Undergraduate → Calculus → Multivariable Calculus ↓
Stokes' Theorem
Stokes' theorem is an important result in vector calculus that connects the surface integral of a vector field over a surface to the line integral of the field along the boundary of that surface. This theorem serves as a powerful tool for converting problems involving complicated surface integrals into simple line integrals and vice versa, leading to easier calculations and a deeper understanding of the behavior of fields and surfaces.
The theorem states: If S
is an oriented, smooth surface with an oriented, closed boundary curve C
, and F
is a vector field whose components have continuous partial derivatives over an open region containing S
, then:
∮_c f • dr = ∬_s curl f • ds
Here, ∮_C
indicates the line integral of the vector field F
along the curve C
, curl F
denotes the curl of F
, and dS
is the vector field on the surface S
Understanding the notation
To better understand Stokes' theorem, let's take a moment to understand the notation and terms involved:
- Vector field (
F
): A function that assigns a vector to every point in space. For example,F(x, y, z) = (P, Q, R)
whereP
,Q
, andR
are functions ofx
,y
, andz
. - Curl (
curl F
): A vector that describes the infinitesimal rotation of a 3D vector field. It is calculatedcurl F = ( ∂R/∂y - ∂Q/∂z, ∂P/∂z - ∂R/∂x, ∂Q/∂x - ∂P/∂y )
- Surface integral (denoted as
∬
): An integral where we integrate over a surface. For Stokes' theorem, the surface integral accounts for the component of the curl perpendicular to the surface at each point. - Line integral (noted as
∮
): An integral that involves integration over a curve or line. - Surface (
S
): A two-dimensional manifold, which is essentially a 2D shape like a piece of paper or a sea wave. In mathematics, these manifolds can be infinitely large and can be described by equations. - Boundary curve (
C
): The closed curve that outlines the surfaceS
Now that we understand the main components and variables involved in the theorem, the main purpose of Stokes' theorem is to equate these two types of integrals - the surface integral over the surface S
and the line integral around the boundary C
Analogies and visualizations
To understand Stokes' theorem intuitively, consider the following analogy: Imagine a field of wind flowing over a surface such as a piece of cloth, where each vector in the field represents both the direction and speed of the wind at that point. The curve C
represents the boundary of the cloth. Stokes' theorem tells us that the "swirl" effect of the wind across the surface of the cloth (represented by curl F
) is equal to the cumulative effect measured around the boundary.
Let's use a visual example to make this clear. Consider a rectangular piece of fabric whose edges form a border curve:
In the illustration, the red arrows indicate a vector field acting on the surface S
The line integral along C
will involve the sum of the effects of this vector field along the path of the boundary. However, computing the curl on S
allows for the simplification described by Stokes' theorem: turning this 3D complexity into a 2D boundary construction.
Application of Stokes theorem: An example
Let us work through an example to further strengthen our understanding:
Suppose we have a vector field F = (xz, yz, z)
, and we are dealing with a surface S
that is shaped as the part of the sphere x² + y² + z² = 1
in the first octant, that is, only where x, y, z
are non-negative and where z = 0
is a circular disk of radius 1.
The limit curve C
is the circle at the vertex when z = 1
We are to evaluate the line integral ∮_C F • dr
using Stokes' theorem.
First, let's find curl F
:
F = (xz, yz, z) curl F = (∂/∂y (z) - ∂/∂z (yz), ∂/∂z (xz) - ∂/∂x (z), ∂/∂x (yz) - ∂/∂y (xz)) = (0 – y, x – 0, y – x) = (-y, x, y – x)
The main component contributing to our surface integral is the component perpendicular to the surface (-y, x, yx)
.
For the surface z = 1
, we evaluate the double integral of k
component (yx)
over the surface.
∬_S curl F • dS = ∬_S (y-x) dS
Let's parametrize x² + y² = 1
in this surface with polar coordinates: x = r cosθ
, y = r sinθ
, where r
goes from 0
to 1
and θ
from 0
to π/2
.
∬_s(yx)ds = ∫_(0)^(π/2)∫_(0)^(1) (r sinθ - r cosθ) r dr dθ = ∫_(0)^(π/2)∫_(0)^(1) (r² sinθ - r² cosθ) dr dθ
By computing the inner integral and then the outer integral, we find that the area integral is equivalent to the line integral around C
, thereby verifying Stokes' theorem.
Key concepts and implications
- Stokes theorem helps in converting surface integrals to line integrals and vice versa, which is important when calculating one type of integral is simpler.
- The vector field
curl
provides important information about rotational behavior within the field, which is often applied in physics problems. - This theorem generalizes several fundamental theorems of vector calculus, including both Green's theorem and the divergence theorem.
From understanding weather patterns to the behavior of electromagnetic fields, Stokes' theorem provides valuable insights and connects the three-dimensional understanding of the nature of vector fields to two-dimensional intuitive concepts.