Integral said:
The best I can interpret what you are saying the formula I gave you on my first post is the one you want.
S = 2 \pi R h
Where R is the Radius of the sphere
h would be the distance from the ground to the top of the dome.
No, Integral, that's the lateral area of a cylinder of radius R and height h.
Here's how I would do it:
Set up a coordinate system have origin at the center of the sphere and positive z axis perpendicular to the base of the dome.
The equation of the sphere is F(x,y,z)= x
2+ y
2+ z
2= R
2 and we think of that as a "level surface" for a function F(x,y,z). Then grad F= 2xi+ 2yj+ 2zk is normal to the sphere at each point. We can "normalize" that, using the xy-plane as reference by dividing by the z component: dS= ((x/z)i+ (y/z)j+ k). The "differential of surface area" is The length of that, &sqrt;((x
2/z
2)+ (y
2)/z
2)+ 1)dA. That is the same as (&sqrt(x
2+ y
2+ z
2)/z)dA= (R/z)dA.
z= √(R
2- x
2- y
2) so it is simplest to do the integral in polar coordinates: the differential of surface area is (R/√(R
2- r
2))rdrdθ
Now, if the height of the dome is h< R, the z= R-h and the equation of the sphere becomes x
2+ y
2+ (R-h)
2=
r
2+ R
2- 2hR+ h
2= R
2 so
that r
2= 2hR- h
2 and the integration over r will be from 0 to √(2hr- h
2).
Since θ does not appear explicitely in the integral the θ integral is just 2π.
The surface area is 2π integral of (R/√(R
2- r
2)rdr with limits of integration r=0 to √(2hr- h
2).
That can be integrated by letting u= R
2- r
2 so that
du= -r dr and the integration is from u= R to R
2- 2hr+ h
2= (R-h)
2.
In terms of u, the surface area is 2πRintegral of u
-1/2du=
4πRu
1/2 evaluated between (R-h)2 and R2: that is, of course, 4πR(R- (R-h))= 4πRh, exactly twice what Integral said.