00:01
So in this situation, we have a particle far away from the sun, and we want to know the residual force that it applies to know what direction of the tail of the comet is pointing at.
00:23
So a distance away from the sun, let's call this distance r, capital r.
00:34
We have the pull of gravity, but also the sun is radiating away.
00:39
And so there is a radiation pressure, is there anything a force in this particle that we assume to be spherical? we just need to know each one of these forces and then see when they are, combine when they cancel out to know the limit between the the place where the gravity wins and the limit where the radiation pressure wins.
01:09
So first the force of the radiation is just the intensity times the cross -sectional area divided by c.
01:22
So we are assuming a spherical particle so the area cross -sectional area will be pi r square so this is the intensity is the pressure the power of the sun divided by the distance away so this intensity is power of the sun divided by four pi r square and the cross -section area is pi r square divided by c so we can just simplify a little little bit.
02:13
So this is power of the sun, radius of the sphere divided by 4r square c.
02:24
Now the force of gravity is just the newton's constant, the mass of this sum, mass of this particle divided by the distance away, this r square.
02:41
So this is, we can write the mass in terms of the density because we we are assuming that is a sphere and the volume of sphere is four thirds of pi r q so this is gm s divided by r square times four pi r q divided by three and we can write this as four pi gms gms rule so this we have a row here because we are writing the mass as density times volume.
03:26
R cube divided by 3r square.
03:36
Now we want to know what radius this happens.
03:43
So let's find out the condition where fr is equal to fg...