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-10mu C, 40 mu C and q are the charges ...

`-10mu C, 40 mu C` and q are the charges on three identical conductors P,Q and R respectively, Now P and Q attract each other with a force F when they are separated by a distance d. Now P and Q are made in contact with each other and then separated . Again Q and R are touched and they are separated by a distance 'd' . The repulsive force between Q and R is 4F . Then the charge q is:

A

`10 mu C`

B

`30 mu C`

C

`40 mu C`

D

`65 mu C`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we will analyze the forces acting on the charges and apply the principles of electrostatics. ### Step 1: Understand the Initial Attraction between P and Q Given: - Charge on P, \( q_P = -10 \, \mu C \) - Charge on Q, \( q_Q = 40 \, \mu C \) The force \( F \) between P and Q when they are separated by a distance \( d \) can be expressed using Coulomb's Law: \[ F = k \frac{|q_P \cdot q_Q|}{d^2} \] Substituting the values: \[ F = k \frac{|-10 \cdot 40|}{d^2} = k \frac{400}{d^2} \] ### Step 2: Contact and Separation of P and Q When P and Q are brought into contact, the total charge is shared equally because they are identical conductors. The total charge before contact is: \[ q_{total} = q_P + q_Q = -10 \, \mu C + 40 \, \mu C = 30 \, \mu C \] After contact, each conductor will have: \[ q_{P,Q} = \frac{q_{total}}{2} = \frac{30 \, \mu C}{2} = 15 \, \mu C \] So, after separation: - Charge on P, \( q_P' = 15 \, \mu C \) - Charge on Q, \( q_Q' = 15 \, \mu C \) ### Step 3: Analyze the Repulsion between Q and R Now, Q (with charge \( 15 \, \mu C \)) is brought into contact with R (with charge \( q \)). After contact, the total charge on Q and R will be: \[ q_{total, QR} = q_Q' + q = 15 \, \mu C + q \] After contact, the charge on both Q and R will be: \[ q_{Q,R} = \frac{q_{total, QR}}{2} = \frac{15 + q}{2} \] ### Step 4: Calculate the Repulsive Force between Q and R The repulsive force between Q and R when separated by distance \( d \) is given as \( 4F \): \[ 4F = k \frac{(q_{Q,R})^2}{d^2} \] Substituting \( q_{Q,R} \): \[ 4F = k \frac{\left(\frac{15 + q}{2}\right)^2}{d^2} \] From Step 1, we know: \[ F = k \frac{400}{d^2} \] Thus: \[ 4F = 4 \cdot k \frac{400}{d^2} = k \frac{1600}{d^2} \] Setting the two expressions for \( 4F \) equal gives: \[ k \frac{1600}{d^2} = k \frac{\left(\frac{15 + q}{2}\right)^2}{d^2} \] Canceling \( k \) and \( d^2 \) (since they are non-zero), we have: \[ 1600 = \left(\frac{15 + q}{2}\right)^2 \] ### Step 5: Solve for q Taking the square root of both sides: \[ 40 = \frac{15 + q}{2} \] Multiplying by 2: \[ 80 = 15 + q \] Thus: \[ q = 80 - 15 = 65 \, \mu C \] ### Final Answer The charge \( q \) is: \[ \boxed{65 \, \mu C} \]
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