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Advanced Topics in Single-Variable Calculus and an Introduction to Multivariable Calculus
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Calculus Textbooks Boundless Calculus Advanced Topics in Single-Variable Calculus and an Introduction to Multivariable Calculus Multiple Integrals
Calculus Textbooks Boundless Calculus Advanced Topics in Single-Variable Calculus and an Introduction to Multivariable Calculus
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Calculus
Concept Version 5
Created by Boundless

Change of Variables

One makes a change of variables to rewrite the integral in a more "comfortable" region, which can be described in simpler formulae.

Learning Objective

  • Use a change a variables to rewrite an integral in a more familiar region


Key Points

    • There exist three main "kinds" of changes of variable (to polar coordinate in R2R^2R​2​​, and to cylindrical and spherical coordinates in R3R^3R​3​​); however, more general substitutions can be made using the same principle.
    • When changing integration variables, make sure that the integral domain also changes accordingly.
    • Change of variable should be judiciously applied based on the built-in symmetry of the function to be integrated.

Term

  • polar coordinate

    a two-dimensional coordinate system in which each point on a plane is determined by a distance from a fixed point and an angle from a fixed direction


Full Text

The limits of integration are often not easily interchangeable (without normality or with complex formulae to integrate). One makes a change of variables to rewrite the integral in a more "comfortable" region, which can be described in simpler formulae. To do so, the function must be adapted to the new coordinates.

For example, for the function f(x,y)=(x−1)2+yf(x, y) = (x-1)^2 +\sqrt yf(x,y)=(x−1)​2​​+√​y​​​, if one adopts this substitution x′=x−1, y′=yx' = x-1, \ y'= yx​′​​=x−1, y​′​​=y, therefore x=x′+1, y=y′x = x' + 1, \ y=y'x=x​′​​+1, y=y​′​​, one obtains the new function:

f2(x,y)=(x′)2+yf_2(x,y) = (x')^2 +\sqrt yf​2​​(x,y)=(x​′​​)​2​​+√​y​​​

which is simpler than the original form. When changing integration variables, however, make sure that the integral domain also changes accordingly. In the example, if integration is performed over xxx in [0,1][0,1][0,1]] and y in [0,3][0,3][0,3], the new variables x′x'x​′​​ and y′y'y​′​​ vary over [−1,0][-1,0][−1,0] and [0,3][0,3][0,3], respectively. There exist three main "kinds" of changes of variable (one in R2R^2R​2​​, two in R3R^3R​3​​); however, more general substitutions can be made using the same principle.

1. Polar coordinates

The function to be integrated transforms as:

f(x,y)→f(ρcosϕ,ρsinϕ)f(x,y) \rightarrow f(\rho \cos \phi,\rho \sin \phi )f(x,y)→f(ρcosϕ,ρsinϕ)

and the integral accordingly changes as:

∬Df(x,y) dxdy=∬Tf(ρcosϕ,ρsinϕ)ρdρdϕ\displaystyle {\iint_D f(x,y) \ dx\, dy = \iint_T f(\rho \cos \phi, \rho \sin \phi) \rho \, d \rho\, d \phi}∬​D​​f(x,y) dxdy=∬​T​​f(ρcosϕ,ρsinϕ)ρdρdϕ

2. Cylindrical coordinates

The function to be integrated transforms as:

f(x,y,z)→f(ρcosϕ,ρsinϕ,z)f(x,y,z) \rightarrow f(\rho \cos \phi, \rho \sin \phi, z)f(x,y,z)→f(ρcosϕ,ρsinϕ,z)

and the integral accordingly changes as:

∭Df(x,y,z)dxdydz=∭Tf(ρcosϕ,ρsinϕ,z)ρdρdϕdz\displaystyle {\iiint_D f(x,y,z) \, dx\, dy\, dz = \iiint_T f(\rho \cos \phi, \rho \sin \phi, z) \rho \, d\rho\, d\phi\, dz}∭​D​​f(x,y,z)dxdydz=∭​T​​f(ρcosϕ,ρsinϕ,z)ρdρdϕdz

Cylindrical Coordinates

Changing to cylindrical coordinates may be useful depending on the setup of problem.

3. Spherical coordinates

The function to be integrated transforms as:

 f(x,y,z)⟶f(ρcosθsinϕ,ρsinθsinϕ,ρcosϕ)f(x,y,z) \longrightarrow f(\rho \cos \theta \sin \phi, \rho \sin \theta \sin \phi, \rho \cos \phi)f(x,y,z)⟶f(ρcosθsinϕ,ρsinθsinϕ,ρcosϕ)

and the integral accordingly changes as:

$\displaystyle {\iiint_D f(x,y,z) \, dx\, dy\, dz \\ = \iiint_T f(\rho \sin \phi \cos \theta, \rho \sin \phi \sin \theta, \rho \cos \phi) \rho^2 \sin \phi \, d\rho\, d\theta\, d\phi}$

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