If D is the union of non-overlapping regions D1 and D2:
∬DfdA=∬D1fdA+∬D2fdA
Change of variables
Suppose that T is a C1 transformation whose Jacobian is nonzero and that it maps a region
S in the uv− plane onto a region R in the xy−plane. and that f is continuous on R and that R and S are type I or type II planar regions. And also that T is one-to-one, except perhaps on the boundary of S. Then:
∬Rf(x,y)dA=∬Sf(x(u,v),y(u,v))∂(u,v)∂(x,y)dA
Derivative under double integral
Suppose f be a function with continuous second partial derivatives on a rectangular
domain R with vertices (x1,y1),(x1,y2),(x2,y2) and (x2,y1), where x1<x2 and
y1<y2.
More generally, this is true if we assume that f is bounded on R, f is discontinuous only on a finite number of
smooth curves, and the iterated integrals exist.
Non-recatangular regions
f is continuous and D lies between two continuous functions of x.
Suppose D=[a,b]×[g1(x),g2(x)].
∬Df(x,y)dA=∫ab∫g1(x)g2(x)f(x,y)dydx
Similarily it can be extended when two continuous functions of y are given.
In Polar Coordinates
f is continuous and D lies between two continuous functions of r.
Suppose D=[a,b]×[g1(r),g2(r)].
∬Df(x,y)dA=∫ab∫g1(r)g2(r)f(r,θ)drdθ
Common Shapes
All the common shapes in polar coordinates are explained below. They are defined in cos. The same version can be adapted for sin.
Archimedes’ Spiral
r=θ
Gradually spirals outwards from (0,0) to (0,2π).
Circle
r=acosθ
Center point is (a/2,0). Radius is a.
Cardioid
a=0.
r=a+bcosθ
Goes through (b+a,0) and (b−a,0).
Shape
When
Cardioid
a=b
One-loop Limacon
b<a<2b
Inner-loop Limacon
a<b
Lemniscate
Suppose a=0.
r2=a2cos(2θ)
Resembles the infinity symbol. Center point is (0,0). Width 2a. Height 2b.