00:01
One of the things that's true about a charged object held near a polarizable material is there's always a force of attraction.
00:13
And so we're going to develop a little model that explains this.
00:17
We're going to bring a point charge somewhere in the vicinity of a neutral molecule, which can be polarized.
00:28
And a reminder that polarizability relates the dipole moment of that molecule p to the external electric field in which that molecule is sitting through the polarizability alpha.
00:49
So first off, that dipole acquires a dipole moment because of the electric field.
01:00
Of the point charge.
01:09
And that dipole moment will be aligned such that the negative end of the dipole is closer to the positive point charge, just for the sake of argument.
01:23
But we'll kind of not worry too much about the actual details since we're making a general model.
01:32
But anyway, the point charge electric field is of course just the kulam relationship, q over 4 pi epsilon not, divided by the inverse squared of the separation.
01:52
So we now have an expression for the dipole moments.
02:06
Now what's going to create the attraction is the electric field of the dipole on the point charge.
02:15
So if we write down the force, on plus q, it's going to be equal to plus q times the electric field of the dipole.
02:33
And recalling a previous relationship for this electric field, we can write it down in terms of spherical coordinates or coordinate free representation, if we prefer.
02:52
But that field basically goes as the dipole moment over arc cubed, and then some vector relationships.
03:13
I started off drawing this picture with everything aligned along the z axis on purpose...