4-Vector Cross Product

  • #1
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Could someone tell me if this 4-Vector cross product is correct:

i j k t
dx dy dz 1/c*dt
Ex Ey Ez Et
=[(dy(Ez)-dz(Ey))-(dy(Et)-1/c*dt(Ey))+(dz(Et)-1/c*dt(Ez))]*i
-[(d(E)-d(E))-(d(E)-d(E))+(d(E)-d(E))]*j
+[(d(E)-d(E))-(d(E)-d(E))+(d(E)-d(E))]*k
-[(d(E)-d(E))-(d(E)-d(E))+(d(E)-d(E))]*t
 

Answers and Replies

  • #2
Orodruin
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There is no such thing as a 4-vector cross product. The closest thing you will get is the wedge product between two 1-forms (or rather, its dual), which is a 2-form.
 
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  • #3
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How do you do the wedge product between 2 1-forms.
I searched for Wedge Product. I got Exterior Algebra. Here are some Equations could someone explain the "^" operator to me.
5bb4798f8855d885779dc1fa14ecfb76826766b9
?
1d43519392c264351c893a0bf4595d21d6860a48
where k=4

3d62b07f8c3aa1d58552a995fa3dd79ed5613cdc
?
 
  • #4
Orodruin
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I believe a better path is to identify your purpose, what do you need a generalisation of the cross product for? Once we have established that, we may be able to point you in an appropriate direction.
 
  • #5
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I am trying to solve Maxwell Equations in 4 dimensions.
 
  • #6
Orodruin
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Maxwell’s equations are already in 4 space-time dimensions. Their appearance in the tensor formalism of special relativity takes the form ##\partial_\mu F^{\mu\nu} = J^\nu## and ##\epsilon^{\mu\nu\sigma\rho}\partial_\nu F_{\sigma\rho}=0##, where F is the antisymmetric rank 2 field tensor.
 
  • #7
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To solve for for some Maxwell Equation it takes the cross product:
grad=dx,dy,dz,1/c*dt
dx = partial d/dx
dy = partial d/dy
dz = partial d/dz
dt = partial d/dt

grad X E(r,t) = -dt(B(r,t))

grad X H(r,t) = dt(D(r,t)) + J
 
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