In the transformation from cartesian to polar coordinates r2 = x2 + y2
The bounds of integration are particularly nice because they don't depend on θ , the angle. Therefore, the integration is from r2 = 4 to 9. This has the solutions for r positive or negative, but if we allow the angle to go from 0 to 2pi, we can state the limits as r = [2,3] and θ = [0,2pi]
The integral becomes (I'm assuming the A is under the integral sign indicating the limits)
Int from 0 to 2π(Int from 2 to 3(sin(r2) rdr)dθ)
Note that rdrdθ is the areal element in polar coordinates.
Nothing depends on θ, so we can do that integral first
Integral = 2π (Int from 2 to 3 of (sin(r2) rdr) ) which is integrable as 1/2sin(u) du
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