PRISM:
A prism is a transparent medium separated from the surrounding medium by at least two plane surfaces which are inclined at a certain angle in such a way that, light incident on one of the plane surfaces emerges from the other plane surface.
Consider a triangular glass prism. It contains two triangular bases and three rectangular plane lateral surfaces. These lateral surfaces are inclined to each other. Let us consider that triangle PQR represents outline of the prism where it rests on its triangular base.
Let us assume that a light ray is incident on the plane surface PQ of a prism at M as shown in figure. Draw a perpendicular to the surface at M. It becomes a normal to that surface. The angle between the incident ray and normal is called angle of incidence (i1). The ray is refracted at M. It moves through prism and meets the other plane surface at N and finally comes out of the prism. The ray which comes out of the surface PR at N is called emergent ray. Draw a perpendicular to PR at point N. The angle between the emergent ray and normal is called angle of emergence (i2 ).The angle between the plane surfaces PQ and PR is called the angle of the prism or refracting angle of prism A and the angle between the incident ray and emergent ray is called angle of deviation(d).
It is a triangle. Name its vertices as P, Q, and R.[for many prisms the triangle formed is equilateral]. The refracting surfaces could be rectangular in shape. Find the angle between PQ and PR . This is the angle of the prism (A). Mark M on the side of triangle PQ and also draw a perpendicular to PQ at M. Place the centre of the protractor at M and along the normal. Mark an angle of 300 and then draw a line up to M. This line denotes the incident ray. This angle is called angle of incidence. Note it in a table
Now join the
points M and N by a straight line. The line passing through the points A, B, M,
N, C and D represents the path of light when it suffers refraction through the
prism. Extend both incident and emergent rays till they meet at a point ‘O’. Measure
the angle between these two rays. This is the angle of deviation. It is denoted
by a letter- ‘d’. Note it in table. Repeat this procedure for various angles of
incidence such as 400,500 etc. Find the corresponding angles
of deviation and angles of emergence and note them in table.
You will notice
that the angle of deviation decreases first and then increases with increase in
the angle of incidence.
Now try to plot a graph
Take angle of
incidence along X- axis and the angle of deviation along Y- axis. Using a
suitable scale, mark points on a graph paper for every pair of angles. Finally
join the points to obtain a graph (smooth curve).
Draw a tangent
line to the curve, parallel to X- axis, at the lowest point of the graph. The
point where this line cuts the Y- axis gives the angle of minimum deviation. It
is denoted by D. Draw a parallel line to y-axis through the point where the
tangent touches the graph. This line meets x-axis at a point showing the angle
of incidence corresponding to the minimum deviation. If you do the experiment
with this angle of incidence you will get an angle of emergence equal to the
angle of incidence.
Derivation
of formula for refractive index of a prism
From triangle OMN,
we get
d = i1-
r1 + i2 – r2
d = (i1+i2)
– (r1+r2) ––—— (1)
From triangle PMN,
we have
A + (900-r1)
+ (900-r2) = 1800
By simplification,
we get
r1 + r2
= A ———(2)
From (1) and (2),
we have
d = (i1+i2)
– A
A+d = i1+i2
––——(3)
This is the
relation between angle of
incidence, angle
of emergence, angle of deviation and angle of prism.
From Snell’s law,
we know that n1 sin i =
n2 sin r
Let n be the
refractive index of the prism.
Using Snell’s law
at M, with refractive index of air
n1 =1;
i = i1 ; n2 = n ; r = r1 , gives
sin i1
= n sin r1 ———(4)
similarly, at N
with n1 = n ; i = r2 ; n2 = 1 ; r = i2
, gives
n Sin r2
= Sin i2 ———(5)
We know that at
the angle of minimum deviation (D), the angle of incidence is equal to the
angle of emergence i.e., i1 = i2.
You will note that
MN is parallel to the side QR, actually ray MN is parallel to the base of the
prism.
When i1
= i2, angle of deviation (d) becomes angle of minimum deviation (D).
Then equation (3)
becomes
A+D = 2i1
or i1 =
(A+D)/2
When i1
= i2 then, it is clear that r1 = r2
So from equation
(2) we get,
2r1 = A
or r1 =
A/2
Substituting i1
and r1 in (4) we get
Sin{(A+D)/2)} = n.
Sin(A/2)
n = Sin(A+D/2)/Sin(A/2) |
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