Total internal reflection: Definition from Answers.com

"Critical angle" redirects here. For the aviation term, see Angle of attack.

The larger the angle to the normal, the smaller is the fraction of light transmitted, until the angle when total internal reflection occurs. (The color of the rays is to help distinguish the rays, and is not meant to indicate any color dependence.)

Total internal reflection is an optical phenomenon that occurs when a ray of light strikes a medium boundary at an angle larger than a particular critical angle with respect to the normal to the surface. If the refractive index is lower on the other side of the boundary, no light can pass through and all of the light is reflected. The critical angle is the angle of incidence above which the total internal reflection occurs.

When light crosses a boundary between materials with different refractive indices, the light beam will be partially refracted at the boundary surface, and partially reflected. However, if the angle of incidence is greater (i.e. the ray is closer to being parallel to the boundary) than the critical angle – the angle of incidence at which light is refracted such that it travels along the boundary – then the light will stop crossing the boundary altogether and instead be totally reflected back internally. This can only occur where light travels from a medium with a higher refractive index to one with a lower refractive index. For example, it will occur when passing from glass to air, but not when passing from air to glass.

1 Optical description
2 Critical angle
3 Derivation of evanescent wave
4 Frustrated total internal reflection
5 Phase shift upon total internal reflection
6 Applications
7 Examples in everyday life
8 See also
9 References
10 External links

Optical description

Total internal reflection

Total internal reflection in a block of PMMA

Total internal reflections can be demonstrated using a semi-circular glass block. A "ray box" shines a narrow beam of light (a "ray") onto the glass. The semi-circular shape ensures that a ray pointing towards the centre of the flat face will hit the curved surface at a right angle; this will prevent refraction at the air/glass boundary of the curved surface. At the glass/air boundary of the flat surface, what happens will depend on the angle. Where θ_c is the critical angle (measured normal to the surface):

If θ < θ_c, the ray will split. Some of the ray will reflect off the boundary, and some will refract as it passes through.
If θ > θ_c, the entire ray reflects from the boundary. None passes through. This is called total internal reflection.

This physical property makes optical fibers useful and prismatic binoculars possible. It is also what gives diamonds their distinctive sparkle, as diamond has an extremely high refractive index.

Critical angle

The critical angle is the angle of incidence above which total internal reflection occurs. The angle of incidence is measured with respect to the normal at the refractive boundary. The critical angle $θ c$ is given by:

$\theta_c = \arcsin \left( \frac{n_2}{n_1} \right),$

where $n 2$ is the refractive index of the less optically dense medium, and $n 1$ is the refractive index of the more optically dense medium.

If the incident ray is precisely at the critical angle, the refracted ray is tangent to the boundary at the point of incidence. If for example, visible light were traveling through acrylic glass (with an index of refraction of 1.50) into air (with an index of refraction of 1.00). The calculation would give the critical angle for light from acrylic into air, which is

$\theta _{c}=\arcsin \left( 1.00/1.50 \right)=41.8{}^\circ$ .

Light incident on the border with an angle less than 41.8° would be partially transmitted, while light incident on the border at larger angles with respect to normal would be totally internally reflected.

The critical angle for diamond in air is about 24.4°, which means that light is much more likely to be internally reflected within a diamond. Diamonds for jewelry are cut to take advantage of this; in particular the brilliant cut is designed to achieve high total reflection of light entering the diamond, and high dispersion of the reflected light (known to jewelers as fire).

If the fraction: $\frac{n_2}{n_1}$ is greater than 1, then arcsine is not defined--meaning that total internal reflection does not occur even at very shallow or grazing incident angles.

So the critical angle is only defined when $\frac{n_2}{n_1}$ is less than 1.

Derivation of evanescent wave

Fig. 1

An important side effect of total internal reflection is the propagation of an evanescent wave across the boundary surface. Essentially, even though the entire incident wave is reflected back into the originating medium, there is some penetration into the second medium at the boundary. The evanescent wave appears to travel along the boundary between the two materials, leading to the Goos-Hänchen shift.

If a plane wave, confined to the xz plane, is incident on a dielectric with an angle $θ I$ and wavevector $\mathbf{k_I}$ then a transmitted ray will be created with a corresponding angle of transmittance as shown in Fig. 1. The transmitted wavevector is given by:

$\mathbf{k_T}=k_Tsin(\theta_T)\hat{x}+k_Tcos(\theta_T)\hat{z}$

If $n 1 > n 2$ , then $s i n (θ T) > 1$ since in the relation $sin(\theta_T)=\frac{n_1}{n_2}sin(\theta_I)$ obtained from snell's law, $\frac{n_1}{n_2}sin(\theta_I)$ is greater than one. As a result of this $c o s (θ T)$ becomes complex:

$cos(\theta_T)=\sqrt{1-sin^2(\theta_T)}=i\sqrt{sin^2(\theta_T)-1}$

The electric field of the transmitted plane wave is given by $\mathbf{E_T}=\mathbf{E_0}e^{i(\mathbf{k_T}\cdot\mathbf{r}-\omega t)}$ and so evaluating this further one obtains:

