The Advanced Part of a Treatise On the Dynamics of a System of Rigid Bodies Be

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On Repeated Boots. When the root p = mi$ a, repeated root of the equa- tion A Cp)=0, the demonstration just given no longer applies. Since p is arbitrary we may differentiate the equation (1) as often as we please, and after each differen- tiation we may write p = m. Since A (m) = 0, A' (m) = 0, &c. The successive left-hand 20G DETERMINATION OF THE CONSTANTS OF INTEGRATION.
sides reduce to II (m), dU (m)/dm, &o. On the successive right-hand sides we have only terms whioh contain the exponential
... e nt .
It follows that if A (p) =0 have a roots each equal to in, the operators UWl dm » "dm a ' . Fa, — 1 * all produce zero when we substitute for x, y, d'c. Any solutions of the differential equations which do not contain the exponential e mt .
Thus it appears that if we calculate the results of these operations by substitut- ing the particular parts of the values of x, y, &c. Which depend on the root m of the equation A (5) = 0, the results will be general, i. E. , will be the same as if we had substituted the complete values of x, y, &c.


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