Problem #0076 Mechanics Sub-menu Problem #0078 Chapters Chapters

77 (c).

Hydrostatic Equilibrium in Spherical Fluid Mass

We have to show that in a homogeneous spherical fluid mass of radius R and density , pressure at a distance r from the centre of the sphere is

For the Earth taking and , we have to find the pressure at the centre.

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Let us consider a cylindrical surface of unit cross-section width at a distance r from the centre of the spherical fluid system in hydrostatic equilibrium. Condition of equilibrium for this fluid element is that the inward gravitational pull on it has to be balanced by the pressure force acting on its opposite faces, each of which is assumed to be unit cross-sectional area. Let the pressure inside the fluid be denoted by the function .

The inward gravitational pull on this fluid element will be the force due to the fluid mass contained in the sphere of radius r and acting from its centre. That is

Net pressure force acting in the outward radial direction will be

Condition of equilibrium

gives the equation for pressure variation,

Integrating this equation, we get

Requiring that at the boundary of the fluid mass pressure is zero, , we find

Radial variation of pressure is, therefore, given by the function

We next calculate the pressure at the centre of the Earth considering it to be a homogeneous spherical fluid mass of radius and density.

Substituting the values, we find that