698 Iterated and multiple integrals
We therefore use this number as an approximation to the pth moment
of the subset. The sum
(13.644) Z(x - xo)PS(x,y,z) Ax Ay Az,
which contains a term for each subset, should then be a good approxima-
tion to the total pth moment of the whole solid whenever the diameters
of the subsets are all small. This leads us to the formula
(13.645) M = lim E(x - xo)'S(x,y,z) Ax Ay Az,
the right side of which is taken to be the definition of the number M=P'zp
which we are seeking. In accordance with the definition of triple integ-
rals, the right side of (13.645) is a triple integral which we can denote by
one or the other of the symbols in the formula
(13.646) Mz-'Z, = fffs (x-xo)PS(x,y,z) dS
=f f fs (x- xo)"5(x,y,z) dx dy dz.
With the aid of Theorem 13.63, we can undertake to express the triple
integral in terms of iterated integrals in various ways. It is, however,
worthwhile to learn to use a procedure which leads directly to iterated
integrals. As above, we build up the expression
(13.65) (x - xo)'S(x,y,z) Ax Ay Az
to serve as an approximation to the required moment of a single subset.
We then form the sum
(13.651) Ax Ay I (x - xo)'S(x,y,z) Az,
x,11 fixed
where the part "x, y, fixed" of the symbol serves to inform us that the
sum contains only terms arising from those subsets which comprise a
single vertical column such as that shown in Figure 13.64. Thus (13.651)
and the number
I:(x.v)
(13.652) dx Dy f
(x y) (x - xo)'S(x,y,z) dz
are approximations to the required moment of one column. Next we
form the sum
(13.653) Ax I Ay (x -
x fixed
Ji(x,y) xo)'S(x,y,z) dz,
where the part "x fixed" of the symbol serves to inform us that the sum
contains only terms arising from columns that comprise a slab running
from the cylinder on which y = yl(x) to the cylinder on whichy = y2(x).