Taking the unit sphere in the first octant, we define three curves parallel to the x y , x z and y z planes, parametrically, as follows:
p 1 ( t ) = ( sin θ 0 cos t , sin θ 0 sin t , cos θ 0 ) , 0 ≤ t ≤ 2 π
p 2 ( s ) = ( sin θ 0 cos s , cos θ 0 , sin θ 0 sin s ) , 0 ≤ s ≤ 2 π
p 3 ( r ) = ( cos θ 0 , sin θ 0 cos r , sin θ 0 sin r ) , 0 ≤ r ≤ 2 π
If θ 0 = 0 . 8 4 Radians, then find the area bounded by the three curves of the surface on the sphere, (shaded in yellow)
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We're going to consider the area shaded in light blue in the figure above. It is 6 1 of the required
area (from symmetry). To compute its area we'll define the green arc as the great arc (center at the origin) and characterised by y = z, and the blue arc as the great arc (center at the origin) characterised by x = y.
Blue Area = ∫ ϕ = 4 π ϕ 1 ∫ θ = θ 0 θ 1 sin θ d θ d ϕ
where ϕ 1 is characterised by sin θ 0 sin ϕ 1 = cos θ 0
Therefore, ϕ 1 = sin − 1 ( cot θ 0 )
And sin θ 1 sin ϕ = cos θ 1 , thus θ 1 = tan − 1 ( sin ϕ 1 )
After integration with respect to θ , the above integral becomes,
Blue Area = ∫ ϕ = 4 π ϕ 1 ( cos θ 0 − cos θ 1 ) d ϕ
Since tan θ 1 = sin ϕ 1 then cos θ 1 = 1 + sin 2 ϕ sin ϕ
Hence, the integral becomes,
Blue Area = cos θ 0 ( ϕ 1 − 4 π ) − ∫ ϕ = 4 π ϕ 1 1 + sin 2 ϕ sin ϕ d ϕ
Substituting sin 2 ϕ = 1 − cos 2 ϕ , the integral becomes,
Blue Area = cos θ 0 ( ϕ 1 − 4 π ) − ∫ ϕ = 4 π ϕ 1 2 − cos 2 ϕ sin ϕ d ϕ
Blue Area = cos θ 0 ( ϕ 1 − 4 π ) − ∫ ϕ = 4 π ϕ 1 2 1 − ( cos ϕ / 2 ) 2 sin ϕ d ϕ
Using the substituting u = 2 cos ϕ , the integral becomes
Blue Area = cos θ 0 ( ϕ 1 − 4 π ) + sin − 1 ( cos ϕ 1 / 2 ) − 6 π
Hence, finally, the required area is 6 times the above expression, and is given by
Area = 6 ( cos θ 0 ( ϕ 1 − 4 π ) + sin − 1 ( cos ϕ 1 / 2 ) − 6 π )