How is the spin force related to electromagnetic wave curl and vector calculus?

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SUMMARY

The spin force in electromagnetic wave theory can be expressed as F_{spin}=\frac{-1}{2}Im(\alpha)Im(E\cdot\nabla E^{*})=\nabla\times L_s, where \alpha is a complex quantity and E is the electric field vector. The discussion highlights the use of the imaginary part of complex numbers and the curl operation in vector calculus to derive the spin force. The identity for the curl of a cross product is also referenced to facilitate understanding of the relationship between the spin force and the vector L_s. The challenge lies in correctly interpreting the conjugation of the term E\cdot\nabla E^{*}.

PREREQUISITES
  • Understanding of vector calculus, specifically curl and gradient operations.
  • Familiarity with complex numbers and their properties, including imaginary parts.
  • Knowledge of electromagnetic wave theory, particularly the role of the electric field vector E.
  • Ability to manipulate vector identities in mathematical expressions.
NEXT STEPS
  • Study the properties of complex numbers, focusing on imaginary components and conjugation.
  • Learn about vector calculus identities, particularly the curl of vector fields.
  • Explore electromagnetic wave theory, emphasizing the significance of the electric field vector E.
  • Investigate the mathematical derivation of the spin force in electromagnetic contexts.
USEFUL FOR

Students and professionals in physics and engineering, particularly those studying electromagnetism, vector calculus, and mathematical physics. This discussion is beneficial for anyone seeking to understand the mathematical foundations of spin forces in electromagnetic waves.

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Homework Statement


I put this in the math forum because although it's for my EM waves class, it's a math question.

Show that the spin force can be written as:

F_{spin}=\frac{-1}{2}Im(\alpha)Im(E\cdot\nabla E^{*})=\nabla\times L_s

Find L_s.

Where \alpha is complex. I'm using E^{*} to denote the complex conjugate of E. Also, since these are all vectors, I'm omitting the arrow notation atop the vector quantities.

Homework Equations



Im(z)=\frac{1}{2i}(z-z^{*})

The Attempt at a Solution



From the relevant equations:
Im(\alpha)=\frac{1}{2i}[\alpha-\alpha^{*}]
Im(E\cdot\nabla E^{*})=\frac{1}{2i}[E\cdot\nabla E^{*}-(E\cdot\nabla E^{*})^{*}]

Substituting in,
F_{spin}=\frac{1}{8}[\alpha-\alpha^{*}][E\cdot\nabla E^{*}-(E\cdot\nabla E^{*})^{*}]=\nabla\times L_s

Here, in order to make a curl appear, I'd like to apply the identity:
\nabla\times(A\times B)=A(\nabla\cdot B)-B(\nabla\cdot A)+(B\cdot\nabla)A-(A\cdot\nabla)B

However, I'm not sure what the quantity [(E\cdot\nabla E^{*})^{*}] looks like... I don't know how to conjugate this and I'm stuck here for the moment.
 
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If E is a vector then I'm not sure what ∇E means. ∇.E would be a scalar, making E.(∇.E) problematic. Do you mean ∇×E?
 
E is the electric field vector. it is a function of position and time, so that's just its gradient vector, also a function of position and time.
 
jtleafs33 said:
E is the electric field vector. it is a function of position and time, so that's just its gradient vector, also a function of position and time.
If you have a scalar field f, then ∇f = grad f is the gradient vector. But here you say E is a vector, so I'm at a loss to understand what ∇E represents. See item e) at http://www.math.ucla.edu/~ronmiech/Calculus_Problems/32B/chap14/section5/930d31/930_31.html
 

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