A Treatise On Statics, With Applications to Physics

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But PQ = — F'Q, therefore the element of potential = •^•■^t-t > which bears the constant ratio, -=• > to the potential of the element i> « at P'. Hence the potential of the whole shell at P is -j: times the potential at F', or ^ « _ iTTypra' ^= D ' which is the same as if the shell were condensed into a particle at its centre. • j p The resultant attraction-intensity at P = ~jn (measured towards O), which gives the same result as before.
These results can also be easily deduced analytically by
...breaking up the shell into zones, as has been done (p. 246) in calculating the force-intensity at P and P'. Thus, the mass of a zone being, as in p. 246, 2irpT~rdr where r=P'Q or PQ, the potential produced " a by the zone is 2i[ypT—dr; and for the internal point the limits of c r are a+ c, while for the external point they are c+ a.
The value of V can also be deduced from the differential equation (y), Art. 329. For V depends solely on the distance, r, of the in- ternal point from the centre, and not on 6 or .


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