Consider a cylindrical body PQRS of cross-sectional area A immersed in a liquid of density ρ as shown in the figure. Let the upper surface PQ of body be at a depth h1 while it’s lower surface RS be at a depth h2 below the free surface of the liquid.
At depth h1, the pressure on the upper surface PQ
P1 = h1 ρ g
∴ Downward thrust on the upper surface PQ
F1 = pressure x area = h1 ρ g A [Equation 1]
At depth h2, the pressure on the lower surface RS
P2 = h2 ρ g
∴ Upward thrust on the lower surface RS
F2 = pressure x area = h2 ρ g A [Equation 2]
The horizontal thrust at various points on the vertical sides of the body get balanced because liquid pressure is same at all points at the same depth.
From above equations (1) and (2), it is clear that F2 > F1 as h2 > h1 and hence the body will experience a net upward force.
Resultant upward thrust on the body
FB = F2 – F2
= h2ρgA – h2ρgA
= A(h2 – h1)ρg
But, A(h2 – h1) = V, the volume of the body submerged in the liquid.
∴ Upthrust FB = Vρg
Vρg = Volume of solid immersed x density of liquid x acceleration due to gravity
Since a solid when immersed in a liquid, displaces liquid equal to the volume of its submerged part, therefore
Vρg = Volume of liquid displaced x density of liquid x acceleration due to gravity
= mass of liquid displaced x acceleration due to gravity
= weight of the liquid displaced by the submerged part of the body.
Hence,
Upthrust = weight of the liquid displaced by the submerged part of the body.
