Two infinite line charges are parallel to the z-axis and pass through the x-axis at x= ±d as shown. Find the energy required to move a negative point charge -q from the origin (midway between the two line charges) to a point h along the y-axis. Recall that the field and potential of a single uniform line charge are given by E(r)=f_Pro 2πεor Φ(r)=- where r is the distance from the line charge normal to its axis. ριο 2περ - Inr

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**Problem Description:**

Two infinite line charges are parallel to the z-axis and pass through the x-axis at \( x = \pm d \) as shown. Find the energy required to move a negative point charge \(-q\) from the origin (midway between the two line charges) to a point \( h \) along the y-axis. Recall that the field and potential of a single uniform line charge are given by:

\[
\vec{E}(r) = \hat{r} \frac{\rho_{\ell 0}}{2\pi \varepsilon_0 r}
\]

\[
\Phi(r) = -\frac{\rho_{\ell 0}}{2\pi \varepsilon_0} \ln r
\]

where \( r \) is the distance from the line charge normal to its axis.

**Diagram Explanation:**

The diagram on the right shows two infinite line charges running parallel to the z-axis. These lines are denoted with charge density \(\rho_{\ell 0}\). They are positioned symmetrically at \( x = d \) and \( x = -d \) on the x-axis. The negative point charge \(-q\) is located at the origin, at equal distance from both line charges, and needs to be moved to a point \( h \) along the positive y-axis.

The electrostatic field and potential equations provided are essential for calculating the energy required to move the charge \(-q\) from its initial to final position.
Transcribed Image Text:**Problem Description:** Two infinite line charges are parallel to the z-axis and pass through the x-axis at \( x = \pm d \) as shown. Find the energy required to move a negative point charge \(-q\) from the origin (midway between the two line charges) to a point \( h \) along the y-axis. Recall that the field and potential of a single uniform line charge are given by: \[ \vec{E}(r) = \hat{r} \frac{\rho_{\ell 0}}{2\pi \varepsilon_0 r} \] \[ \Phi(r) = -\frac{\rho_{\ell 0}}{2\pi \varepsilon_0} \ln r \] where \( r \) is the distance from the line charge normal to its axis. **Diagram Explanation:** The diagram on the right shows two infinite line charges running parallel to the z-axis. These lines are denoted with charge density \(\rho_{\ell 0}\). They are positioned symmetrically at \( x = d \) and \( x = -d \) on the x-axis. The negative point charge \(-q\) is located at the origin, at equal distance from both line charges, and needs to be moved to a point \( h \) along the positive y-axis. The electrostatic field and potential equations provided are essential for calculating the energy required to move the charge \(-q\) from its initial to final position.
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