00:01
So torque acting on a dipole in presence of an electric field is given by magnitude of the dipole times magnitude of the electric field times sine of the angle between them.
00:19
Now if the net torque is zero, this means that theta has to be either zero degree or 180 degree.
00:33
And this is for the case when you have a dipole and hence the electric field and the magnetic dipole, sorry, the electric field and the electric dipole moment are not zeros.
00:46
So for that case, only possibility that for the torque to be zero is when the value of theta is either zero degree or 180 degree, which means that the dipole moment should either be parallel, or anti -parallel to the electric field.
01:07
So let's draw the orientations of the dipole in a uniform electric field.
01:14
So let's say the electric field is along towards the right or towards the positive x -axis if this is your x -axis.
01:28
Now the condition that we got is the dipole should has to be either parallel or parallel to the electric field in order to in order for the net torque to be zero.
01:42
So if the dipole is parallel to the electric field, then we should have the negative charge to be on the left and positive charge on the right, since dipole always points towards the positive charge.
02:02
Now the other possibility is for the dipole to be anti -parallel to the electric fields.
02:07
For that the direction of the dipole or the dipole moment should be like so and for this case we should have the negative charge on the right and positive charge on the left so these are the two orientations for the dipole so that the torque on the dipole is zero now in the second part we have to find which orientation of the dipole is stable now the this is really simple.
02:41
The stable orientation is when the dipole is parallel to the electric field.
02:48
So theta should be equal to zero for stability.
02:53
And unstable orientation is the one where both of them are anti -parallel...