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Tutorial ID | Title | Tutorial | Video Tutorial | Revision Notes | Revision Questions | |
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9.2 | Buoyancy. Archimedes' Principle |
In these revision notes for Buoyancy. Archimedes' Principle, we cover the following key points:
Buoyancy is the lifting ability of fluids on objects immersed in them. In this sense, we can define buoyancy as an opposing force to gravity caused by the resistance of fluid against any molecular shift caused by the downward tendency of objects' motion. This resistance comes due to the medium's inertia (here, medium is represented by the fluid).
Buoyant force is the upward force exerted by a fluid on an object that is completely or partially immersed in it.
Buoyant force is symbolically expressed as Fb and like all the other forces, it is measured in Newton.
There are three possible positions of an object inside a liquid.
The equation of buoyant force for objects in a liquid is
By measuring the volume of the displaced water, Archimedes calculated indirectly the volume of immersed objects in water. Then, he used the equation of density (density = mass / volume) to find the density of unknown objects. Thus, Archimedes' Principle says:
"The buoyant force acting on an object immersed in a liquid is numerically equal to the weight of the displaced liquid."
Mathematically, we can write the Archimedes principle as
or
Archimedes' Principle is very important in daily life as its applications include a wide range of situation, where the most notorious is the ships construction. Thus, we can use Archimedes' Principle to calculate how much weight a boat or ship can hold without sinking.
We can obtain three important ratios based on the Archimedes' Principle, which give the percentage of the immersed part of a floating object:
where Fb1 is the buoyant force acting on a floating object and Fb2 is the new buoyant force acting on the same object when it is forced to immerse completely in liquid.
We can say the same words for buoyancy in gases as well. The only difference is that in gases there is no floating; we consider the object completely immersed in gas (especially in air). The third case mentioned above when buoyancy in liquids was explain (i.e. when density of object is smaller than the density of gas), is discussed only to see whether the object is moving up or not. Thus, the three cases explained in the buoyancy of liquids adapted for buoyancy in gases are:
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