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Charges 4Q, q and Q and placed along x-a...

Charges 4Q, q and Q and placed along x-axis at positions `x=0,x=t//2` and `x=1`, respectively. Find the value of q so that force on charge Q is zero

A

Q

B

Q/2

C

`-Q//2`

D

`-Q`

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To solve the problem of finding the value of charge \( q \) such that the net force on charge \( Q \) is zero, we can follow these steps: ### Step 1: Identify the positions of the charges We have three charges: - Charge \( 4Q \) is located at \( x = 0 \) - Charge \( q \) is located at \( x = \frac{1}{2} \) - Charge \( Q \) is located at \( x = 1 \) ### Step 2: Determine the forces acting on charge \( Q \) The forces acting on charge \( Q \) are due to the other two charges: 1. The force \( F_1 \) due to charge \( 4Q \) (located at \( x = 0 \)). 2. The force \( F_2 \) due to charge \( q \) (located at \( x = \frac{1}{2} \)). ### Step 3: Calculate the force \( F_1 \) on charge \( Q \) The force \( F_1 \) exerted by charge \( 4Q \) on charge \( Q \) is given by Coulomb's law: \[ F_1 = \frac{1}{4 \pi \epsilon_0} \cdot \frac{(4Q)(Q)}{(1-0)^2} = \frac{4Q^2}{4 \pi \epsilon_0} \] This force is repulsive since both charges are positive. ### Step 4: Calculate the force \( F_2 \) on charge \( Q \) The force \( F_2 \) exerted by charge \( q \) on charge \( Q \) is also given by Coulomb's law: \[ F_2 = \frac{1}{4 \pi \epsilon_0} \cdot \frac{(q)(Q)}{(1 - \frac{1}{2})^2} = \frac{qQ}{4 \pi \epsilon_0 \cdot \left(\frac{1}{2}\right)^2} = \frac{4qQ}{4 \pi \epsilon_0} \] This force is attractive if \( q \) is negative (since \( Q \) is positive). ### Step 5: Set the net force on charge \( Q \) to zero For the net force on charge \( Q \) to be zero, we need: \[ F_1 - F_2 = 0 \] Substituting the expressions for \( F_1 \) and \( F_2 \): \[ \frac{4Q^2}{4 \pi \epsilon_0} - \frac{4qQ}{4 \pi \epsilon_0} = 0 \] This simplifies to: \[ 4Q^2 = 4qQ \] Dividing both sides by \( 4Q \) (assuming \( Q \neq 0 \)): \[ Q = q \] ### Step 6: Determine the sign of \( q \) Since the force \( F_1 \) is repulsive and \( F_2 \) must be attractive to balance it, \( q \) must be negative: \[ q = -Q \] ### Conclusion Thus, the value of charge \( q \) that makes the net force on charge \( Q \) equal to zero is: \[ q = -Q \]
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