This explanation clarifies the concept of the centre of buoyancy, often denoted as '$B$', in fluid mechanics. Understanding the centre of buoyancy is crucial for analyzing the stability of both submerged and floating bodies. It relates directly to the buoyant force experienced by an object immersed in a fluid.
When an object is placed in a fluid (like water or air), it experiences an upward force. This force is known as the buoyant force. According to Archimedes' Principle, the magnitude of this buoyant force is equal to the weight of the fluid that the object displaces.
Mathematically, the buoyant force ($F_B$) can be expressed as:
$F_B = \rho_{fluid} \times V_{displaced} \times g$
Where:
The centre of buoyancy ($B$) is the specific point where this buoyant force effectively acts. It is defined as:
The centre of gravity of the volume of fluid displaced by the body.
Key points about the centre of buoyancy ($B$):
Let's examine why the other options are not the correct definition of the centre of buoyancy:
Therefore, the most accurate definition of the centre of buoyancy ($B$) for any body in fluid mechanics is the center of gravity of the volume of fluid displaced by the body. The buoyant force acts vertically upwards through this point.
The volume of a sealed packet is 1 liter and its mass is 800 g. The packet is first put inside the water with a density of 1 g cm -3 and then in another liquid B with a density of 1.5 g cm -3 . Then which one of the following statements holds true?
Buoyancy is a/an
A metallic sphere with an internal cavity weight 40g in air and in water it weighs 20g. If the density of material with cavity be 8 gm/cc then the volume of cavity is:
A piece of copper of density 8.8 g/cm 3 having an internal cavity weight 264 g in air and 221 g in water. the volume of cavity is: