When a magnetic dipole is placed in a magnetic field, it has a natural
tendency to minimize its potential energy by aligning itself with the field.
If there is sufficient thermal energy present, however, the dipole may rotate
so that it is no longer aligned with the field. Using \(k_{\mathrm{B}} T\) as a
measure of the thermal energy, where \(k_{\mathrm{B}}\) is Boltzmann's constant
and \(T\) is the temperature in kelvins, determine the temperature at which
there is sufficient thermal energy to rotate the magnetic dipole associated
with a hydrogen atom from an orientation parallel to an applied magnetic field
to one that is antiparallel to the applied field. Assume that the strength of
the field is \(0.15 \mathrm{~T}\)