bkvitha said:
I just finished this chapter as well.
I don't understand :
doesnt archimedes principle state that
bouyancy force=the weight of fluid displaced
well...if the object is right at the bottom of its container, didn't any fluid get displaced?!
wouldn't the total of fluid displaced when the object is simply submerged half way through the fluid will equal to to the same amount of fluid displaced when the object reaches the bottom!?
pls o pls correct me if I'm wrong!
ty
Archimedes principle is wonderfully useful when properly applied, but buoyancy is not a fundamental force like gravity or electrical force. In order for an object to float, the force pushing from underneath the object must cancel the weight of the object plus any additional forces pushing it down from above. The beauty of Archimedes principle is that for any object of any weird shape the difference between the upward and downward forces on the object due to the fluid pressure surrounding it is just the weight of the fluid displaced.
The pressure of a fluid acting on an object is the average force applied by molecules of the fluid bombarding the surface of the object. If there is no fluid below the object, there are no molecules to crash into the object.
Fluids have no rigid structure, so any pressure is
isotropic, meaning independent of direction. Solids have rigid structure, so pressure applied to one side is not spread uniformly throughout the material (anisotropic). As a result, an object on the hard bottom of a body of water does not feel the pressure of water at the bottom that it would feel if raised even slightly off the bottom.
In reality, it is very hard to keep the water from leaking in between the object and the hard bottom, so even if the object momentarily stays on the bottom, it will soon be lifted. A porous bottom like sand will not be able to keep an object that normally floats on the bottom.
You can do an experiment to demonstrate this with a small glass and a fairly large sheet of rubber material. Fill a reservoir of water (your sink will do). Invert the glass and let it fill with water until just enough air is left for the glass to float upside down. Press the sheet of rubber against the rim of the glass. You might have to put a bit of a dent in the rubber to squish a bit more water out of the glass. Now let the rubber sheet and the glass sink to the bottom. If the seal is good, the glass will remain in contact with the rubber sheet at the bottom of reservoir for a long time, in spite of the fact that the inverted glass parrtially filled with water is displacing more than its own weight of water. If the seal is not perfect, eventually water will seep into the glass increasing the pressure at the bottom of the air until the glass breaks free of the rubber and floats to the surface.