) cm from the center is: \[ V = 0 { V} \]
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