00:01
Okay, so if we look to the figure of this problem, we have the venturi meter, which is something like this.
00:07
Let's draw here.
00:13
We have the first cross -sectional area and we have another area in here.
00:24
So let's see.
00:26
Here we have the other hole, the venture in the pipe.
00:36
So it's something like this.
00:43
It's not quite good but this is divinity divinity meter okay so here we have the water so here we have water and here we have the difference in height so this distance here is what we call and call okay so here is the point two and here are the point one point two so that's our system now that we have the system well established we can answer what the problem wants and well the first item of this problem we just need to show a relation of the pressure okay so first of all, let's look to the system and we're going to say that the pressure on point one.
02:11
Since the hole is open into the air, we have atmospheric pressure plus h1, because h1 is the distance from the liquid.
02:34
To the point one so this is h1 and the pressure on point two let's put in here the pressure on point two it's going to be the atmospheric pressure plus g age 2 where age 2 is just this heighten here so this is age 2 now to answer to answer the question we have to determine what is the difference in pressure between the two points so we can say that p1 minus p2 is going to be delta p the difference in pressure and that is just we can cross the atmospheric pressure because it's equal on both ends and what is left is just that multiplies h1 minus h2.
03:53
But if we see h1 minus h2 is just equal h.
04:00
Therefore, we show in the first item that the difference in pressure between the two points is just hgh.
04:10
That's the first answer.
04:12
Now let's move on to the second item.
04:15
Okay, so in the second item, we have to use the bernoulli's and the continuity equation to show a relation that the problem wants.
04:26
So first of all, let's remember that the bernoulli's equation is just p1 plus the connecting energy of point 1, which is whole v1 square, that is equal the pressure on point 2 plus the connect the energy of point 2...