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Line integral
∫v*dl, from vectors a to b
Surface integral
∫v*da over a surface S
Volume integral
∫Tdt over volume V with T as a scalar function
Fundamental theorem for gradients
∫(delT)*dl = T(b)-T(a)
Divergence theorem/Gauss’ Law
∫del*Adt = ∫°vda
Fundamental theorem of curls/Stokes
∫(del*f)*da = ∫°f*dl
Field E of a point charge
E = q/4piεr² r
According to the Helmholtz theorem, every vector field is specified by…
The curl, divergence, and boundary conditions
Equation 2.8/Coulomb’s law
E(r ) = 1/4piε∫p(r’)/(script r)² (script r) dt’
[E]
N/C = force/charge
[linear charge density]
charge/length = C/m
Maxwell 1 - differential form
del*E = p/ε
In units, del adds a term of
1/length
Maxwell 1 integral form
∫°E*da = Qencl/ε = flux of E
Maxwell 2
del x E = 0 for statics
Field from potential
E = -delV
Principal of superposition
The total field is just a sum of the individual fields
Poisson’s equation
-del²V = p/ε
Laplace’s equation
-del²V = 0
Force on a point charge q
F = qE