Why aren't other electromagnetic waves used in optical fibres instead of visible light?
Is it because the wavelength of light fits the internal reflection/refractive index of the material used for the fibre? e.g. Is the material that refracts light cheaper compared to material that refracts EM waves with other wavelengths?
[Physics] Why is visible light used in Optical fibers (instead of other EM waves)
electromagnetismoptics
Related Solutions
Refractive index describes the speed of propagation of light in a medium. So to restate your question:
why is the speed of light slower in some media than in others?
The wave equation tells us that speed of propagation depends on two factors: one is an inertial term, while the other is an elastic term. Let's look at a simple case of a string. The velocity of wave propagation in a string goes as
$$v = \sqrt\frac{T}{\mu}$$ where $T$ is the tension, and $\mu$ is the mass per unit length.
When light propagates in a dielectric medium, the electrons in that medium are moved by the EM field of the light. These moving electrons in turn emit an electromagnetic wave, but this wave will be lagging in phase with the signal that caused their motion.
Because of this phase lag, the combined signal that propagates is the sum of the initial signal (now a bit smaller because it gave some of its energy to the electron) plus the phase-shifted signal from the electron. Together, they create a phase shift in the original signal - it is as though it is going slower.
The shift due to one electron is tiny; but the more electrons you have per unit volume, the greater the effect will be. The actual force with which the electrons are bound (the "elastic constant" if you like) also comes into play, so you can't simply say that refractive index scales with density - but for similar materials, it does; the following graph (from http://upload.wikimedia.org/wikipedia/en/3/3b/Density-nd.GIF) shows that similar materials with different densities have a pretty believable relationship between density and refractive index:
The wikipedia page on refractive index contains some more information on the topic...
Suppose we define the following $\zeta = \ln{\varepsilon}$ and $\xi = \ln{\mu}$, where $\varepsilon$ and $\mu$ are the permittivity and permeability, respectively. In a system with no sources (i.e., $\mathbf{j} = 0$ and $\rho_{c} = 0$), then we know that $\nabla \cdot \mathbf{D} = 0$, where $\mathbf{D} = \varepsilon \ \mathbf{E}$ and $\mathbf{B} = \mu \ \mathbf{H}$. After a little vector calculus we can show that: $$ \nabla \cdot \mathbf{E} = - \nabla \zeta \cdot \mathbf{E} \tag{0} $$ Using this and some manipulation of Faraday's law and Ampêre's law, we can show that the general differential equation in terms of electric fields only is given by: $$ \left( \mu \varepsilon \frac{ \partial^{2} }{ \partial t^{2} } - \nabla^{2} \right) \mathbf{E} = \left( \mathbf{E} \cdot \nabla \right) \nabla \zeta + \left( \nabla \zeta \cdot \nabla \right) \mathbf{E} + \nabla \left( \zeta + \xi \right) \times \left( \nabla \times \mathbf{E} \right) \tag{1} $$
We can get a tiny amount of reprieve from this by assuming that the permeability is that of free space, i.e., $\nabla \xi = 0$. If we further argue that the only direction in which gradients matter is along $\hat{x}$ and that the incident wave vector, $\mathbf{k}$, is parallel to this, then we can further simplify Equation 1 to: $$ \left( \mu_{o} \varepsilon \frac{ \partial^{2} }{ \partial t^{2} } - \frac{ \partial^{2} }{ \partial x^{2} } \right) \mathbf{E} = \left( \mathbf{E} \cdot \nabla \right) \zeta' \hat{x} + \left( \zeta' \frac{ \partial }{ \partial x } \right) \mathbf{E} + \zeta' \hat{x} \times \left( \nabla \times \mathbf{E} \right) \tag{2} $$ where $\zeta' = \tfrac{ \partial \zeta }{ \partial x }$.
After some more manipulation, we can break this up into components to show that: $$ \begin{align} \text{x : } \left( \mu_{o} \varepsilon \frac{ \partial^{2} }{ \partial t^{2} } - \frac{ \partial^{2} }{ \partial x^{2} } \right) E_{x} & = E_{x} \zeta'' + \zeta' \frac{ \partial E_{x} }{ \partial x } \tag{2a} \\ \text{y : } \left( \mu_{o} \varepsilon \frac{ \partial^{2} }{ \partial t^{2} } - \frac{ \partial^{2} }{ \partial x^{2} } \right) E_{y} & = 0 \tag{2b} \\ \text{z : } \left( \mu_{o} \varepsilon \frac{ \partial^{2} }{ \partial t^{2} } - \frac{ \partial^{2} }{ \partial x^{2} } \right) E_{z} & = 0 \tag{2c} \end{align} $$
In the limit where the incident wave is entirely transverse, then $E_{x} = 0$ and the x-component (Equation 2a) is entirely zero.
Next you assume that $\mathbf{E} = \mathbf{E}_{o}\left( x \right) e^{i \omega t}$, where $\omega$ is the frequency of the incident wave. Then there will be incident, reflected, and transmitted contributions to the total field at any given point (well the transmitted is always zero in the first medium, of course). Any incident and transmitted contributions with have $\mathbf{k} \cdot \mathbf{x} > 0$ while reflected waves will satisfy $\mathbf{k} \cdot \mathbf{x} < 0$. You define the ratio of the reflected-to-incident fields (well impedances would be more appropriate) to get the coefficient of reflection.
Simpler Approach
A much simpler approach is to know where to look for the answer to these types of questions. As I mentioned in the comments, there has been a ton of work on this very topic (i.e., spatially dependent index of refraction) done for the ionosphere. If we look at, for instance, Roettger [1980] we find a nice, convenient equation for the reflection coefficient, $R$, as a function of the index of refraction, given by:
$$
R = \int \ dx \ \frac{ 1 }{ 2 \ n\left( x \right) } \frac{ \partial n\left( x \right) }{ \partial x } \ e^{-i \ k \ x} \tag{3}
$$
There is no analytical expression for $R$ for your specific index of refraction. However, numerical integration is not difficult if one knows the values for $d$ and $\epsilon$. Note that if we do a Taylor expansion for small $\epsilon$, then the integrand (not including the exponential) is proportional to cosine, to first order in $\epsilon$ (cosine times sine if we go to second order).
References
- Gossard, E.E. "Refractive index variance and its height distribution in different air masses," Radio Sci. 12(1), pp. 89-105, doi:10.1029/RS012i001p00089, 1977.
- Roettger, J. "Reflection and scattering of VHF radar signals from atmospheric refractivity structures," Radio Sci. 15(2), pp. 259-276, doi:10.1029/RS015i002p00259, 1980.
- Roettger, J. and C.H. Liu "Partial reflection and scattering of VHF radar signals from the clear atmosphere," Geophys. Res. Lett. 5(5), pp. 357-360, doi:10.1029/GL005i005p00357, 1978.
Best Answer
Almost all fibers (and certainly all telecomms fibers) do not use visible light but infrared light. A typical wavelength used is 1550 nm. At this wavelength the combined effects of absorption and (Rayleigh) scattering in the fiber attains a minimum value, thereby allowing long transmission distances.