Total internal reflection is an optical phenomenon that occurs when a ray of light strikes a medium boundary at an angle larger than the 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, so effectively 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.
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 θc is the critical angle (measured normal to the surface):
This physical property makes optical fibers useful, and rainbows and prismatic binoculars possible. It is also what gives diamonds their distinctive sparkle, as diamond has an extremely high refractive index.
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 from a glass (i.e. Lucite 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 Lucite into air, which is
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: 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 for .
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.
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.
Wipo Publishes Patent of Hamamatsu Photonics K.K. for "Total Reflection Spectroscopic Measurement Method" (Japanese Inventors)
Oct 04, 2012; GENEVA, Oct. 4 -- Publication No. WO/2012/128001 was published on Sept. 27. Title of the invention: "TOTAL REFLECTION...
US Patent Issued to JASCO on Sept. 10 for "Microscopic Total Reflection Measuring Apparatus" (Japanese Inventors)
Sep 10, 2013; ALEXANDRIA, Va., Sept. 10 -- United States Patent no. 8,531,674, issued on Sept. 10, was assigned to JASCO Corp. (Hachioji-shi,...
US Patent Issued to FUJIFILM on July 2 for "Total Reflection Illuminated Sensor Chip, Method for Producing the Total Reflection Illuminated Sensor Chip, and Sensing Method Using the Total Reflection Illuminated Sensor Chip" (Japanese Inventor)
Jul 02, 2013; ALEXANDRIA, Va., July 2 -- United States Patent no. 8,477,312, issued on July 2, was assigned to FUJIFILM Corp. (TokyoTotal...
US Patent Issued to Hamamatsu Photonics on April 9 for "Total Reflection Terahertz Wave Measurement Device" (Japanese Inventors)
Apr 12, 2013; ALEXANDRIA, Va., April 12 -- United States Patent no. 8,415,625, issued on April 9, was assigned to Hamamatsu Photonics K.K....
WIPO PUBLISHES PATENT OF PHOTONICS PLANAR INTEGRATION TECHNOLOGY FOR "TOTAL REFLECTION TYPE OPTICAL SWITCH USING POLYMER INSERTION TYPE SILICA OPTICAL WAVEGUIDE AND MANUFACTURING METHOD THEREOF" (SOUTH KOREAN INVENTORS)
May 17, 2012; GENEVA, May 17 -- Publication No. WO/2012/060567 was published on May 10. Title of the invention: "TOTAL REFLECTION TYPE OPTICAL...