$\mathbf{E_T}=\mathbf{E_0}e^{i(\mathbf{k_T}\cdot\mathbf{r}-\omega t)}=\mathbf{E_0}e^{i(xk_Tsin(\theta_T)+zk_Tcos(\theta_T)-\omega t)}$

$\mathbf{E_T}=\mathbf{E_0}e^{i(xk_Tsin(\theta_T)+zk_Ti\sqrt{sin^2(\theta_T)-1}-\omega t)}$

Using the fact that $k_T=\frac{\omega n_2}{c}$ and snell's law one finally obtains:

$\mathbf{E_T}=\mathbf{E_0}e^{-\kappa z}e^{i(kx-\omega t)}$

where $\kappa=\frac{\omega}{c}\sqrt{(n_1sin(\theta_I))^2-n^2_2}$ and $k=\frac{\omega n_1}{c}sin(\theta_I)$

This wave in the optically denser medium is known as the evanescent wave. Its characterized by its propagation in the x direction and its exponential attenuation in the z direction. Another unique feature of evanescent waves is that on average no energy will be transmitted perpendicular to the face of the medium.

Frustrated total internal reflection

Fingerprints on a glass of water made visible by frustrated total internal reflection

Under "ordinary conditions" it is true that the creation of an evanescent wave does not affect the conservation of energy, i.e. the evanescent wave transmits zero net energy. However, if a third medium with a higher refractive index than the second medium is placed within less than several wavelengths distance from the interface between the first medium and the second medium, the evanescent wave will be different from the one under "ordinary conditions" and it will pass energy across the second into the third medium. (See evanescent wave coupling.)

A transparent, low refractive index material is sandwiched between two prisms of another material. This allows the beam to "tunnel" through from one prism to the next in a process very similar to quantum tunneling while at the same time altering the direction of the incoming ray.

Phase shift upon total internal reflection

An additional less known aspect of total internal reflection is that the reflected light has an angle dependent phase shift between the reflected and incident light. Mathematically this means that the Fresnel reflection coefficient becomes a complex rather than a real number. This phase shift is polarization dependent and grows as the incidence angle deviates further from the critical angle toward grazing incidence.

The polarization dependent phase shift is long known and was used by Fresnel to design the Fresnel rhomb which allows to transform circular polarization to linear polarization and vice versa for a wide range of wavelengths (colors), in contrast to the quarter wave plate. The polarization dependent phase shift is also the reason why TE and TM guided modes have different dispersion relations.

Applications

Optical fibers, which are used in endoscopes and telecommunications.
Rain sensors to control automatic windscreen/windshield wipers.
Another interesting application of total internal reflection is the spatial filtering of light.^[1]
Prismatic binoculars use the principal of Total internal reflections to get a very clear image
Multi-touch screens [1] use frustrated total internal reflection in combination with a camera and appropriate software to pick up multiple targets.
Gonioscopy to view the anatomical angle formed between the eye's cornea and iris.
Gait analysis instrument, CatWalk [2], uses frustrated total internal reflection in combination with a high speed camera to capture and analyze footprints of laboratory rodents.
Fingerprinting devices, which use frustrated total internal reflection in order to record an image of a person's fingerprint without the use of ink.

Examples in everyday life

Total internal reflection of the turtle can be seen at the air-water boundary.

Total internal reflection can be observed while swimming, if one opens one's eyes just under the water's surface. If the water is calm, its surface appears mirror-like.

One can demonstrate total internal reflection by filling a sink or bath with water, taking a glass tumbler, and placing it upside-down over the plug hole (with the tumbler completely filled with water). While water remains both in the upturned tumbler and in the sink surrounding it, the plug hole and plug are visible since the angle of refraction between glass and water is not greater than the critical angle. If the drain is opened and the tumbler is kept in position over the hole, the water in the tumbler drains out leaving the glass filled with air, and this then acts as the plug. Viewing this from above, the tumbler now appears mirrored because light reflects off the air/glass interface.

Another very common example of total internal reflection is a critically cut diamond. This is what gives it maximum sparkle.

References

^ Moreno, Ivan; J. Jesus Araiza, Maximino Avendano-Alejo (2005). "Thin-film spatial filters" (PDF). Optics Letters 30 (8): pp. 914–916. doi:10.1364/OL.30.000914. http://planck.reduaz.mx/~imoreno/Publicaciones/OptLett2005.pdf.

This article incorporates public domain material from the General Services Administration document "Federal Standard 1037C" (in support of MIL-STD-188).

External links

Wikimedia Commons has media related to: Total internal reflection

FTIR Touch Sensing
Multi-Touch Interaction Research
iBar Intelligent Surface System
http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/totint.html
Total Internal Reflection by Michael Schreiber, Wolfram Demonstrations Project
Total Internal Reflection - St. Mary's Physics Online Notes

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