Integration (Intermediate)
Integral theorems of vector calculus (upper-undergraduate level)
Overview of the Intermediate Level
At the intermediate level, we study the integral theorems of vector calculus: line integrals along curves, surface integrals over surfaces, and the three great integral theorems of Green, Stokes, and Gauss.
Learning Goals
- Understand the definition and computation of line integrals
- Understand surface integrals and flux
- Understand and apply Green's theorem
- Understand Stokes' theorem
- Understand the Gauss divergence theorem
- Understand the three integral theorems as unified through the generalized Stokes theorem
Contents
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Chapter 1
Line Integrals of Scalar Fields
Integration along a curve, arc-length parameter
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Chapter 2
Line Integrals of Vector Fields
Work, circulation, conservative fields
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Chapter 3
Green's Theorem
Planar regions and boundary curves, applications
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Chapter 4
Surface Integrals
Parametrization of surfaces, flux
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Chapter 5
Stokes' Theorem
Surfaces and boundary curves, curl
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Chapter 6
The Gauss Divergence Theorem
Closed surfaces, divergence, physical applications
Related Topics
- Differentiation under the integral sign (Feynman's trick) — Explains differentiation under the integral sign (the Leibniz integral rule, Feynman's trick).
- Evaluating the Gaussian integral — Evaluates the Gaussian integral $\int e^{-x^2}\,dx=\sqrt{\pi}$ by several methods: polar-coordinate change, differentiation under a parameter, and complex integration.
- Real integrals via residues — Explains how to compute real definite integrals using the residue theorem.
Prerequisites
- The content of Integration (Basic)
- Vector differentiation (gradient, divergence, curl)
- Parametrization of curves and surfaces
The Three Great Integral Theorems
Green's theorem
When $D$ is a region in the plane and $\partial D$ is its boundary:
$$\oint_{\partial D} (P\,dx + Q\,dy) = \iint_D \left(\dfrac{\partial Q}{\partial x} - \dfrac{\partial P}{\partial y}\right) dA$$Stokes' theorem
When $S$ is a surface and $\partial S$ is its boundary curve:
$$\oint_{\partial S} \mathbf{F} \cdot d\mathbf{r} = \iint_S (\nabla \times \mathbf{F}) \cdot d\mathbf{S}$$Gauss's divergence theorem
When $V$ is a three-dimensional region and $\partial V$ is its boundary surface:
$$\iint_{\partial V} \mathbf{F} \cdot d\mathbf{S} = \iiint_V (\nabla \cdot \mathbf{F}) \, dV$$Reading
- The boundary tells of the interior — three theorems were one [Reading] — How Green, Stokes, and Gauss are really a single statement: “the integral on the boundary = the integral over the interior.” Tells of the beauty of unification revealed by the generalized Stokes theorem.
- The freedom to change coordinates — multiple integrals, polar coordinates, and Gauss's trick [Reading] — The same integral can come apart at once simply by changing coordinates. Why a double integral can change its clothes, and why the Gaussian integral $\int e^{-x^2}\,dx=\sqrt{\pi}$ resolves so brilliantly in polar coordinates — told all the way to the true nature of the Jacobian.
- The integral that forgets its path — conservative fields and a single hole in space [Reading] — There are line integrals whose value does not change no matter which path joins the same two points. Why an integral can “forget the path and remember only the endpoints” — the conservative fields and potentials behind it, and how a single hole opened in space breaks that magic.
Frequently Asked Questions
What do you learn in intermediate integration?
You study the integral theorems of vector calculus: line integrals along curves (work and circulation), surface integrals over surfaces (flux), and the three great integral theorems of Green, Stokes, and Gauss. The focus is on how to capture a vector field through integration.
How do line integrals and surface integrals differ?
A line integral is an integral along a curve $C$, representing the work $\int_C \mathbf{F}\cdot d\mathbf{r}$ done by a vector field or its circulation. A surface integral is an integral over a surface $S$, representing the flux $\iint_S \mathbf{F}\cdot d\mathbf{S}$ the field carries through the surface. The essential difference is whether the object of integration is a curve or a surface.
Why can Green's, Stokes', and Gauss's theorems be unified into one?
Each expresses the same statement — that the integral over the boundary equals the integral over the interior — and they are all special cases of the generalized Stokes theorem $\int_{\partial\Omega}\omega=\int_\Omega d\omega$. The two-dimensional case is Green's theorem, the surface case is Stokes' theorem, and the three-dimensional case is Gauss's divergence theorem.