Field form in the optic fibers from Maxwell's equations

In summary, Emily is looking for information on the solution of Maxwell's equations in cylindrical coordinates for an optic fiber with a step-index variation in the core and cladding. There is a discussion about the choice of sine or cosine variation for the electric and magnetic fields, and how it affects the continuity of the tangential components at the core/cladding boundary. She is also wondering if there are any textbooks or online resources that provide similar computations and derivations for this topic.
  • #1
EmilyRuck
136
6
Hello!
In this document a solution of Maxwell's equations in cylindrical coordinates is provided, in order to determine the electric and magnetic fields inside an optic fiber with a step-index variation. The interface between core and cladding is the cylindrical surface [itex]r = a[/itex].
For example, the most general solution (pp. 18-19) for [itex]E_z[/itex] is

[itex]E_z (r, \phi) = \Phi(\phi) R(r) = \left[ K_1 \cos (\nu \phi) + K_2 \sin (\nu \phi) \right] \left[ A J_{\nu}(k_c r) + CY_{\nu}(k_c r) \right][/itex]

In page 21 (17.70) though, just the sine variation is kept, putting (I think, arbitrarily) [itex]K_1 = 0[/itex] and [itex]K_2 = 1[/itex].

- Why should [itex]K_2[/itex] equal unity while [itex]A[/itex] is left unchanged?
- Is this a standard choice? Why is the cosine variation excluded? Is this just for convenience, or the contemporary presence of sine and cosine variation with respect to [itex]\phi[/itex] in both electric and magnatic fields can violate the continuity of the tangential components across the surface [itex]r = a[/itex]?

Moreover, in page 22 it is pointed out that:

« In this case, where we have assumed the [itex]sin(\nu \phi)[/itex] for the electric field, we must have the [itex]cos(\nu \phi)[/itex] variation for the [itex]H_z[/itex] field to allow matching of the tangential fields (which include both [itex]z[/itex] and [itex]\phi[/itex] components) at the core/cladding boundary ».

- How can this be proved?
 
  • #3
Greg Bernhardt said:
Do you have any further information, come to any new conclusions or is it possible to reword the post?

Not new conclusions, but: is there a textbook where similar computations are showed? Or another pdf from the web, with the same subject matter?
I need the derivation of the longitudinal fields for a step-index optic fiber, with the considerations about the choice of the [itex](r,\phi)[/itex] dependence: when [itex]\sin (\nu \phi)[/itex] is to be chosen, or the [itex]\cos (\nu \phi)[/itex], etc.
Even if you can't suggest the proofs I'm looking for, could you provide some (maybe) useful link?
Thank you anyway,

Emily
 

Related to Field form in the optic fibers from Maxwell's equations

1. What are Maxwell's equations?

Maxwell's equations are a set of fundamental equations that describe the behavior of electromagnetic fields. They were first derived by James Clerk Maxwell in the 19th century and have been widely accepted as the basis for understanding electromagnetism.

2. How do Maxwell's equations apply to optic fibers?

Optic fibers are thin, transparent fibers made of glass or plastic that are used to transmit light signals. Maxwell's equations apply to optic fibers because they describe the behavior of electromagnetic fields, which includes light.

3. What is field form in the context of optic fibers and Maxwell's equations?

Field form refers to the specific arrangement and behavior of electromagnetic fields in optic fibers, as described by Maxwell's equations. This includes the direction, intensity, and polarization of the fields.

4. How do Maxwell's equations influence the design of optic fibers?

Maxwell's equations are essential for designing optic fibers that can effectively transmit light signals. They dictate the properties and dimensions of the fibers, such as the refractive index and core diameter, to ensure efficient transmission of light.

5. What are some practical applications of understanding field form in optic fibers from Maxwell's equations?

Understanding the field form in optic fibers from Maxwell's equations has numerous practical applications, including the development of high-speed communication systems, fiber optic sensors, and medical imaging devices. It also allows for the optimization of optic fiber designs for various purposes.

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