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A charge Q is placed at each corner of a...

A charge Q is placed at each corner of a cube of side a. The potential at the centre of the cube is

A

`(8Q)/(piin_(a)a)`

B

`(4Q)/(4piin_(0)a)`

C

`(4Q)/(sqrt(3)piin_(0)a)`

D

`(4Q)/(piin_(a)a)`

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The correct Answer is:
To find the potential at the center of a cube with charge \( Q \) placed at each corner, we can follow these steps: ### Step 1: Understand the Geometry of the Cube The cube has a side length \( a \). Each corner of the cube has a charge \( Q \). The center of the cube is equidistant from all corners. ### Step 2: Calculate the Distance from a Corner to the Center The distance \( R \) from a corner of the cube to the center can be found using the body diagonal of the cube. The length of the body diagonal \( d \) of a cube with side \( a \) is given by: \[ d = \sqrt{a^2 + a^2 + a^2} = \sqrt{3a^2} = a\sqrt{3} \] Since the center is at half the length of the body diagonal, the distance \( R \) is: \[ R = \frac{d}{2} = \frac{a\sqrt{3}}{2} \] ### Step 3: Use the Formula for Electric Potential The electric potential \( V \) due to a point charge \( Q \) at a distance \( R \) is given by: \[ V = k \frac{Q}{R} \] where \( k = \frac{1}{4\pi \epsilon_0} \). ### Step 4: Calculate the Total Potential at the Center Since there are 8 charges at the corners of the cube, the total potential \( V_{\text{net}} \) at the center is the sum of the potentials due to each charge: \[ V_{\text{net}} = 8 \times k \frac{Q}{R} \] ### Step 5: Substitute the Expression for R Substituting \( R = \frac{a\sqrt{3}}{2} \) into the equation gives: \[ V_{\text{net}} = 8 \times k \frac{Q}{\frac{a\sqrt{3}}{2}} = 8 \times k \frac{2Q}{a\sqrt{3}} = \frac{16kQ}{a\sqrt{3}} \] ### Step 6: Substitute the Value of k Now substituting \( k = \frac{1}{4\pi \epsilon_0} \): \[ V_{\text{net}} = \frac{16 \cdot \frac{1}{4\pi \epsilon_0} Q}{a\sqrt{3}} = \frac{4Q}{\pi \epsilon_0 a\sqrt{3}} \] ### Final Answer Thus, the potential at the center of the cube is: \[ V_{\text{net}} = \frac{4Q}{\pi \epsilon_0 a\sqrt{3}} \]
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