Square root of volume in fourier expansion of the vector potential

Click For Summary
SUMMARY

The discussion centers on the use of the factor \( \frac{1}{\sqrt{V}} \) in the Fourier expansion of the vector potential \( \vec A(\vec r,t) \). This convention is primarily adopted to simplify the expression of the Poynting energy of the field within a volume \( V \), avoiding the introduction of \( V \) in the total energy calculations. The standard Fourier expansion without this factor would lead to complications in dimensional consistency, particularly affecting the dimensions of the coefficients \( \vec A_{0 \vec{k}}(t) \), which are expressed as having dimensions of \( [A(\vec r,t)] \mathrm{m}^{3/2} \).

PREREQUISITES
  • Understanding of Fourier expansion in three dimensions
  • Familiarity with vector potentials in electromagnetism
  • Knowledge of the Poynting theorem and energy density in electromagnetic fields
  • Basic grasp of dimensional analysis in physics
NEXT STEPS
  • Study the derivation of the Poynting vector and its implications in electromagnetic theory
  • Explore the role of Fourier transforms in quantum mechanics and field theory
  • Investigate the dimensional analysis of physical quantities in electromagnetic equations
  • Learn about the conventions used in quantum field theory, particularly in radiation theory
USEFUL FOR

Physicists, electrical engineers, and students studying electromagnetism or quantum field theory who seek to understand the mathematical conventions used in vector potential expansions and their implications for energy calculations.

center o bass
Messages
545
Reaction score
2
Hi. I just wondered why we use a [itex]1/\sqrt{V}[/itex] in the Fourier expansion of the vector potential. A regular 3 dimensional Fourier expansion is just

[tex]f(\vec r) = \sum_{\vec k} c_\vec{k} e^{i \vec k \cdot \vec r}[/tex]

but as the solution to the equation

[tex](\frac{\partial ^2}{\partial t^2} - \nabla^2 ) \vec A(\vec r,t) = 0[/tex]

one usually writes

[tex]\vec A(\vec r,t) = \frac{1}{\sqrt{V}}\sum_{\vec k} \vec A_{0 \vec{k}}(t) e^{i \vec k \cdot \vec r}.[/tex]

What is the reason for this? Doesn't this also screw up the dimension of the euation when [itex]\vec A_{0 \vec k}[/itex] already has the same dimension as the vector potential since the plane wave solutions are

[tex]\vec A_{0 \vec k}(t) e^{i \vec k \cdot \vec r}?[/tex]
 
Physics news on Phys.org
why we use a 1/V−−√ in the Fourier expansion of the vector potential

It is just a convention. Perhaps you came across it in a book on quantum theory of radiation, where it is sometimes used because it leads to expression of the Poynting energy of the field in the box V in which V does not appear.

If we used the standard convention

[tex] \vec A(\vec r,t) = \sum_{\vec k} \vec A_{0 \vec{k}}(t) e^{i \vec k \cdot \vec r},[/tex]

the integration over volume would introduce the prefactor V in the total Poynting energy.

...Doesn't this also screw up the dimension of the euation when A⃗ 0k⃗ already has the same dimension as the vector potential...

The dimension of [itex]\vec A(\vec r,t)[/itex] stays the same as in the standard convention, but the dimension of [itex]\vec A_{0\vec k}[/itex] is [itex][ A(\vec r,t) ] \mathrm{m}^{3/2}[/itex].
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
1K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 4 ·
Replies
4
Views
4K
  • · Replies 10 ·
Replies
10
Views
4K