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21.2.2. Laws of Geometric Optics<br />

sin e = n 2<br />

( - n 1<br />

(21.4)<br />

Law of Reflection: When a ray of light is reflected from a plane<br />

surface, the incident ray and the reflected ray all lie in the same<br />

plane; the angle of reflection equals the angle of incidence:<br />

i=r<br />

(21.1)<br />

Law of Refraction: When a ray of light passes from one medium<br />

to another, the incident ray, the reflected ray, and the refracted ray<br />

all lie in the same plane; the sine of the angle of incidence bears a<br />

constant ratio to the sine of the angle of refraction:<br />

sin i / sin r = n<br />

( 21.2 )<br />

t<br />

where n I is greater than n2"<br />

2 1<br />

n 2<br />

Fig. 21.4. Total internal reflection<br />

For angles of incidence<br />

greater than i,<br />

the beam is entirely reflected<br />

at the boundary. In<br />

such a way, total internal<br />

reflection occurs only<br />

when light attempts to move<br />

from a medium ofgiven<br />

index of refraction to<br />

a medium of lower index<br />

of refraction.<br />

The ratio sin i / sin r is known as the refractive index from one<br />

medium to another. It is convenient to define the refractive index<br />

of a medium to be the ratio:<br />

c<br />

n=­<br />

V<br />

(21.3 )<br />

where c is the speed of light in a vacuum and, V ­ the speed of<br />

light in a medium.<br />

Here are refraction index values for several common materials<br />

are: air = 1.0003, water = 1.33, glass = 1.52, diamond = 2.42,<br />

lead sulfide = 3.91.<br />

21.2.3. Total Internal Reflection<br />

An interesting effect, called total internal reflection, can occur<br />

when light attempts to move from a medium having given index<br />

of refraction (n) to one having a lower index of refraction (n)<br />

(fig. 21.4). All possible directions of the beam are indicated by rays<br />

1 through 5. At some particular angle of incidence, (i), called<br />

the critical angle, the refracted light ray will move parallel to the<br />

boundary. The value of the critical angle (8) can be found from<br />

the following expression:<br />

142<br />

, ;~<br />

,<br />

Example. Find the critical angle for a water-air boundary (a view from<br />

the fish's eye) if the index of refraction of water is \.33.<br />

Solution. Applying the equation (2\.4), we find the critical angle<br />

to be sine 0= n 1 =_1_ =0 752<br />

c n, 1.33 .<br />

Optical fibers are devices that can be used for transporting<br />

radiation from the source to the sample (e.g., a biological tissue)<br />

for diagnostics, therapy, or surgery. An optical fiber consists of a<br />

long, thin and flexible rod of transparent material. The principle<br />

of the operation of a fiber is based on total internal reflection<br />

that depends on the angle of incidence of the light ray and the<br />

refractive index of the fiber (fig. 21.5). Usually, each fiber consists<br />

three parts: the core at the centre of the fiber; a concentric<br />

Cladding<br />

8 c<br />

= 48.8"<br />

21.2.4. Fiber Optics<br />

... --~--<br />

-----­<br />

Fig. 21.5. Principle<br />

of operation of fiber<br />

143

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