The previous considerations can be extended to include curved areas:

Let
In Fig. 1a imagine a fluid element bounded by
To find the vertical component, we imagine that the element extends to the free surface, as in Fig. 1b. The force on the top of this element will then be zero, and the condition for equilibrium is:
If we apply the above principles to the case of a closed area, such as the surface of a submerged body, we are led directly to Archimedes’ Principle for a floating body.
Consider the forces acting upon a cylindrical element of a submerged body, as shown in Fig. 2.

Considering the area at