Understanding the construction of vector spherical wave functions

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SUMMARY

This discussion focuses on the construction of vector spherical wave functions in the context of electromagnetic scattering. The vector Helmholtz equation yields three independent vector solutions, labeled L, M, and N. However, in the final expressions for wavefunctions, only M and N are utilized, as the electromagnetic field is solenoidal, meaning the divergence of the electromagnetic field vanishes. The reference for further understanding is "Electromagnetic Theory" by J.A. Stratton.

PREREQUISITES
  • Understanding of vector Helmholtz equation
  • Familiarity with electromagnetic scattering concepts
  • Knowledge of solenoidal functions
  • Basic principles of vector calculus
NEXT STEPS
  • Study the properties of vector functions L, M, and N in detail
  • Explore the implications of solenoidal fields in electromagnetic theory
  • Read "Electromagnetic Theory" by J.A. Stratton for comprehensive insights
  • Investigate the application of multipole fields in practical electromagnetic scattering scenarios
USEFUL FOR

Researchers and students in physics, particularly those focusing on electromagnetic theory and scattering, as well as engineers working with electromagnetic field applications.

dave86wave
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Understanding the construction of vector spherical wave functions!

Hi guys,

I'm looking at electromagnetic scattering just now, and in particular, how multipole fields are constructed and then how the wavefunctions are represented as the incident, internal and scattered fields. When you satisfy the vector Helmholtz equation, you get three independent vector solutions to it, typically described as L, M, and N. However, when you get to the final expressions for wavefunctions, they are described in terms of multipole fields M and N. What does happen to L and what does it represent? I'll appreciate any feedback on this strange question. Thanks.
 
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dave86wave said:
Hi guys,

I'm looking at electromagnetic scattering just now, and in particular, how multipole fields are constructed and then how the wavefunctions are represented as the incident, internal and scattered fields. When you satisfy the vector Helmholtz equation, you get three independent vector solutions to it, typically described as L, M, and N. However, when you get to the final expressions for wavefunctions, they are described in terms of multipole fields M and N. What does happen to L and what does it represent?

Peace!M and N are used for the representation of purely solenoidal functions or in other words when the given function is purely solenoidal , the expansion is made in terms of M and N alone.
And if the divergence of the function does not vanish terms in L must be included.

when we are dealing with EM field and we know that divergence of EM vanishes so we can't write EM field in term of L. And we also know that EM field is solenoidal, that why we represent in terms of M and N

The vector functions L, M, and N have certain notable properties that follow directly from their definitions.
Curl of L = 0
divegence of M =0
divegence of N =0 For the construction of these functions you can check Electromagnetic Theory By J.A. Stratton
Reference : Electromagnetic Theory By J.A. Stratton

I'll appreciate any feedback on this strange question. Thanks.

Its not strange for me at all. :DPeace!
 
Last edited:

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