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Slide 1 of 4
Chapter 3: X-RAY PRODUCTION
Ionization and Excitation
Ionization is “knocking” an electron out of an atom
– Creates a free electron + ion (an atom with +1 charge)
– Occurs when radiated with energy above the electron binding
energy
Excitation is “knocking” an electron to a higher orbit
– When the radiation energy is lower than the binding energy
After either ionization or excitation, an atom has higher energy
Slide 2 of 4
Chapter 3: X-RAY PRODUCTION
X-Ray Beam Quality and Intensity
The x-ray beam has two main properties you need to understand.
Beam QUALITY is the ability of the beam to penetrate an object,
its all about the penetrating power of the x-ray photons.
Beam INTENSITY this is the number of x-ray photons in the beam.
Slide 3 of 4
Chapter 3: X-RAY PRODUCTION
Factors Affecting X-ray Quality
1. Filtration.
The primary purpose of adding filtration to the x-ray beam is to
remove low energy x-rays that have no chance of getting to the film.
As filtration is increased, so is the beam quality, but quantity is
decreased.
Slide 4 of 4
Chapter 3: X-RAY PRODUCTION
There are three types of filtration:
i. Inherent Filtration: The glass envelope window equals about 0.5
mm Al
ii. Added Filtration: Added in collimator
iii. Compensating Filtration: Used to improve image quality or
radiation reduction
Slide 5 of 4
Chapter 3: X-RAY PRODUCTION
i. Inherent Filtration
The glass envelope of the tube filters the emerging beam. In
diagnostic x-ray tubes the glass is equal to about 0.5 mm Al.
As tube ages and more tungsten is vaporized, tungsten will build up on
the inside of the tube that will add more filtration.
Slide 6 of 4
Chapter 3: X-RAY PRODUCTION
ii. Added Filtration
One or two mm of aluminum is added filtration placed in the
collimator. This filtration is generally placed on the mirror of the
collimator.
This filtration attenuates x-rays of all energies emitted from the tube.
This shifts the spectrum to the high side.
Slide 7 of 4
Chapter 3: X-RAY PRODUCTION
iii. Compensating Filters
Compensating filters are added to the beam by the operator to
compensate for differences in subject tissue density or type.
In areas of the body where there are great differences in tissue
density, compensating filters are used to reduce exposure in the area
of less density.
This reduced patient exposure and improves image quality. The
thoracic spine and full spine x-rays need filtration.
Slide 8 of 4
Chapter 3: X-RAY PRODUCTION
Compensating Filters
This is the 40” Cervicothoracic Compensating Filter.
It may be called the thyroid filter as it reduces the exposure to the upper thorax.
Slide 9 of 4
Chapter 3: X-RAY PRODUCTION
Compensating Filters
This heart shaped filter is used to reduce exposure to the ovaries of females of child bearing age.
It reduces exposure by about 85%.
Slide 10 of 4
Chapter 3: X-RAY PRODUCTION
2. Kilovoltage
As the kVp is increased, so is beam quality and therefore HVL.
An increase in kVp results in a shift of the x-ray emission spectrum
towards the higher energy side.
This increases the effective energy of the beam, making it more
penetrating.
Slide 11 of 4
Chapter 3: X-RAY PRODUCTION
Factors Affecting X-ray Intensity
A number of factors affect X-ray Intensity @ Quantity. These same
factors also control radiographic film density:-
a) Milliamperage- Seconds (mAs)
b) kVp
c) Distance
d) Filtration
Slide 12 of 4
Chapter 3: X-RAY PRODUCTION
1. mA x time (s) = miliamperage seconds = mAs
The X-ray quantity is directly proportional to the mAs. If we double
the mAs, the number of electrons striking the target is doubled.
300 mA @ 1/30 second = 10 mAs
200 mA @ 1/20 second = 10 mAs
100 mA @ 1/10 second = 10 mAs
Slide 13 of 4
Chapter 3: X-RAY PRODUCTION
2. Kilovoltage
X-ray intensity varies rapidly with changes in kVp.
The change in quantity is proportional to the square of the ratio of the
change.
If the kVp is doubled, the intensity would increase by a factor of four.
Slide 14 of 4
Chapter 3: X-RAY PRODUCTION
What really happens when the kVp is increased?
When kVp is increased, the penetrability of the x-rays is increased and
relatively fewer x-rays are absorbed in the patient.
More rays pass through the patients to interact with the film.
