00:01
In part a, we want to figure out what the stress is.
00:04
So recall that the young's modulus is defined as stress over strain.
00:11
So stress over strain.
00:15
And now we can determine that a 5 % elongation, which is given in the problem, 5 % elongation implies that delta l over l0 is equal to 0 .05, since delta l is the change in length and l0 is the original length.
00:35
So 5 % elongation implies that the ratio is equal to this.
00:42
And so this is just the strain.
00:45
And we know young's modulus, so we can find the stress by solving for it.
00:49
So stress is equal to young's modulus times strain.
00:54
And this is equal to the strain.
00:57
And we're given young's modulus.
00:58
So we can solve this to get 7 .4 times 10 to the 7 pascals.
01:06
And that's the answer to part a.
01:11
In part b, we want to figure out what the spring constant is if this can be modeled as a spring.
01:17
And so now we recall that the stress is also written as ft over the cross -sectional area.
01:26
We can solve this for ft since we just solved for the stress and we know a.
01:31
And we get that ft is equal to 5 .76 times 10 to the third newton's.
01:40
This will be the force that we plug in into hook's law in order to find the spring constant...