Buoyancy is defined as the tendency of a body to float or rise when submerged in a fluid.
We
all have had numerous opportunities of observing the buoyant effects of a liquid. When we go
swimming, our bodies are held up almost entirely by the water. Wood, ice, and cork float on
water. When we lift a rock from a stream bed, it suddenly seems heavier on emerging from the
water. Boats rely on this buoyant force to stay afloat. The amount of this buoyant effect was
first computed and stated by the Greek philosopher Archimedes. When a body is placed in a
fluid, it is buoyed up by a force equal to the weight of the water that it displaces.
If a body weighs more than the liquid it displaces, it sinks but will appear to lose an amount of
weight equal to that of the displaced liquid, as our rock. If the body weighs less than that of the
displaced liquid, the body will rise to the surface eventually floating at such a depth that will
displace a volume of liquid whose weight will just equal its own weight. A floating body
displaces its own weight of the fluid in which it floats.
Compressibility
Compressibility is the measure of the change in volume a substance undergoes when a pressure
is exerted on the substance. Liquids are generally considered to be incompressible. For instance,
a pressure of 16,400 psig will cause a given volume of water to decrease by only 5% from its
volume at atmospheric pressure. Gases on the other hand, are very compressible. The volume
of a gas can be readily changed by exerting an external pressure on the gas
Relationship Between Depth and Pressure
Anyone who dives under the surface of the water notices that the pressure on his eardrums at a
depth of even a few feet is noticeably greater than atmospheric pressure. Careful
measurements
show that the pressure of a liquid is directly proportional to the depth, and for a given depth
the
liquid exerts the same pressure in all directions.
The pressure of the liquids in each of the previously cited cases has been due to the weight of
the liquid. Liquid pressures may also result from application of external forces on the liquid.
Consider the following examples. Figure 2 represents a container completely filled with liquid.
A, B, C, D, and E represent pistons of equal cross-sectional areas fitted into the walls of the
vessel. There will be forces acting on the pistons C, D, and E due to the pressures caused by
the different depths of the liquid. Assume that the forces on the pistons due to the pressure
caused by the weight of the liquid are as follows: A = 0 lbf, B = 0 lbf, C = 10 lbf, D = 30 lbf,
and E = 25 lbf. Now let an external force of 50 lbf be applied to piston A. This external force
will cause the pressure at all points in the container to increase by the same amount. Since the
pistons all have the same cross-sectional area, the increase in pressure will result in the forces
on the pistons all increasing by 50 lbf. So if an external force of 50 lbf is applied to piston A,
the force exerted by the fluid on the other pistons will now be as follows: B = 50 lbf, C = 60
lbf, D = 80 lbf, and E = 75 lbf.