00:01
We have a wire with a radius of 3 .4 millimeters, and the current density in both cases features this constant, which is 5 .5 times 10 to the 4th amper per square meter.
00:12
And so we want to evaluate the total current in this wire in the case where we have this current density and then this current density.
00:20
And so the total current, i'll write this on the bottom.
00:23
Of course, there's just going to be the integral of j of r, d ,a.
00:28
And since there is no angular dependence in the current density here, we can do the angular integral, the d -theta integral, and this will just be the integral from zero to r of j of r times r, dr, so let's do that integral for both cases.
00:44
So here we can fact out the constant j -0 in front of the integral, so we have 2 pi times j -not, times the integral from 0 to r of little r over big r times r, d -r, so we can write this as a, like r squared d r and so that integral is a one -third r cubed one -third little r cubed and when we evaluate it and everything um and plug in the answers we'll get something like two pi over three times j -not times r squared um and so with the numbers we're given this is about 1 .33 amps next up similar thing going on here we can factor out this constants once again and we have the integral from zero to capital r of one minus little r over big r times r d r and so the first term in the integral is going to produce a one -half r squared the second term in the integral is going to produce you know a negative one -third r cubed neglecting the constants and so we'll have like two pi times j -not times one -half capital r squared minus one -third third capital r squared so 1 half minus the third is a sixth.
02:00
So this is just a sixth of the previous, or sorry, it's half of the previous current density, basically...