1. point of interest Pressure is a scalar quantity.
“Fluid exerts the same pressure in all directions” means that the force transmitted through an interface near a given point does not depend on the orientation of the interface.
Positive pressure means that adjacent fluid elements are pushing each other
The pushing force acts through the interface and is proportional to the area of the interface.
2x area => 2x force.
point of interest

2. Hydrostatic equilibrium (no motion, no net forces)
Condition for hydrostatic equilibrium – constant pressure throughout the fluid volume.
Variation of pressure creates net force in the direction of decreasing pressure.

3. Hydrostatic equilibrium with external forces: Gravity
Force from above (pushing down)
Force from below (pushing up)
Gravitational force (pulling down)
Balance (equilibrium) equation

4. Hydrostatic equilibrium with external forces: Gravity
We have got a differential equation… Where do we go from here?
We need to integrate it. Can we?
If both r and g are constant, certainly yes.
What is P0? And BTW, what is h?
P0 is the constant of integration – the value of pressure at h = 0.
It is natural to count h downwards from the fluid surface (h = depth). Then P0 is the pressure at the surface – the atmospheric pressure.
If the atmospheric pressure changes, does the pressure at a given depth change?
Yep!

5. Hydrostatic equilibrium with external forces: Gravity
We have got a differential equation… Where do we go from here?
We need to integrate it. Can we?
If both r and g are constant, certainly yes.
What is P0? And BTW, what is h?
Pascal’s law: a pressure change anywhere in a fluid is felt throughout the fluid.

6. Hydrostatic equilibrium with external forces: Gravity
The density, r, is only constant in liquids. Gasses are compressible, and one must assume variable r(h).
Earth atmosphere:

7. Pressure at the surface of water or at 0 altitude is the usual good candidate for P0
Ocean (or cup).
Atmosphere
Here h is the depth.
Here h is the altitude.
Pressure grows by about 1 atm (105 Pa) every 10 m
Pressure drops by about 120 Pa every 10 m

8. Drinking through a straw.
When you get a tooth extracted you are warned not to drink through a straw. Why so?
The pressure of liquid at the top of the straw is
For you to drink, the pressure inside your mouth should drop below Ptop. This implies a substantial negative pressure difference, rgh, between the blood vessels in your gums and your mouth, which may open the wound.

9. The total force acting on the bottom of the vessel is
The most remarkable thing about the expression for pressure is what it does not include.
The expression for hydrostatic pressure is easy to see for the straight, unobstructed column, but not obvious for more contorted geometries.
The force exerted on the bottom may be strikingly different from the weight of the liquid!

10. P1 = P2 Win = Wout Hydraulic lift
A multiplication of force can be achieved by the application of fluid pressure according to Pascal's principle, which for the two pistons implies           
P1 = P2
This allows the lifting of a heavy load with a small force, as in an auto hydraulic lift…
Hydraulic lift
but of course there can be no multiplication of work, so in an ideal case with no frictional loss:
Win = Wout

11. Hydraulic lift is very similar to a lever….
“GIVE ME A PLACE TO STAND AND I WILL MOVE THE EARTH”
Archimedes

12. A vacuum cleaner Does the vacuum suck the dust?
Strictly speaking the pump of the cleaner creates lower pressure inside it and the air and dust are driven into the hose by the pressure of the atmosphere.

13. r = 13600 kg/m3 - density of mercury
A barometer
evacuated volume
Pressure of the air, Patm, drives mercury into the hollow tube.
There is no air and no pressure inside the tube. Therefore Patm is balanced by hydrostatic pressure of the mercury. h
Patm = rgh
r = kg/m3 - density of mercury

14. A manometer – pressure gauge
Now there is a fluid (gas) under pressure in the reservoir.
The difference between the pressure inside the reservoir, Pres, and Patm is now balanced by hydrostatic pressure of the mercury.
– gauge pressure
– absolute pressure
A manometer is measuring gauge pressure

15. Buoyant force
Archimede’s principle: The buoyant force on an object is equal to the weight of the fluid displaced by the object.
The buoyant force is applied to the center of gravity of the fluid (center of the submerged volume of the body).

16. Archimedes principle: The buoyant force on an object is equal to the weight of the fluid displaced by the object, Vdisp rfluid g.
Ship empty.
Ship loaded with 50 ton of iron.
Ship loaded with 50 ton of styrofoam.
Volume of the submerged part of the ship (or any other floating object) is equal to the mass of the ship divided by the density of water:

17. Equal Volumes Feel Equal Buoyant Forces
Suppose you had equal sized balls of cork, aluminum and lead, with respective densities of 0.2, 2.7, and 11.3 times the density of water. If the volume of each is 10 cubic centimeters then their masses are 2, 27, and 113 gram.
Each would displace 10 grams of water, yielding apparent masses of -8 (the cork would accelerate upward), 17 and 103 grams respectively (and weights of -0.08, 0.17 and 1.03 N).
Apparent mass can be defined as apparent weight divided by the gravitational acceleration, g.

18. Center of gravity vs. center of buoyancy
Gravitational force is applied at the center of gravity. Buoyancy force is applied to the center of buoyancy. Center of gravity should be below center of buoyancy for stable equilibrium.
Is that a necessary condition of equilibrium?
There is something wrong with the picture on the left… What?
Center of buoyancy is the center of volume of the submerged part of the boat. It cannot possibly be at or above the water-line!