Introduction
a single integral can be thought of as the area under the curve between two points approximated with rectangles.
If we take the limit of the number of rectangles to infinity, we get our 1D integral
integral(a-b) (fx) dx
Double integrals
z = f(x,y)
When we have a function of two variables, we can sum up cuboids with base area dA to find the volume under the 2D curve.
By taking the limit of the number of cuboids to infinity, we have a double integral.
volume = double integral ((limits R at bottom) ( f(x,y) dA))
where R is the 2D region of integration.
Examples of double integrals
Volume = double integral ((limits:R at bottom)(f(x,y))dA)
Area = double integral ((limits: R at bottom)(1)dA)
Second moment of area e.g
Ixx = double integral ((limits: R at bottom)(y^2)dA)
Centre of mass x = 1/M double integral( (xp(x,y)dA)
Iterated integral
Can be expressed as a replacement for double integral. This allows us to evaluate the integral by doing normal integration twice.
Extra notes
We find the volume under the surface f(x,y) by splitting the calculation into two parts:
Evaluate the inner integral to find the equation for the area of a 2D ‘slice’ of the volume
while holding the other variable constant.
This method is also known as partial integration.
The volume is found by outer integral summing these areas together for an arbitrarily large number of slices.
Non rectangular regions
the integration limits contain x and y
we can follow the following steps:
Change of order
A few things to remember:
If the inner integral is dx, draw horizontal strips on R. The lower/upper limits are functions of left / right ends of the horizontal strips.
If the inner integral is dy, draw vertical strips on R. The lower/ upper limits are functions of bottom / top end of the vertical strips
Outer integral limits should contain CONSTANT VALUES ONLY.
Limits are equal to the range of values along the variable of the outer integral for the region R.
Change of Variable
General procedure
Jacobian
j = r in polar coordinates j = detriment of partial derivative of (dx/du, dx/dv,dy,du,dy,dv)