00:02
Okay, in this problem, we're given a tank and there's a small hole punched in the bottom of the tank.
00:09
We want to know how fast seawater is going to be flowing out of that hole.
00:14
So the principle that we want to use to tackle this problem is, or i should say the equation that we want to use to tackle, this is bernoulli's equation, which i've written here.
00:24
And we're going to let the subscript 1 to denote values at the surface of the seawater in the tank.
00:31
And the subscript 2 to denote values at the hole.
00:38
So because we were told that the hole is small, we can neglect the motion of water at the surface, the height of the height of the water of the tank is not going to be changing by much.
00:55
And we were given that p1 is at a gauge pressure of three atmospheres.
01:04
Remember, gauge pressure is the pressure above the atmospheric pressure, and p2 is open to the air.
01:13
That's where the hole is, and so it has the atmospheric pressure...