Ryan C. answered 07/27/22
Ivy League Professor | 10+ Years Experience | Patient & Kind
Hi Ayaka,
Thanks for your question!
To solve this problem, we need to use the formula for the surface area of a function z = f(x,y) defined over a region R of the xy-plane:
S = ∫∫R(fx2+fy2+1)1/2dA.
In the formula above, subscripts indicate partial derivatives and dA indicates a small element of area of the region R.
For this problem, we are told f(x,y) = xy/(a+b). Therefore, fx = y/(a+b) and fy = x/(a+b), so our surface area formula becomes
S = ∫∫R((y/(a+b))2+(x/(a+b))2+1)1/2dA,
= 1/(a+b)∫∫R((x2+y2+(a+b)2)1/2dA.
We are told that our surface f must remain in the first octant of 3D space and that it must remain within the cylinder x2+y2 = a2+b2. Consequently, the region R over which f is defined must remain in the first quadrant of the xy-plane and remain inside the circle x2+y2 = a2+b2.
Our region R is best described in polar coordinates (r,θ) instead of rectangular coordinates (x,y). In particular, this region is described by (r,θ) satisfying 0 < r < (a2+ b2)1/2 and 0< θ <π/2. As a result, we express the integral representing our surface area in polar coordinates:
S = 1/(a+b)∫0π/2∫0(a^2+b^2)^(1/2)((r2+(a+b)2)1/2rdrdθ,
where we have used that x2+y2 = r2 and that dA = rdrdθ.
We now can solve our iterated integral. The inner integral can be solved by u-substitution with u = r2 + (a+b)2. After some work, one finds
S = 1/(a+b)∫0π/21/3[(a2+b2+(a+b)2)3/2 - (a+b)3]dθ.
The outer integral is even simpler, as the integrand is effectively constant with respect to θ. We find
S = 1/3[(a2+b2+(a+b)2)3/2 - (a+b)3]/(a+b)∫0π/2dθ,
= π/6[(a2+b2+(a+b)2)3/2 - (a+b)3]/(a+b),
= π/6[(a2+b2+(a+b)2)3/2/(a+b) - (a+b)2].