Green's theorem is a vector identity which is equivalent to the curl theorem in the plane. Over a region in the plane with boundary
, Green's theorem states
|
(1) |
where the left side is a line integral and the right side is a surface integral. This can also be written compactly in vector form as
|
(2) |
If the region
is on the left when traveling around
, then area of
can be computed using the elegant formula
|
(3) |
giving a surprising connection between the area of a region and the line integral around its boundary. For a plane curve specified parametrically as for
, equation (3) becomes
|
(4) |
which gives the signed area enclosed by the curve.
The symmetric form above corresponds to Green's theorem with and
, leading to
However, we are also free to choose other values of and
, including
and
, giving the "simpler" form
|
(10) |
and
and
,
giving
|
(11) |
A similar procedure can be applied to compute the moment about the -axis using
and
as
|
(12) |
and about the -axis
using
and
as
|
(13) |
where the geometric centroid is given by
and
.
Finally, the area moments of inertia can be computed using
and
as
|
(14) |
using
and
as
|
(15) |
and using
and
as
|
(16) |
See also
Area, Area Moment of Inertia, Curl Theorem, Divergence Theorem, Geometric Centroid, Multivariable Calculus, Stokes' Theorem
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References
Arfken, G. "Gauss's Theorem." §1.11 in Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, pp. 57-61, 1985.Kaplan, W. "Green's Theorem." §5.5 in Advanced Calculus, 4th ed. Reading, MA: Addison-Wesley, pp. 286-291, 1991.
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Cite this as:
Weisstein, Eric W. "Green's Theorem." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/GreensTheorem.html