7. A rod of line t has a total charge of Q and a linear charge density of A, find the electric potential at point P due to the rod dq dx= The electric potential dV at P due to dq at x is: dV = k- dq Where dq = Adx and r Integrate over the charge distribution on the line: (Show your work below) bp v= [ = Adx k- %3D va' + x kQ 1+ Va? +1? - In 1 (1+ va² +1? = kAln a a

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### Problem Statement:
7. **Given:** 
   - A rod of length \( l \) has a total charge \( Q \) and a linear charge density of \( \lambda \).
   - **Objective:** Find the electric potential at point \( P \) due to the rod.

### Diagram Description:
The diagram illustrates a rod aligned along the x-axis, with a point \( P \) located on the y-axis at a distance \( a \) from the origin \( O \). The rod extends from \( O \) to length \( l \). 

### Explanation:
An infinitesimal charge element \( dq \) is considered at a distance \( x \) along the rod. The distance \( r \) from this infinitesimal element to point \( P \) is given by:

\[ r = \sqrt{a^2 + x^2} \]

### Electric Potential Calculation:
The electric potential \( dV \) at \( P \) due to \( dq \) at \( x \) is:

\[ dV = k \frac{dq}{r} \]

Where:
\[ dq = \lambda dx \quad \text{and} \quad r = \sqrt{a^2 + x^2} \]

### Integration Over the Charge Distribution:
To find the total electric potential \( V \) at point \( P \), we integrate along the length of the rod from \( x = 0 \) to \( x = l \):

\[ V = \int_0^l k \frac{dq}{r} = \int_0^l k \frac{\lambda dx}{\sqrt{a^2 + x^2}} \]

### Solution:
Combining the terms and solving the integral:

\[ 
V = k \lambda \int_0^l \frac{dx}{\sqrt{a^2 + x^2}} 
\]

This integral evaluates to:

\[ 
V = k \lambda \left. \ln \left( \frac{x + \sqrt{a^2 + x^2}}{a} \right) \right|_0^l 
\]

After applying the limits:

\[ 
V = k \lambda \left[ \ln \left( \frac{l + \sqrt{a^2 + l^2}}{a} \right) - \ln \left( \frac{0 + \sqrt{a^2
Transcribed Image Text:### Problem Statement: 7. **Given:** - A rod of length \( l \) has a total charge \( Q \) and a linear charge density of \( \lambda \). - **Objective:** Find the electric potential at point \( P \) due to the rod. ### Diagram Description: The diagram illustrates a rod aligned along the x-axis, with a point \( P \) located on the y-axis at a distance \( a \) from the origin \( O \). The rod extends from \( O \) to length \( l \). ### Explanation: An infinitesimal charge element \( dq \) is considered at a distance \( x \) along the rod. The distance \( r \) from this infinitesimal element to point \( P \) is given by: \[ r = \sqrt{a^2 + x^2} \] ### Electric Potential Calculation: The electric potential \( dV \) at \( P \) due to \( dq \) at \( x \) is: \[ dV = k \frac{dq}{r} \] Where: \[ dq = \lambda dx \quad \text{and} \quad r = \sqrt{a^2 + x^2} \] ### Integration Over the Charge Distribution: To find the total electric potential \( V \) at point \( P \), we integrate along the length of the rod from \( x = 0 \) to \( x = l \): \[ V = \int_0^l k \frac{dq}{r} = \int_0^l k \frac{\lambda dx}{\sqrt{a^2 + x^2}} \] ### Solution: Combining the terms and solving the integral: \[ V = k \lambda \int_0^l \frac{dx}{\sqrt{a^2 + x^2}} \] This integral evaluates to: \[ V = k \lambda \left. \ln \left( \frac{x + \sqrt{a^2 + x^2}}{a} \right) \right|_0^l \] After applying the limits: \[ V = k \lambda \left[ \ln \left( \frac{l + \sqrt{a^2 + l^2}}{a} \right) - \ln \left( \frac{0 + \sqrt{a^2
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