Stephen Wiggins, School of Mathematics, University of Bristol
Link Lecture: Differential Forms
1Tuesday, 16 March 2010
Multivariable calculus: What you have learned?
Domains and Ranges of functions: Rn , where distances between points are measured using the Euclidean distance
scalar valued functions on Rn, e.g. energy
vector valued functions on Rn, e.g. a vector field, such as force
curves in Rn i.e. . vector valued functions of a scalar
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What do we want to do with these functions--Calculus
Differentiate them
Integrate them
But the underlying “algebraic structure” is essential, i.e. we (almost) take it for granted that we can “add, subtract, multiply, and divide”
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Differentiation of curves• tangent vectors• curvature
Differentiation of scalar valued functions of a vector variable• gradient• Hessian
Differential properties of vector fields• divergence• curl
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Integration of curves• line integrals
Integration of scalar valued functions• multiple integrals
One general theory encompassing all of this: DIFFERENTIAL FORMS
Élie Joseph Cartan (9 April 1869 – 6 May 1951
Jules Henri Poincaré (29 April 1854 – 17 July 1912)
5Tuesday, 16 March 2010
v ! u = "u ! v
u ! u = 0
c(u ! v) = (cu) ! v = u ! (cv)
u ! (v + w) = u ! v + u !w
2 vectors: the wedge product
Some Properties (I left out associativity, but it is)
Hermann Günther Grassmann (April 15, 1809, Stettin (Szczecin) – September 26, 1877, Stettin
Generalize the idea of vectors and vector spaces: “p-vectors”
6Tuesday, 16 March 2010
F (x, y, z)i+G(x, y, z)j+H(x, y, z)k!" F (x, y, z)dx+G(x, y, z)dy+H(x, y, z)dz
Differential 1 forms and vectors
“work form”
7Tuesday, 16 March 2010
F (x, y, z)i + G(x, y, z)j + H(x, y, z)k!"
F (x, y, z)dy # dz + G(x, y, z)dz # dx + H(x, y, z)dx # dy
Differential 2 forms and 2 vectors
“flux form”
8Tuesday, 16 March 2010
F (x, y, z)dx ! dy ! dz
Differential 3 forms and 3 vectors
9Tuesday, 16 March 2010
d(c1! + c2") = c1d! + c2d"
d(! ! ") = d! ! " + ("1)p! ! d", where ! is a p form
d2 = dd = 0
The “d operator”: the exterior derivative
d of a k form is a k+1 form
define recursively: d of a 0 form is a 1 form (the “usual” derivative)
Basic properties
10Tuesday, 16 March 2010
f is a 0 form, ! and " are 1 forms
d(c1! + c2") = c1d! + c2d"
d(f!) = df ! ! + fd!,
d(dx) = d(dy) = d(dz) = 0
For the relevant assigned problems you can assumed(dy ! dz) = d(dz ! dx) = d(dx ! dy) = 0
The “d operator”: Special CaseBasic properties
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d of a 0 form corresponds to the gradient of a vector fieldd of a 1 form corresponds to the curl of a vector fieldd of a 2 form corresponds to the divergence of a vector field
The relationship with classical vector analysis in 3 Dimensions
12Tuesday, 16 March 2010
A di!erential k form, !, is exact if there is a di!erential k-1 form, ", such that ! = d"
A di!erential k form, !, is said to be closed if d! = 0
An exact form is closed, but a closed form is not necessarily exact
A conservative force field on R3 corresponds to an exact di!erential 1 form
F = !"V
F = !Vxi! Vyj! Vzk"# !dV = d(!V ) = !Vxdx! Vydy ! Vzdz
“Closed and Exact” Differential Forms
Example
13Tuesday, 16 March 2010
! b
ag!(x)dx = g(b)! g(a)
!
CPdx + Qdy =
! !
D
"!Q
!x! !P
!y
#dxdy
Integration: Stokes Theorem
1 dimension: Fundamental Theorem of Calculus
2 dimensions: Greenʼs Theorem (on the plane)
George Green (14 July 1793 – 31 May 1841)
14Tuesday, 16 March 2010
!
volume! · F dV =
!
boundary of volume
F · n dS
! : k-1 form, ! : smooth n dimensional surface!
!d! =
!
!!!
3 dimensions: The divergence theorem
n dimensions: Stokes Theorem
n is a unit vector on the surface of the volume pointing “outwards”
Sir George Gabriel Stokes, 1st Baronet FRS (13 August 1819–1 February 1903)
15Tuesday, 16 March 2010
What do I want you to take away from this lecture?
✓A glimpse of how mathematicians synthesize and generalize “simple ideas” into theories and techniques with far reaching implications and applications
✓An idea of how such generalizations can “free your mind” to think more broadly about problems
✓The ability to do some simple calculations with the wedge product and exterior derivative, and relate these to “standard” ideas in multivariable and vector calculus
16Tuesday, 16 March 2010