Photo-Electric Effect Experiment
What is photo Electric Effect? What is work function?
Definition
Definition
When light of suitable frequency falls on
metal surface, the electrons are emitted. These are called photo-electrons and
process is known as “Photo electric effect”.
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Photo-electric effect Experiment |
Experimental observation
1) The number of photo-electrons (photo-current) is directly
proportional to the intensity of incident radiation.
2) It is spontaneous emission. Emission of electrons occurs
immediately after the radiation falls on the surface.
3) Electrons are emitted from the metal surface,
no matter the incident radiation is weaker in intensity. Emission of electrons
from metal surface is independent of intensity of the radiation.
4) Emission of electrons depends upon the
threshold frequency, if frequency of incident radiation is higher than the
threshold frequency then electrons will be emitted without decay.
Ø Above results cannot explained by the
photo-electric effect. The classical theory cannot explain the threshold
frequency of light.
Ø The results cannot be explained on the basis
of electromagnetic wave theory of light.Quantum mechanical Explanation
Einstein put forward
Quantum mechanical explanation of the photo-electric effect using Planck’s
black body radiation theory.
Theory
1) Incident radiation in photo-electric effect consist of tiny
particles carry quanta of energy called photon like tiny oscillator
defined in black body radiation. E=hѵ
2) On interaction of those photons with electrons of metal. All of
the energy of photons is transferred to electrons.
3) The acquired energy from photons by electrons is used up as
follows.
Overcome the work-function of metal
1) Releases the electron from metal surface.
2) Remaining energy is converted into the K.E of the electrons.
Mathematically
i.e.
hѵ=
hѵ0 +K.E
hѵ0 =Work function ѵ0 = Threshold frequency
Measurement of work function
K.E of emitted
electrons i-e Photo electrons can be measured by collecting electrons at anode
i-e at negative potential. The voltage at which Electrons are stopped is called
as stopping potential.
Mathematically.
K.E=eѵ0 Where
ѵ0 = stopping potential
Ø hѵ = hѵ0 +ev
h(ѵ- ѵ0) =
K.E
If ѵ <ѵ0 Then K.E<
0
Which is not true.
Hence no electrons can be emitted from the metal surface if incidents frequency
is less than threshold frequency.
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