We can solve algebraically for the bounds of integration, which are the theta values of the points of intersection between the two polar curves. These points lie in Quadrant IV and I:
2 + 2 cosΘ = 3
cosΘ = 1/2
Θ = - π/3 or π/3
For Θ in this range, r2 > r1, so we integrate 1/2(r2 - r1)2 dΘ as follows:
A = ∫-π/3π/3 [1/2(2 + 2 cosΘ - 3)2] dΘ
= 1/2 ∫-π/3π/3 [(2 cosΘ - 1)2] dΘ
= 1/2 ∫-π/3π/3 [4 cos2Θ - 4cosΘ + 1] dΘ ...
Note: 4cos2Θ can be integrated by using the double-angle identity cos2Θ = (cos2Θ + 1) / 2