00:01
Chapter 9, probably 23, a 0 .75 kilogram sheet is centered on a closed line as shown in figure 9 -63.
00:11
The clothesline on either side of the hanging sheet makes an angle of 3 .5 degrees with the horizontal.
00:19
This is downwards, right? so this is hanging sheet.
00:24
Calculate the tension in the clothesline, ignoring its mass on either side of the sheet.
00:30
And the question is, why is the tension so much greater than the weight? of the sheet.
00:36
Essentially, why isn't the sheet, how can such a flimsy string, a small string hold up a heavy, it's not that heavy of a sheet, but a little, a weighty sheet.
00:49
It does have some decent mass to it.
00:53
It probably weighs about seven new ones.
00:57
So here we have the free body diagram of our situation, the close line.
01:02
I essentially reduced the close line to a point mass, just so we could talk about the forces.
01:09
It's feeling.
01:11
So i have the two tensions at theta degrees above the horizontal.
01:19
Yeah.
01:21
Well, there's a couple ways to think about it.
01:23
You could either have this horizontal and have it coming off there or either way.
01:38
So yes, we have two tensions, both the same degrees, and then we have the weight.
01:43
So we have to understand where the tension is coming from to understand what could what kind of factors build into the tension what makes what makes the tension the tension so our handy -dandy trick for this chapter has been to use newton's second law so we're doing so we're using that again and here we have basically just the sum of the forces in two directions x and y since it's a two dimensional problem and we see that there's only two x components right so we have one x component for t1 and we have one x component for t2 now i'm going to call, let's define our coordinate system.
02:24
Positive y is this direction and sorry it's a little slanted but imagine i made it line up with this.
02:31
Maybe that's a little bit better.
02:37
Forget about this part.
02:41
Can i get the eraser? let's not worry about it.
02:45
So yes, i have a coordinate system here and so t1 is going to have its x component in the positive x direction while t2 has the negative component.
02:57
Well t2's x component is in the negative direction, i should say.
03:00
So this just only tells us that they have the same tension in both directions, the closed line.
03:10
And so essentially the forces are canceling each other out...