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~Lalit Kishore,
The Plenum School, HP
Production of Electromagnetic
waves
 When a charged particle is accelerated:
 Electromagnetic wave / stream of photons
(Bremmstrahhung radiation/ braking) is produced
 The larger the acceleration or deceleration of charged
particle, the higher is frequency (or lower the
wavelength) of penetration of the produced e-m waves
or emitted photons
Production of X-rays: High
frequency e-m waves / photons
 X-Ray photons are produced by:
 Bombarding high speed cathode rays (beam of
electrons) against a mental target
 Cause of production
 Sudden stoppage and change in direction of the
beam of electrons / cathode rays which is nothing
but a very large deceleration /retardation
 Note: A lot of thermal energy / heat is also produced in
the process
Diagram of X-Ray Tube
Diagram with numbered parts Label for the parts
1. Evacuated glass envelope
2. Low voltage source
3. Heated filament as cathode
4. X-ray window
5. Cooled metallic anode
6. Target metal
7. High voltage source
8. Cathode rays
9. X-rays
X-Ray spectrum: Variation in X-ray
wavelengths
Spectrum description
Curve for typical wave length
variation
 Two typical X-Ray spectrum
components
 Continuous distribution
accelerating cathode rays of
wavelengths interrupted by
line spectrum of target metal
 Two sharp cut-offs at short
wavelength side of spectrum
as line spectrum of target
metal
 Sharp spectrum cut-offs
produce X-Rays
Applied formula for cut-off
wavelength of X-rays
 Cut-off wavelength of X-rays is given by the following
formula
hc/eV
 Where
 h is Plank’s constant
 c is velocity of light
 e is charge on electron
 V is PD across electrodes
Diagram of X-ray image formation
Numbered Diagram Labels for parts
1. Beam of X-rays
2. Soft tissues
3. Bone
4. X-ray film
5. Developed film parts
a. White for the bone
b. Dark or black for the bone
Absorption and penetration of X-
rays through human body
 Barium meal is given for investigating stomach
ailments
 Barium sulphate is a good absorber of X-rays to give a
clear image of the stomach
 By injecting a radio-opaque dye into the into the
blood stream, blood vessels can be imaged on X-ray
film
X-rays imaging of bones
Curve: A common X-ray spectrum parts
 X-axis: wavelength
 Y-axis: Intensity of X-rays
 Peak-1 as line spectrum of
target
 Peak-2 as line spectrum of
target
 Note : cut-off wavelength formula
of X-rays
hc/eV
Attenuation (change of intensity) of X-rays for diagnosis
Attenuation Curve Application
 Principle: When X-rays pass
through a medium, their
intensity is reduced
 The %age of intensity
transmitted with thick has the
typical curve
 It has been seen that same
thickness produces half of the
variation of intensity
 With a parallel beam, linear
attenuation coefficient of tissues
is calculated for diagnostic
purposes
 Formula is given on the curve

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X-Rays and their Medical Use.pptx

  • 2. Production of Electromagnetic waves  When a charged particle is accelerated:  Electromagnetic wave / stream of photons (Bremmstrahhung radiation/ braking) is produced  The larger the acceleration or deceleration of charged particle, the higher is frequency (or lower the wavelength) of penetration of the produced e-m waves or emitted photons
  • 3. Production of X-rays: High frequency e-m waves / photons  X-Ray photons are produced by:  Bombarding high speed cathode rays (beam of electrons) against a mental target  Cause of production  Sudden stoppage and change in direction of the beam of electrons / cathode rays which is nothing but a very large deceleration /retardation  Note: A lot of thermal energy / heat is also produced in the process
  • 4. Diagram of X-Ray Tube Diagram with numbered parts Label for the parts 1. Evacuated glass envelope 2. Low voltage source 3. Heated filament as cathode 4. X-ray window 5. Cooled metallic anode 6. Target metal 7. High voltage source 8. Cathode rays 9. X-rays
  • 5. X-Ray spectrum: Variation in X-ray wavelengths Spectrum description Curve for typical wave length variation  Two typical X-Ray spectrum components  Continuous distribution accelerating cathode rays of wavelengths interrupted by line spectrum of target metal  Two sharp cut-offs at short wavelength side of spectrum as line spectrum of target metal  Sharp spectrum cut-offs produce X-Rays
  • 6. Applied formula for cut-off wavelength of X-rays  Cut-off wavelength of X-rays is given by the following formula hc/eV  Where  h is Plank’s constant  c is velocity of light  e is charge on electron  V is PD across electrodes
  • 7. Diagram of X-ray image formation Numbered Diagram Labels for parts 1. Beam of X-rays 2. Soft tissues 3. Bone 4. X-ray film 5. Developed film parts a. White for the bone b. Dark or black for the bone
  • 8. Absorption and penetration of X- rays through human body  Barium meal is given for investigating stomach ailments  Barium sulphate is a good absorber of X-rays to give a clear image of the stomach  By injecting a radio-opaque dye into the into the blood stream, blood vessels can be imaged on X-ray film
  • 9. X-rays imaging of bones Curve: A common X-ray spectrum parts  X-axis: wavelength  Y-axis: Intensity of X-rays  Peak-1 as line spectrum of target  Peak-2 as line spectrum of target  Note : cut-off wavelength formula of X-rays hc/eV
  • 10. Attenuation (change of intensity) of X-rays for diagnosis Attenuation Curve Application  Principle: When X-rays pass through a medium, their intensity is reduced  The %age of intensity transmitted with thick has the typical curve  It has been seen that same thickness produces half of the variation of intensity  With a parallel beam, linear attenuation coefficient of tissues is calculated for diagnostic purposes  Formula is given on the curve