00:01
So this question let's directly get to part a.
00:04
So part a, we know that at r, it's equal to capital r, uppercase r over 2, which is equal to 1 .5 centimeter.
00:14
So we know that r is less than 3r.
00:19
So we directly start by performing an integration of ets, which will be equal to the enclosed over epsilon 0.
00:31
So since the enclosed charge is zero, you can directly state this as zero.
00:39
And this is the end for the first part.
00:41
For b, we know that at r is equal to two uppercase r, which is equal to 6 cm.
00:51
So again, we perform an integration over here.
00:55
And in the image shown to us, we know that charge enclosed within the gaussian surface, is lambda l.
01:07
So writing that out, we can say that e is equal to lambda 2 pi epsilon 0 r.
01:17
And plugging in data from the problem, all the values in, we get this.
01:31
It now it is a bit large.
01:47
And from this we can state the final answer, 6 into 10 to power 3.
01:52
And do not forget the units.
01:56
Now let's move on to c.
01:58
For c we have to plot a graph of uppercase e versus a lowercase r.
02:05
For the range, 0 to 2r.
02:08
Okay.
02:09
So in this, i'll draw a rough graph as i don't have a plotting software available with me at the moment.
02:14
But you should get an idea of how to draw the graph.
02:19
Okay? so we can just draw one here.
02:23
Oh, that can come right, sorry.
02:29
And another one graphly.
02:36
Okay.
02:36
So this value here we can state it as this label the axis...