PROPORTIONAL
COUTER
OBJECTIVES
Introduction
construction
Principle
Operation
Working
Uses
Advantage
Disadvantage
PROPORTIONAL COUNTER
Classification of detectors
oIt is a ion collection based detector which
is used to Detect the nuclear particles or
radiations.
oIt is classified in gaseous state detectors
Introduction
CONSTRUCTION
Thin metalic wire
strip
o It contains cylinder metallic tube filled with argon and
methane gas.
o The ratio of argon and methane gas is 9:1 at one
atmospheric pressure .
o Metallic wire (tungsten) act as a anode.
o Metallic tube act as a cathode.
o The wire is connected to pulse amplifire.
 When a particle of low specific ionization passes
through an ionisation chamber the pulse produced is
too small to be detected.
 When applied voltage is increased in chamber is
increased it start works in proportinal region.
PRINCIPLE
Operation
 E =
𝑉
𝑟 ln(
𝑏
𝑎
)
Where:-
V = applied potential difference
b = radii of the cylinder
a = radii of an axial wire
r = distance from the central wire
When a charged particle or radiation such as ᾳ, ᵦ-
particle or ϒ-ray photon enters an ionisation
chamber, ionisation of gas take place resulting in an
ion pair formation.
Positive ion chamber.
Electron central wire.
In this multiplication or gas amplification, the number of
ions increases exponentially.this process is cumulative and is
called avalanche.
Dependency of avalanche
Radius of anode wire.
Radius of tube.
Applied voltage.
Nature of gas.
The value of gas multiplication factor ‘M’ is give by 103 in
this region.
 M=
𝑛
(1−𝑛𝑝)
Here
n=number of secondary electrons produced by the primary eletrons.
p=the probability of production of photoelectrons.
The shape of the voltage pulse does not depend on the
track of the primary ions.
Uses
The proportional counter permits both the counting
and energy determination of particles even of very
low energy.
It can be used as a spectrometer.
They are also used for detection of neutrons, fission
fragments etc.
Counting ᾳ-particle in the presence of ᵦ-particle and
ϒ-rays.
Disadvantage
This counter is that the amplification
factor depends on the applied voltage.
The applied voltage must be
maintained constant within the narrow
limit because a slight change in voltage
changes the gas amplification.
 Harish Kumawat 15CS15
 Harsh Bansal 15CS16
 Harshit gupta 15CS17
 Hemant Khorwal 15CS18
 Hemraj Saini 15Cs19
 Himani Sharma 15CS20
 Hitesh Runthala 15CS21
THANK YOU

Proportional counter

  • 1.
  • 3.
  • 4.
  • 5.
    oIt is aion collection based detector which is used to Detect the nuclear particles or radiations. oIt is classified in gaseous state detectors Introduction
  • 6.
  • 7.
    o It containscylinder metallic tube filled with argon and methane gas. o The ratio of argon and methane gas is 9:1 at one atmospheric pressure . o Metallic wire (tungsten) act as a anode. o Metallic tube act as a cathode. o The wire is connected to pulse amplifire.
  • 8.
     When aparticle of low specific ionization passes through an ionisation chamber the pulse produced is too small to be detected.  When applied voltage is increased in chamber is increased it start works in proportinal region. PRINCIPLE
  • 10.
    Operation  E = 𝑉 𝑟ln( 𝑏 𝑎 ) Where:- V = applied potential difference b = radii of the cylinder a = radii of an axial wire r = distance from the central wire
  • 11.
    When a chargedparticle or radiation such as ᾳ, ᵦ- particle or ϒ-ray photon enters an ionisation chamber, ionisation of gas take place resulting in an ion pair formation. Positive ion chamber. Electron central wire.
  • 12.
    In this multiplicationor gas amplification, the number of ions increases exponentially.this process is cumulative and is called avalanche.
  • 13.
    Dependency of avalanche Radiusof anode wire. Radius of tube. Applied voltage. Nature of gas.
  • 14.
    The value ofgas multiplication factor ‘M’ is give by 103 in this region.  M= 𝑛 (1−𝑛𝑝) Here n=number of secondary electrons produced by the primary eletrons. p=the probability of production of photoelectrons.
  • 15.
    The shape ofthe voltage pulse does not depend on the track of the primary ions.
  • 16.
    Uses The proportional counterpermits both the counting and energy determination of particles even of very low energy. It can be used as a spectrometer. They are also used for detection of neutrons, fission fragments etc. Counting ᾳ-particle in the presence of ᵦ-particle and ϒ-rays.
  • 17.
    Disadvantage This counter isthat the amplification factor depends on the applied voltage. The applied voltage must be maintained constant within the narrow limit because a slight change in voltage changes the gas amplification.
  • 18.
     Harish Kumawat15CS15  Harsh Bansal 15CS16  Harshit gupta 15CS17  Hemant Khorwal 15CS18  Hemraj Saini 15Cs19  Himani Sharma 15CS20  Hitesh Runthala 15CS21 THANK YOU