Transcript File

by
Bhaskar
Department of Physics
K L University
Lecture 07 (25 Aug)
Interference in Thin Films
Newton Rings
• Another method for viewing interference is to
place a planoconvex lens (L) on top of a flat
glass (G) surface.
• The air film between the glass surfaces varies
in thickness from zero at the point of contact
to some thickness “d”.
• A pattern of light and dark rings is observed.
These rings are called Newton’s Rings.
• Newton’s Rings can be used to test optical
lenses.
Newton Rings…..
Newton Rings…
• Ray 1 undergoes a phase change of 180 on
reflection, whereas Ray 2 undergoes no
phase change
R= radius of curvature of lens
r=radius of Newton’s ring
Newton Rings…
How are these rings are formed?
Let us consider a particular point
which is at a distance of r from the
point of contact of the lens with the
glass plate.
All points having the same
thickness – Destructive
Interference.
Why are they circular?
The locus of all the points from a circular dark ring with ‘r’ as
radius.
Centre is dark because of phase change during reflection at
glass plate.
Newton Rings…
 For constructive
interference
 For destructive
interference
Newton Rings…..
Conclusion: Fringe width decreases with the order of
the fringe and fringes get closer with increases in
their order.
D16 -D9=2√Rλ ------------->7 Fringes
D9-D4 = 2√Rλ -------------->5 fringes
D4-D1= 2√Rλ ---------------->3 Fringes
Newton Rings…..
Out Comes:

Determination of wavelength of
monochromatic source.
 Determination of refractive index of liquid.
Determination of wavelength of monochromatic
source:
Measure the radii or diameter of rings formed
Measure the radius of curvature of the lens (R).
R = l²/6h+h/2
Where l is the distance between
two legs of spherometer. h is height of
convex lens.
Dn , Dm are the diameters of the mth and nth
dark rings
Dn2 – Dm2
λ=
4 𝑚−𝑛 𝑅
D2
D 2 vs m
m
Spherometer
Newton Rings…
Determination of refractive index of liquid:
Liquid
Determination of refractive index ( µ ) of liquid
lens
glass plate
2
Dn –
Dm2
lens
air
= 4(m-n) λ R
liquid
glass plate
D1n2
–
D1n2 – D2m2
µ=
Dn2 –Dm2
D2m2=
4(m−n) λ R
µ
Newton Rings…
For a air film between the plane convex lens and a flat
glass
• For a liquid medium (whose refractive index is to be
measured) between the plane convex lens and a flat
glass
• Resultantly the RI of
liquid medium can be written as
Primary Application's of Interferometer
1) Optical Testing : Surface Quality
a) Flat Surfaces
b) Spherical Surfaces
c) Surface roughness
2) Direct phase measurements
a) phase shifting
b) phase stepping
3) Aligning very high quality lenses
4) Space applications
a) Radio Astronomy
b) Measuring light intensity
c) used in retrieving images from telescope
Newton Rings… In white light
light :a wave leading to our future
The end
Problems
1) In Newton’s ring experiment , the diameter of the 10th dark ring
is 0.433cm . Find the wavelength of incident light, if the radius of
curvature of the lens is 70cm .
2) In Newton’s ring experiment , the diameter of the 5th dark ring
was 0.3 cm and the diameter of 25th ring was 0.8 cm. If the
radius of curvature of the plano convex lens is 100cm. Find the
wavelength of light used.