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Monday, 5 November 2012
PHYSICS EXPERIMENT 11
Experiment No.-11
Object:-
To verify Inverse square law of light using a photo cell.
Apparatus Required:-
Optical bench, Photocell housed with Red and Black sockets, lamp house with
lamps, DC Microammeter.
Theory:- The
Photoelectric emission may be regarded as a phenomena of liberation of an
electron at the surface of a metal when a photon of light having energy above
threshold energy (metal work function) incident on a metallic surface and
transfer the enough energy to the electron to escape through the potential
barrier layer. The photo cell can be considered as the generation of a voltage
across a circuit element under illumination.
Let
P be the illuminating Power of a source so the intensity of illumination I due
to it at a distance r would be
I=
P/r2
Since
the photo electric current (θp) produced is directly proportional to the
intensity of illumination ie.
I
α θp
I=Kθp
Where
K is constant, hence I= P/r2 = Kθp. Since P and K are constant hence
the relationship between 1/r2 and θp is straight line which verifies
the inverse square law of radiation.
Procedure:-
1.
Arrange the optical bench in such a
way that both the lamp and the photo cell are at the same level as shown in the
figure.
2.
Make the connection of photo cell to
microammeter Red to (+)ve and black to (–)ve terminal of the microammeter.
3.
Adjust the distance of the lamp such that we
will get the microammeter reading
4.
Then decreases the distance in step
of 5cm and each time note the reading in microammeter and note your observation
in table-1.
5.
Draw the curve between 1/r2 and d.
1/r2 on x axis and θp at y axis.
Observation
table:-
S.N.
|
Distance of lamp from cell in
cm ‘r’
|
1/r2
|
Reading in microammeter
(θp) uA
|
1.
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2.
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3.
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4.
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5.
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6.
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7.
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8.
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9.
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10.
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Result:-
The
graph between θp and 1/r2 is a straight line. It show that
microammeter reading is inversely proportional to the square of the distance
from the source. but deflection is directly proportional to the intensity of
illumination of the surface. Hence we can say that intensity of illumination
varies inversely square of the distance from the source. Thus inverse square
law is verified.
Precautions:
1.
Light should fall on normally on the photocell
2.
The photocell should not be exposed to light for a long time continuously.
3.
A Cover should be placed on the photocell to protect it.
Viva Voce:
Q.1
What is photoelectric effect?
Ans:
When light is falls on metal surface, an electron is emitted from a metal if the energy of the photon is greater
than the work function of the metal.
Q.2
What is the photo cell?
Ans: A photocell is
a type of resistor. When light strikes the cell, it allows current to flow more
freely. When dark, its resistance increases dramatically.
Q.3:
Does the photo electric current depend on frequency of light and intensity of
light? How?
Ans: The photons of a light
beam have a characteristic energy proportional to the frequency of the light.
In the photoemission process, if an electron within some material absorbs the
energy of one photon and acquires more energy than the work function (the electron binding energy) of the material, it is
ejected. If the photon energy (Frequency) is too low, the electron is unable to
escape the material. Increasing the intensity of the light beam increases the
number of photons in the light beam, and thus increases the number of electrons
excited, but does not increase the energy that each electron possesses. The
energy of the emitted electrons does not depend on the intensity of the
incoming light, but only on the energy or frequency of the individual photons.
It is an interaction between the incident photon and the outermost electron.
Q.4:
Define the illuminating power, Intensity of illumination?
Ans: Illumination power is defined as the
intensity per unit area. Intensity is defined as no. of photon incident per
unit area.
Q.5:Explain the construction of photo cell?
Ans: This is Selenium Photocell. This consist of
metal base plate mainly Aluminum, steel or brass. On This base plate a very
thin layer of special grade selenium is deposited followed by a deposition of
light transparent protective film of cadmium or cadmium Oxide. The light
sensitive face of a selenium photocell is either brown or bluish brown in
appearance and has a narrow silvery collector strip. This strip serves as a
negative terminal. The back of base plate is also coated with the same material
as the narrow strip and serves as a positive terminal.
|
PHYSICS EXPERIMENT 10
EXPERIMENT NO. 10
Object:
To measure the numerical aperture of the given an optical fiber.
Apparatus
Required: Diode Laser Source, Fiber Holders,
Optical Fiber, and Base With Rotational Mount, Holders And Bases.
Theory:
Numerical aperture is a basic descriptive characteristic of a specific fiber.
It represents the size or degree of openness of the input acceptance cone.
Mathematically it is defined as the sine half angle of the acceptance cone.
Using snell’s law,
the maxima angle with in which light will be accepted into and guided through
fiber is
NA=Sin(өa)=
(n12- n22)1/2
Where өa
is
the numerical aperture and n1 and n2 are the refractive
indices of the core and the cladding. If the incident angle ө < өa,
the ray undergoes multiple internal reflections at core and cladding interface
and it is called the guided ray. If өa < ө, the ray undergoes only partial reflection at core cladding interface.
In short length of straight fiber, ideally a ray launched at angle ө at the input
end should come out at the same angle ө
from output end. Therefore, the far field at the output end will also appear as
a cone of semi angle өa
emanating from the fiber end.
DIAGRAM:-
DIAGRAM:-
Procedure:
1.
Mount Laser source, objective and
detector on the respective holders.
2.
Mount both the ends of the optical
fiber on the fiber holders.
3.
Align the difference objects as per
the setup shown below.
4.
Couple the light from the laser
source onto one of the fiber ends using a microscopic objective (provided with
the kit).
5.
Place the screen (sheet having
circular markings) at some distance from the output end of the fiber such that
it is perpendicular to the axis of the fiber. Now move the screen towards or
away from the output end of the fiber such that circular beam emanating from
the fiber end covers the (1st or 2nd or 3rd)
circle on the screen.
6.
Measure the distance between the
output end of optical fiber and screen. Let this be L, also measure the
diameter of the circular spot formed on the screen. (Diameter is mentioned in
mm). Let it be D.
7.
Use the formula
Observations
table:
S.No.
|
Diameter of Laser Spot
D mm
|
Distance between Optical Fiber and
Screen
L mm
|
NA=Sin ө
|
||
Result:
Numerical
Aperture of given optical fiber is=……………………………………
Percentage Error:-
(Standard value~ Observed Value) X 100
Standard Value
Precautions:
1.
Reading should be taken carefully.
2. Direct viewing of laser
light should be avoided.
3.
Laser light should be incident normally on the Screen.
Viva voce
1. Define optical fiber.
Ans.
It is a cable which carries optical signal.
2.
On which phenomenon light propagation take place in optical fiber
Ans.
Total internal reflection.
3. What
is total internal reflection?
Ans.
When light travels from denser medium to rarer medium and angle of incidence is greater than critical
angle then light reflects back into same medium this phenomenon is called Total
internal reflection.
4. Define angle of acceptance
Ans. Angle at
which light enter into optical fiber and Total Internal Reflection takes place.
5. What
is physical significance of numerical aperture.
Ans. Light gathering
ability of the fiber.
6. What
are the types of optical fiber
Ans.
There are two types of fiber (1) step index fiber (2) graded index fiber.
7. What
is fractional refractive index?
Ans. It is the
ratio of difference of the refractive indices of core and cladding to the
refractive index of core i.e.,
8. Which
light source is used in experiment
Ans. Diode Laser
9. LASER
stands for what?
Ans. Light
Amplification by Stimulated Emission of Radiation
10.
How many type of fiber losses are
there?
There are three types of fiber losses
(1) Absorption
(2) Rayleigh
Scattering
(3)
Geometrical losses
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