Consider the case below. A ray of light travels from a watery medium to air. The light ray will be refracted at the point where the two mediums meet. The refracted light ray bends away from the normal as it passes from a medium of a higher refractive index to one of a lower refractive index. The angle of incidence at which the refraction angle is 90 degrees is called the critical angle. The incident ray will reflect back to the medium when the angle of incidence is larger than the critical angle. This is known as total internal reflection.
When Does Total Internal Reflection Occur?
Consider two lights passing through an optically denser media and into an optically rarer material at specific points.
The refraction of light is the phenomenon that causes light to bend off its normal path. This is a unique situation in which the refracted angle exceeds the incident angle.
The above statement describes how increasing the angle of incidence causes the angle of refraction to increase.
There is still a moment where the refraction angle becomes perpendicular. The refracted light will become parallel to the interface as a result of this.
The refracted ray angle of the rarer medium corresponds to the incident ray angle of the denser medium, which is 90°. This is called the critical angle of total internal reflection (c).
The ray returns to the same medium when it is incident on the surface at an angle larger than the critical angle. Total internal reflection refers to the full process of returning a light beam away from a denser medium. So total internal reflection occurs when the incidence angle is greater than the critical angle.
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Conditions for total internal reflection of light
There are two primary factors that influence whether or not the phenomena of total internal reflection occurs. (TIR) is founded on. A little difference in the two circumstances may not yield the desired effect.
There are two prerequisites for total internal reflection:
Total internal reflection of light formulas:
n1/n2 = sin r/sin i
Critical angle formula
Θcrit= sin-1 (n2/n1)
Here are some examples of total internal reflection:
Total internal reflection in optical fiber
One of the most important applications of total internal reflection is seen in optical fiber. In an optical fiber, the total internal reflection approach is used. The core of the higher refractive index fiber contains the inner component of the fiber. Another layer of glass surrounds all of these fibers. They have a refractive index that is just below that of the lower refractive index. The fibers are protected by a plastic jacket.
When light from one end of the core goes toward the cladding and propagates through it, this is known as back to back total internal reflection. Optical fibers have a lot of uses in the medical field, especially for endoscopy.
Define Acceptance angle:
The acceptance angle of an optical fiber is determined by ray optics is the maximum angle of a ray striking the fiber core (against the fiber axis) that allows incident light to be directed by the core. The numerical aperture is defined as the sine of that permissible angle (assuming an incident ray in air or vacuum) and is mostly governed by the refractive index contrast between the core and cladding of the fiber (assuming an incident ray in air or vacuum):
Acceptance angle formula
n 0 = refractive index of the medium around the fibre
ncore = refractive index of core
ncladding = refractive index of cladding
θacc = acceptance angle
Total internal reflection in diamond: The incident ray is greater than the critical angle when it falls on every face of the diamond. The diamond's critical value is 23°. This situation is responsible for a diamond's entire internal reflection, which causes it to shine.
It's an optical illusion that causes the water layer to appear at short distances in the desert or on the road. Total internal reflection, which happens as a result of atmospheric refraction, is an example of a mirage.