00:01
Okay, we can, we're going to look at part b, so the figure, figure 88, or rather, figure 9 .88b.
00:11
And so we can say that here we're going to look, we're going to apply the absolute, the concept of the absolute pressure.
00:18
So the left tube, we can say piece of a would be equalling the atmospheric pressure plus the density of water times g multiplied by l minus h.
00:32
Now looking at the right side of the tube, we have p sub b.
00:36
This would be equalling the atmospheric pressure plus the density of oil, g .l.
00:45
And so we know that pascal's principle says p sub a equals p sub b.
00:53
And given this, we can say that h equals l multiplied by one minus the density of oil divided by the density of water.
01:06
After equating these two, we can then say that this would be equalling 5 .00 centimeters multiplied by 1 minus 750 kilograms per cubic meter.
01:20
This would be divided by 1 ,000 kilograms per cubic meter.
01:25
And h is going to give us 1 .25 centimeters.
01:31
This would be our final answer for part a.
01:34
Now for part b, we're going to consider part c of the diagram.
01:40
So here we're going to then apply bernoulli's equation to point a and point b, and we have p sub a plus one half times the density of air...