A conducting sphere of radius R is charged to a potential of V volt. Then the electric field at a distance \(r(>R)\) from the centre of sphere would be :
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Outside a charged sphere, it behaves like a point charge at centre.
Step 1: Understanding the Concept:
A conducting sphere acts as a point charge concentrated at its center for all points outside the sphere. We can relate the surface potential \( V \) to the total charge \( Q \). : Key Formula or Approach:
1. Potential on surface: \( V = \frac{1}{4\pi\epsilon_0} \frac{Q}{R} \).
2. Electric field outside (\( r>R \)): \( E = \frac{1}{4\pi\epsilon_0} \frac{Q}{r^2} \). Step 2: Detailed Explanation:
From the expression for potential \( V \):
\[ \frac{Q}{4\pi\epsilon_0} = V \cdot R \]
Now, substitute this into the expression for electric field \( E \) at distance \( r \):
\[ E = \left( \frac{Q}{4\pi\epsilon_0} \right) \cdot \frac{1}{r^2} \]
\[ E = (V \cdot R) \cdot \frac{1}{r^2} \]
\[ E = \frac{RV}{r^2} \] Step 3: Final Answer:
The electric field at distance \( r \) is \( RV/r^2 \).
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