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Transcript of uday phy gd
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Submitted by-Sidharth sharma
Uday pratap
Vaibhav kaushal
Vikashdeep sagar
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IntroductionRelated theoryObjectiveImportant terms
Formula usedDescription of apparatusProceduresMeasurements
ObservationsResultsPrecautions
CONTENTS
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INTRODUCTION Sodium lights actually energize
the sodium gas trapped insidethe bulb to produce the light.
Wavelength is the distancebetween peaks (high points).
This is similar to Youngs
experiment.
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RELATED THEORY
The wave nature of light was established in the early part ofthe 19th century.
Fresnels experiment with the Biprism was one of the earliest
experiments to yield values for the wavelength of light. To make two coherent source for interference .Biprism make
two sources.
It is similar to Youngs Double slit experiment .
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IMPORTANT TERMS
FresnelsBiprismYoungs
Double SlitExperiment
Interferenceof light Diffraction
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FRESNEL BIPRISM
Fresnel used a biprism to showthe phenomenon of interference.
A biprism is essentially a
combination of two acute prismplaced base to base.
A prism whose refracting angle
is very nearly 180 degrees. to determine wavelengths and
interference fringes
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Youngs Double SlitExperiment In the early 1800's (1801 to 1805), Thomas
Young conducted an experiment. He allowed
light to pass through a slit in a barrier so it
expanded out in wave fronts from that slit as a
light source.
That light, in turn, passed through a pair of slits
in another barrier (carefully placed the right
distance from the original slit). Each slit, in turn,
diffracted the light as if they were also individual
sources of light. The light impacted an
observation screen.
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When a single slit was open, it merelyimpacted the observation screen with
greater intensity at the center and thenfaded as you moved away from the center.There are two possible results of thisexperiment:
Particle interpretation: If light exists asparticles, the intensity of both slits will bethe sum of the intensity from the individualslits.
Wave interpretation: If light exists as waves,
the light waves will have interference underthe principle of superposition, creatingbands of light (constructive interference)and dark (destructive interference).
CONTD
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Interference of light
When two light waves from different coherent
sources meet together, then the distribution of
energy due to one wave is disturbed by the
other. This modification in the distribution oflight energy due to super position of two light
waves is called "Interference of light".
Two types----- constructive interference
destructive interference
----The point at which intensity of light is
maximum is called constructive interference.
-----The point at which intensity of light is
minimum is called destructive interference.
INTERFERENCE CONDITIONS-----
Light must be monochromatic, i.e., involve just
Lamps, flashlights, etc all produce light. But this light is released in many directions, and
the light is very weak and diffuse. In coherent light the wavelength and frequency of the
photons emitted are the same. The amplitude may vary. Such things as lasers and
holograms are composed of coherent light.
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Diffraction
Diffraction is a phenomenon done by
visible light when it passes through a
prism it is seen that it spreads into seven
different colored lights. When it rains arainbow is visible because a drop of rain
acts as the prism and 7 different bright
lights are seen as per the difference in
their wavelengths. More examples can be
light falling on CD or a DVD which enables
us to see different colors. When we blowsoap bubbles against the light, it is notseen as white but as blue, pink, red, etc.
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- The wavelength of the sodium light is given by the
formula in case of biprism
experiment.
= 2d / D
Where = fringe width,
2d = distance between the two virtual sources,
D = distance between the slit and screen.
Again 2d = d1d2Where d1 = distance between the two images formed by
the convex lens in one position.
d2 = distance between the two images formed by the
convex lens in the second position.
Used formula
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Description of
apparatus
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CONTD
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CONTD
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CONTD
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CONTD
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CONTD
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CONTD
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Procedure1. Mount the gadgets on the optical bench.
2.Study all the movements on each stand.3. Ensure that all the pieces are aligned at roughly the same height
4. Remove the stand with the convex lens from the optical bench.
5. Bring the eyepiece close to the biprism.
6. Looking through the eyepiece you will see a bright vertical patch of light. A
slight rotation of the biprism in its own plane will break up this patch into
vertical equidistance fringes.
7. Adjust the slit width to get the best compromise between brightness and
sharpness of the fringe pattern.
8. Move the eyepiece slowly away from the biprism along the optical bench
to a
distance of about 100 cms. Keeping the fringe pattern all the time in the field
of view.9. Keeping eyepiece at a distance of 100 cm from the biprism, measure the
fringe
width by measuring the distance traversed by the eyepiece in crossing about
10 fringes using the main and circular scales on the eye-piece.
10. Interpose the convex lens between the biprism and the eyepiece making
sure
that D>4f.
11. Move the lens along the optical bench till you locate two conjugate
positions
of the lens at which you can see real images of the double slit in the field of
view of the eyepiece.
12. Without disturbing the positions of the slit, biprism and the eyepiece
measure
the double-slit image separations d1 and d2.
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MeasurementsMeasurement of : (Fringe width)
1. The eyepiece is fixed about 100cm away from the slit.
2. The vertical crosswire is set on one of the bright fringes and the
reading on the eyepiece scale is noted.
3. The crosswire is moved on the next bright fringe and the
reading is noted. In this way observation are taken for about 20
fringes.
Measurement of D: (distance between source and screen)
1. The distance between the slit and eyepiece gives D.
Measurement of 2d: (distance between the two sources on
screen)
1. For this part the distance between the eyepiece and slit should
be kept slightly more than four times the focal length of lens. If
necessary the position of the slit and the biprism should not be
altered.
2. The convex lens is introduced the biprism and eyepiece and is
placed near to the eyepiece. The lens is moved towards thebiprism till two sharp images of the slit are seen. The distance d1
is measured by the micrometer eyepiece.
3. The lens is moved towards the biprism till two images are again
seen the distance between these two images give d2.
4. At least two sets of observation for d1 and d2 are taken.
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ObservationFor fringe width--No. of division on the vernire scale-
Least count of vernire-
No. of
fringeMicrometerreading(a) No. of
fringe
Micrometerreading(a) Difference
For 10 fringeMean for10 fringe
Fringewidth(mm)
[Mean10]
MS VS Total(mm)
MS VS Total(mm)
12
3
4
5
67
8
9
10
1112
13
14
15
1617
18
19
20
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CONTDMeasurement of D:
Position of the slit a) =cmPosition of the eyepiece b)=.cmObservation value of D b-a)=..cm
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CONTDMeasurement of 2d-
Micrometer Reading
Mean 2dObservation of d1 Observation of d2
tion of Image Position of IIImage
Position of I Image Position of II Image
VS Total MS VS Total MS VS Total MS VS Total
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Results
Wavelength of Sodium light=
Standard Value of wavelength=5893A0
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Precautionsi) The setting of uprights at the same
level is essential
ii) The Slit should be vertical andnarrow.
iii) Fringe shift should be removed
iv) Bench error should be taken into
account.
v) Crosswire should be fixed in the
center of the fringe while taking observationsfor fringe width.
vi) The micrometer screw should be
rotated only in one direction to avoid backlash
error.
vii) The fringe width should be measured
at a fairly large distance.viii) Convex lens of shorter focal length
should be used (f=25 cms. Approx)
ix) Motion of eyepiece should be
perpendicular to the lengths of the bench.
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