Given the dipole moment $ p $ and the electric field $ E $, find the work done to move the dipole from a parallel orientation to an antiparallel orientation with respect to the electric field.
Show Hint
The work done is negative because the system loses potential energy as the dipole moves from a lower-energy state (parallel) to a higher-energy state (antiparallel).
Step 1: Recall the formula for work done on a dipole
The work done (\( W \)) in rotating a dipole from one orientation to another in an electric field is given by:
\[
W = -\Delta U = - (U_{\text{final}} - U_{\text{initial}})
\]
where the potential energy of a dipole in an electric field is:
\[
U = -\vec{p} \cdot \vec{E} = - p E \cos \theta
\]
Here:
\(\vec{p}\) is the dipole moment,
\(\vec{E}\) is the electric field,
\(\theta\) is the angle between \(\vec{p}\) and \(\vec{E}\). Step 2: Analyze the orientations
1. Initial orientation: Parallel to the electric field (\(\theta_i = 0^\circ\)).
Potential energy:
\[
U_{\text{initial}} = - p E \cos(0^\circ) = - p E \times 1 = - p E
\]
2. Final orientation: Antiparallel to the electric field (\(\theta_f = 180^\circ\)).
Potential energy:
\[
U_{\text{final}} = - p E \cos(180^\circ) = - p E \times (-1) = + p E
\]
Step 3: Calculate the change in potential energy
\[
\Delta U = U_{\text{final}} - U_{\text{initial}} = (+ p E) - (- p E) = p E + p E = 2 p E
\]
Step 4: Work done
The work done (\(W\)) is:
\[
W = - \Delta U = - (2 p E) = - 2 p E
\]
Step 5: Conclusion
The work done to move the dipole from parallel to antiparallel to the electric field is:
\[
{(D) -2 p E}
\]