In this section, we examine the dynamics of a permanent dipole moment p placed in a uniform external electric field E. Although the net force on the dipole is zero in a uniform field since E is constant, the charges experience equal and opposite forces leading to a torque that tends to align the dipole with the field. The torque
\[ \tau = p \times E \]
is pivotal as it helps the dipole rotate until it is aligned with E, thus minimizing its potential energy in the field. In cases where the electric field is not uniform, the net force on the dipole is non-zero and directed towards regions of stronger field intensity. The section ties in real-life applications, such as how charged objects influence uncharged materials by inducing dipole moments, thus explaining observable phenomena in electrostatic interactions.