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A conducting sphere of radius R and carr...

A conducting sphere of radius `R` and carrying a charge `Q` is joined to an uncharged conducting sphere of radius `2R`. The charge flowing between them will be

A

`(1)/(4piepsilon_(0)).(Q^(2))/(4R)`

B

`(1)/(4pi epsilon_(0)).(Q^(2))/(2R)`

C

`(1)/(4pi epsilon_(0)).(Q^(2))/(R)`

D

`(2)/(2pi epsilon_(0)).(Q^(2))/(3R)`

Text Solution

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The correct Answer is:
To solve the problem of charge flow between two conducting spheres, we will follow these steps: ### Step 1: Understand the Problem We have two conducting spheres: - Sphere 1 (radius = R, charge = Q) - Sphere 2 (radius = 2R, charge = 0) When these two spheres are connected, charge will flow until both spheres reach the same electric potential. ### Step 2: Write the Expression for Electric Potential The electric potential \( V \) of a conducting sphere is given by: \[ V = \frac{Q}{4\pi \epsilon_0 R} \] where \( Q \) is the charge on the sphere and \( R \) is its radius. For Sphere 1 (with charge \( Q_1 \)): \[ V_1 = \frac{Q_1}{4\pi \epsilon_0 R} \] For Sphere 2 (with charge \( Q_2 \)): \[ V_2 = \frac{Q_2}{4\pi \epsilon_0 (2R)} = \frac{Q_2}{8\pi \epsilon_0 R} \] ### Step 3: Set the Potentials Equal Since the spheres will reach the same potential when connected, we set \( V_1 = V_2 \): \[ \frac{Q_1}{4\pi \epsilon_0 R} = \frac{Q_2}{8\pi \epsilon_0 R} \] ### Step 4: Simplify the Equation We can cancel \( 4\pi \epsilon_0 R \) from both sides: \[ Q_1 = \frac{Q_2}{2} \] ### Step 5: Use Charge Conservation The total charge before connecting the spheres is \( Q \) (from Sphere 1) and \( 0 \) (from Sphere 2). Thus, we have: \[ Q_1 + Q_2 = Q \] ### Step 6: Substitute \( Q_1 \) in Terms of \( Q_2 \) From the equation \( Q_1 = \frac{Q_2}{2} \), we substitute into the charge conservation equation: \[ \frac{Q_2}{2} + Q_2 = Q \] \[ \frac{3Q_2}{2} = Q \] ### Step 7: Solve for \( Q_2 \) Multiplying both sides by \( \frac{2}{3} \): \[ Q_2 = \frac{2Q}{3} \] ### Step 8: Find \( Q_1 \) Now substitute \( Q_2 \) back to find \( Q_1 \): \[ Q_1 = \frac{Q_2}{2} = \frac{1}{2} \cdot \frac{2Q}{3} = \frac{Q}{3} \] ### Step 9: Calculate Charge Flow The charge that flows from Sphere 1 to Sphere 2 is: \[ \text{Charge Flow} = Q - Q_1 = Q - \frac{Q}{3} = \frac{2Q}{3} \] ### Final Answer The charge flowing between the two spheres is: \[ \frac{2Q}{3} \]

To solve the problem of charge flow between two conducting spheres, we will follow these steps: ### Step 1: Understand the Problem We have two conducting spheres: - Sphere 1 (radius = R, charge = Q) - Sphere 2 (radius = 2R, charge = 0) When these two spheres are connected, charge will flow until both spheres reach the same electric potential. ...
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