In finding the motion of heat in a sphere, Fourier expands a function , arbitrary between the limits and , in a series of the form
where , , &. are the successive roots of the equation
Now Fourier gives no demonstration of the possibility of this expansion, but he merely determines what the coefficients , , & would be, if the function were represented by a series of this form. Poisson arrives, by another method, at the same conclusion as Fourier, and then states this objection to Fourier’s solution; but, as is remarked by Mr Kelland (Theory of Heat, p. 81, note), he “does not appear, as far as I can see, to get over the difficulty.” The writer of the following article hopes that the demonstration in it will be considered as satisfactory, and consequently as removing the difficulty.
Let , , and
Then the preceding series will take the form
the accents being omitted above .
Now it is shewn by Fourier, that