00:01
Question, we have a register consisting of a solid cylinder of radius small r and length capital l and the register has resistance capital r and it is carrying current i, okay, using pointing vector to calculate the power radiated out of the surface of the register.
00:15
So we have to calculate here the power using pointing vector, okay? so pointing vector as it is defined as eb divided by mu not and power it is given by pointing vector multiplied by area, okay? so this is the value for the power.
00:31
This is pointing vector s and this is the area of the cylinder.
00:34
Okay.
00:35
So now area of the cylinder, this will be equals to 2 pi r l.
00:40
And electric field in the term of potential.
00:42
So we can write that v by l will be equals to electric field e.
00:46
And magnetic field at distance small r due to current carrying i in the wire.
00:53
So it will be given by b equals to mu not i divided by 2 pi multiplied by r.
00:59
So, now we can substitute all these value area, electric field and magnetic field in this equation and also s in this equation...