We can describe a polar rectangle as in the figure below, with \(R= \{(r,θ)|a \le r \le b, \alpha \le \theta \le β \}\).
Consider a function \(f(r,θ)\) over a polar rectangle \(R\). We divide the interval \([a,b]\) into m subintervals \([r_{i-1},r_i]\) of length \(\Delta r=(b-a)/m\) and divide the interval \([α,β]\) into \(n\) subintervals \([θ_{j-1},θ_j]\) of width \(\Delta θ=(β−α)/n\).
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The area \(\Delta A\) of the polar subrectangle \(R_{ij}\) is: approximately:
This is because the subrectangle looks like a trapezoid.The smaller arc length is \(r_{i-1} \Delta \theta\), the larger arc length is \(r_i \Delta \theta\), and both of these arc length are separated by a distance of \(\Delta r\). Let \(r^*_{ij} = \frac{1}{2} (r_{i-1} + r_i)\), we have \(\Delta A = r^*_{ij} \Delta r \Delta \theta\).
Going back to \(f(r, \theta)\). The function \(f\) is defined over the region \(R\). The polar volume of the thin box above \(R_{ij}\) is:
Using the same idea for all the subrectangles and summing the volumes of the rectangular boxes, we obtain a double Riemann sum as:
Now we can define the polar volume as the limit of double Riemann sum:
This becomes the expression for the double integral:
The double integral over a polar rectangular region can be expressed as an iterated integral in polar coordinates:
If \(f\) is given in terms of \(x\) and \(y\), then: