An introduction to the mathematical theory of attraction ...

60 Lines of Force. EXAMPLES. 1. Determine the lines of force and the equipotential surfaces in the interior of a homogeneous ellipsoid. The differential equations of a line of force are dx dy dz Ax y Cz' where A,, Care the same as in (15), Art. 21. Integrating these equations we have zu = K1x = - 2y where K1 and K2 are arbitrary constants. The differential equation of an equipotential surface is Ax dx + By dy + Cz dz = O, which integrated becomes Ax2 + By2 + Cz2 = E, where K is an arbitrary constant. 2. The attraction of a homogeneous spherical shell at an internal point is zero, and at an external point is the same as if its entire mass were concentrated at its centre. It is obvious from symmetry that the shell is centrobaric both for an internal and an external point, the baric centre being the centre of the sphere. Hence by Art. 38 we obtain the above results. 3. If the resultant force in unoccupied space be uniform in direction it must be uniform in magnitude. In this case the lines of force are parallel straight lines; a tube of force is therefore a cylinder whose section is constant. Hence by Art. 28 the force is constant along any one line of force; and by a method similar to that employed in Art. 38, we can show that the force does not vary in going from one line of force to another. In this case the equipotential surfaces are planes. 4. A hollow closed conductor is charged with electricity in equilibrium. If there be no mass in the interior hollow, show that at every point in it the resultant force is zero, and that there is no charge at any point on the inner surface of the conductor. Since the interior hollow @ is unoccupied, no tube of force can begin or end there; and therefore, since a tube of force cannot be a closed curve, if there be a tnbe of force in @, it must begin and end on the interior surface of the conductor, which by Art. 31 is impossible. Again, since there is no force on either side of the interior surface of the conductor, by Art. 29 there can be no charge.

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Title
An introduction to the mathematical theory of attraction ...
Author
Tarleton, Francis Alexander.
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Page 42
Publication
London:: Longmans, Green & Co.,
1899-1913.
Subject terms
Attractions

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"An introduction to the mathematical theory of attraction ..." In the digital collection University of Michigan Historical Math Collection. https://name.umdl.umich.edu/abr3212.0001.001. University of Michigan Library Digital Collections. Accessed June 23, 2025.
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