Title: Newton
1Newtons Rings
2A
B
Plano convex lens
Air film
Q
P
O
Glass plate
Thickness of air film is zero at point of contact
O.
3Reflected light
L
Air film
G
Circular interference fringes are formed by
reflected light
4Microscope
45º
S
glass
L
Lens
Air film
Glass plate
5Interference occurs between the light reflected
from the lower surface of the lens and the
upper surface of the glass plate G.
Since the convex side of the lens is a spherical
surface, the thickness of the air film will
be cons- tant over a circle (whose centre will be
at O ) and we will obtain concentric dark and
bright rings.
Newtons rings
6It should be pointed out that in order to observe
the fringes the microscope has to be focused on
the Surface of the film.
Each ring will be locus of all such points where
thickness is same.
7Condition for bright ring will be
For air film , ? 1 and for near normal
incidence r is very small and hence cos r 1
Thus,
Where n 0,1,2,3.
8For dark rings,
Again for air film ? 1 and for small r we
have Condition for dark rings,
9O
R
R - tn
A
B
tn
tn
M
N
rn
10R radius of curvature of lens t thickness of
air film at a distance AB rn OA R - t
- From ?OAB
- R2 (R t)2rn2
- rn2 R2 - (R t)2 R2 - R2 t2 2Rt 2Rt t2
- As Rgtgtt , rn2 2Rt
- ? t rn2/2R
11So condition for bright rings 2t
(2n1)?/2
n 0,1,2,3,.
12Similarly for dark rings,
n 0,1,2,3,.
Diameter of dark rings,
13CENTER IS DARK
At n 0, radius of dark ring 0.
radius of bright ring
Alternately dark and bright rings will be
produced.
The spacing between second and third dark
rings is smaller than the spacing between the
first and second one.
14Consider the diameter of dark rings
Four fringes
15Fringe width decreases with the order of
the Fringe and fringes get closer with increase
in their order.
16Wavelength determination
Radius of the nth dark ring rn is given by
Similarly for (nm)th dark band
17(2) (1)
18Suppose diameter of 6th and 16th ring
are Determined then, m 16-6 10
So
Radius of curvature can be accurately
measured with the help of a spherometer and
therefore by measuring the diameter of dark or
bright ring you can experimentally determine the
wavelength.
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20Newtons rings with transmitted light
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22Transmitted light
23Condition for bright fringes
Condition for dark fringes
For air as thin film and near normal incidence
? 1 and cosr 1
So for bright fringes, 2t n?
For dark fringes,
24But we know that
, r radius of ring
For bright rings
For dark rings
25If we put n 0 then r 0 for the bright ring
So for Newton's rings for transmitted rays the
central ring will be bright.
CENTRAL RING IS BRIGHT.
26WAVELENGTH DETERMINATION
We know radius of the nth dark ring rn is
.(1)
27Similarly,
..(2)
(2) (1)
..(3)
28Suppose diameter of the 8th and 18th ring
are Determined then, m 18-8 10 and
29Refractive index determination
air
Diameter of the dark rings
30?
Liquid of refractive index ?
31(for near normal incidence and ?glt?
Condition for dark ring formation
..(4)
32Similarly we can get
.(5)
(5) (4)
So,
.(6)
This is the value of ? if ? is known.
33? Can also be determine if ? is unknown
We have from equation (3) and (6)
..(3)
.(6)
34Divide (3)/(6)