00:01
For this problem, we have two type of arrangements for two identical bars.
00:10
They could be one top of the other as in part as this part e, or one side by the other as in part a.
00:24
Now, we know that regardless of the arrangement, the heat flows from left to right.
00:36
So, and the first question of this problem is which heat flows, what is the area, the cross -sectional area through which the heat floats is greater in part in the configuration a or in the configuration b.
00:59
So that's the first problem.
01:02
So taking into account the thing, what it says in the problem that flow, that he always flows to left to right, from that to right.
01:22
We need to know that we need to take into account these cross -sectional area.
01:32
And we can write this, we can easily see this, if we can write the other area of a should be, we are going to put numbers in these sides.
01:42
So we call this d and we call these l.
01:47
We call this l and we call this d prime.
01:53
So no, let's d prime exactly.
01:57
So for the configuration a, we have that the cross section of area is the length l times the height d for the configuration b, we have l time d prime.
02:17
But we can easily see that this d is two times and d, this d prime.
02:29
So it will be l times two times d, which is, we just take this, factorize we can easily see that the area of b is two times the area of a.
02:49
The next question of this problem asks which of the thickness is greater through which he flows in the arrangement in a or in the arrangement in b.
03:09
So this can easily easily be seen again.
03:14
We know that the thickness is this longitude in here because these are the parts through which the flow, the heat flows can go.
03:29
And this also is the thickness of this.
03:32
So from here we can see that if we call this, this must be two times c.
03:40
So if we call this, this must be two times c.
03:43
So if we call it, we call it.
03:45
The thickness of a as la, this is equal to 2 times c...