Answer:
showm
Explanation:
Consider a dipole having magnetic moment 'm' is placed in magnetic field [tex]\vec{B}[/tex] then the torque exerted by the field on the dipole is
[tex]\tau = m\times B[/tex]
[tex]\tau=mBsin\alpha[/tex]
Now to rotate the dipole in the field to its final position the work required to be done is
[tex]U=\int \tau d\alpha[/tex]
[tex]U=\int mBsin\alpha d\alpha[/tex]
[tex]U= -mBcos\alpha[/tex]
[tex]U=-\vec{m\times \vec{B}}[/tex]
Minimum energy mB is for the case when m is anti parallel to B.
Minimum energy -mB is for the case when m is parallel to B.