Elements of the Integral Calculus : With a Key to the Solution of Differential Equations

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(3) Jo Joz For, in the second one, which agrees best with the figure, we must take our limits so that the limit of the sum of the projec- tions may be the quadi-ant in which the sphere is cut by the Chap. XI.] AEEAS OF SURFACES.
125 plane XZ ; and the equation of this section is obtained hj letting 2/ = in the equation of the sphere, and is whence z = Va^ — af.
If we take as our limits in the integral ( - clz zero and -s/ar— x^ ^ y we shall get the area whose projection is a strip running from
...the axis of Z to the curve ; then, taking j ( j - f^ ) f?^ from to a, we shall get the area whose projection is the sum of all these strips, and that is om- required surface.
y = Va^_a;2.
(T=al I — Jo Jo Va^ -x'-z^ f clz Vci^ — 3Cp — = sin"-^ - Vcr — af if we regard x as constant ; c7o- >/rt2-a;2 dz cr — a \ -ax = — , Jo 2 2 the required area. Formulas (1) and (3) give the same result.
133. Suppose two cylinders of revolution drawn tangent to each other, and perpendicular to the plane of a great circle of a sphere, each having the radius of the great circle as a diameter ; required the surface of the sphere not included by the cylinders.


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