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Point charge q(1) = 2 mu C and q(2) = - ...

Point charge `q_(1) = 2 mu C` and `q_(2) = - 1mu C` are kept at points `x = 0` and `x = 6` respectively. Electrical potential will be zero at points

A

`x=2 and x=9`

B

`x=1 and x=5`

C

`x=4 and x=12`

D

`x=-2 and x=2`

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The correct Answer is:
To find the points where the electric potential is zero due to the two point charges \( q_1 = 2 \, \mu C \) and \( q_2 = -1 \, \mu C \), we can follow these steps: ### Step 1: Understand the Setup We have two charges: - Charge \( q_1 = 2 \, \mu C \) located at \( x = 0 \) - Charge \( q_2 = -1 \, \mu C \) located at \( x = 6 \) ### Step 2: Write the Expression for Electric Potential The electric potential \( V \) at a point \( P \) due to a point charge \( Q \) is given by the formula: \[ V = k \frac{Q}{r} \] where \( k \) is Coulomb's constant, \( Q \) is the charge, and \( r \) is the distance from the charge to the point. ### Step 3: Consider the Internal Point (Between the Charges) Let’s denote the distance from charge \( q_2 \) (located at \( x = 6 \)) to point \( P \) as \( L \). Therefore, the distance from charge \( q_1 \) to point \( P \) will be \( 6 - L \). The total potential at point \( P \) is: \[ V_P = k \frac{2 \times 10^{-6}}{6 - L} + k \frac{-1 \times 10^{-6}}{L} \] Setting \( V_P = 0 \): \[ k \frac{2 \times 10^{-6}}{6 - L} - k \frac{1 \times 10^{-6}}{L} = 0 \] We can cancel \( k \) (as it is a constant) from both sides: \[ \frac{2 \times 10^{-6}}{6 - L} = \frac{1 \times 10^{-6}}{L} \] ### Step 4: Cross Multiply and Solve for \( L \) Cross multiplying gives: \[ 2L = 6 - L \] Rearranging this: \[ 3L = 6 \implies L = 2 \] ### Step 5: Calculate the Position of Point \( P \) Since \( L = 2 \), the position of point \( P \) from the origin (where \( q_1 \) is located) is: \[ x_P = 6 - L = 6 - 2 = 4 \] ### Step 6: Consider the External Point (Outside the Charges) Now, let’s consider a point \( P \) located to the right of charge \( q_2 \). Let the distance from \( q_2 \) to point \( P \) be \( L \). The distance from \( q_1 \) to point \( P \) will then be \( 6 + L \). The total potential at point \( P \) is: \[ V_P = k \frac{2 \times 10^{-6}}{6 + L} + k \frac{-1 \times 10^{-6}}{L} \] Setting \( V_P = 0 \): \[ k \frac{2 \times 10^{-6}}{6 + L} - k \frac{1 \times 10^{-6}}{L} = 0 \] Again, canceling \( k \): \[ \frac{2 \times 10^{-6}}{6 + L} = \frac{1 \times 10^{-6}}{L} \] ### Step 7: Cross Multiply and Solve for \( L \) Cross multiplying gives: \[ 2L = 6 + L \] Rearranging this: \[ L = 6 \] ### Step 8: Calculate the Position of Point \( P \) Since \( L = 6 \), the position of point \( P \) from the origin is: \[ x_P = 6 + L = 6 + 6 = 12 \] ### Final Answer The points where the electric potential is zero are: 1. \( x = 4 \) 2. \( x = 12 \)
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DC PANDEY ENGLISH-ELECTROSTATIC POTENTIAL AND CAPACITORS-(A) Chapter exercises
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