An electric dipole placed in a uniform electric field will experience torque, and work is done on it when it is rotated. The work done \( W \) in rotating a dipole by an angle \( \theta \) in a uniform electric field can be calculated using the formula:
\[ W = pE(\cos \theta_1 - \cos \theta_2) \]
Where:
- p is the dipole moment (6.0 × 10-6 Cm)
- E is the electric field strength (1.5 × 103 N/C)
- \(\theta_1\) and \(\theta_2\) are the initial and final angles, respectively.
Initially, the dipole moment is aligned with the field, so \(\theta_1 = 0^\circ\), thus \(\cos \theta_1 = \cos 0^\circ = 1\). After rotation by 180°, \(\theta_2 = 180^\circ\) and \(\cos \theta_2 = \cos 180^\circ = -1\). Substitute these values into the equation:
\[ W = (6.0 \times 10^{-6} \text{ Cm})(1.5 \times 10^3 \text{ N/C})(1 - (-1)) \]
Calculate the expression inside the parenthesis:
\[ 1 - (-1) = 2 \]
Now calculate the work done:
\[ W = (6.0 \times 10^{-6} \text{ Cm})(1.5 \times 10^3 \text{ N/C})(2) = 18 \times 10^{-3} \text{ J} = 18 \text{ mJ} \]
The calculated work done is 18 mJ, which falls within the expected range of 18,18 mJ. Thus, the solution is confirmed to be correct.