To maintain a constant exposure of the film, an increase of 15% in
kVp should be accompanied by a reduction of one half the mAs.
Slide 15 of 4
Chapter 3: X-RAY PRODUCTION
3. Distance
Radiation intensity from an x-ray tube varies inversely with the square
of the distance from the target. This is referred to as the inverse
square law.
It is the same for any type of electromagnetic energy.
We will explores distances in the Lab.
Slide 16 of 4
Chapter 3: X-RAY PRODUCTION
4. Filtration
X-ray machines have metal filters inserted into the useful beam.
The primary purpose is the remove the low energy beam that reach
the patient and are absorbed superficially.
These low energy photons contribute nothing to the formation of the
radiographic image.
Filters therefore reduce patient exposure.
Slide 17 of 4
Chapter 3: X-RAY PRODUCTION
Primary and Secondary Radiation
Slide 18 of 4
Chapter 3: X-RAY PRODUCTION
Primary Radiation
The radiation that coming directly from a source, such as a radioactive
substance or an x-ray tube, without interactions with matter.
Slide 19 of 4
Chapter 3: X-RAY PRODUCTION
Secondary Radiation
This type of radiation is produced by a scattering of the primary x-ray
beam.
The x-ray photons and photo-electrons in the beam undergo a change
of direction after interaction with atoms and molecules as they pass
through a substance.
Slide 20 of 4
Chapter 3: X-RAY PRODUCTION
X-ray Tube
The major components of the modern X-ray tube are: -
a) cathode (electron source)
b) anode (acceleration potential)
c) rotor/stator (target device)
d) glass/metal envelope (vacuum tube)
Slide 21 of 4
Chapter 3: X-RAY PRODUCTION
a) Cathode
The cathode consists of:
consists of the filament,
focusing cup, and associated
wiring.
a spiral of heated low
resistance tungsten wire
(filament) is for electron
emission. Wire is heated by
filament current.
Slide 22 of 4
Chapter 3: X-RAY PRODUCTION
b) Anode
Consists of the anode, stator,
and rotor.
Positively charged so that the
electrons from the filament
(cathode) are attracted to it
to produce x-rays.
Slide 23 of 4
Chapter 3: X-RAY PRODUCTION
c) Rotor and Stator
The rotor is the non-
stationary part of a rotary
electric motor or alternator,
which rotates because the
wires and magnetic field of
the motor are arranged so
that a torque is developed
about the rotor's axis.
Slide 24 of 4
Chapter 3: X-RAY PRODUCTION
The stator is the stationary
part of an electric motor or
alternator. Depending on the
configuration of the motor the
stator may act as the field
magnet, interacting with the
armature to create motion. The
stator may be either a per
magnet or an electromagnet.
Slide 25 of 4
Chapter 3: X-RAY PRODUCTION
Rotating and Stationary Anode
Stationary Anode: An anode assembly that is immobile.
Rotating Anode: An anode assembly that turns during exposure.
Slide 26 of 4
Chapter 3: X-RAY PRODUCTION
d) Glass and Metal Envelope
The envelope is the glass
housing that protects the
tube. It is also used to help
protect from excessive
exposure to x-rays. The
envelope is the first part of
the filtration system.
Slide 27 of 4
Chapter 3: X-RAY PRODUCTION
Basic X-ray Circuit
There are two main parts of the circuit, one is the main circuit and
the second is the filament circuit.
A. Main part of X-Ray Circuit: supplies power to the x-ray tube so that
x-rays are produced.
B. Filament Circuit: supplies power to the filament of the x-ray tube so
that the filament supplies enough electrons by thermionic emission.
Slide 28 of 4
Chapter 3: X-RAY PRODUCTION
Basic X-ray Circuit
Slide 29 of 4
Chapter 3: X-RAY PRODUCTION
a) Main X-ray Circuit
Main Switch: The switch that generates the power to the x-ray tube.
Exposure Switch: A remote control device that permits current to
flow through the circuit.
Timer: Device used to end the exposure at an accurately measured
preset time.
Slide 30 of 4
Chapter 3: X-RAY PRODUCTION
In the diagram below are the important parts of the circuit. The blue
part is the main x-ray circuit and the tan part is the filament circuit.
Slide 31 of 4
Chapter 3: X-RAY PRODUCTION
Components
1. main breaker - this is where the alternating current comes from to power the circuit.
2. exposure switch - when you push the button to start an exposure this switch closes to
start the exposure.
3. autotransformer - this is where you adjust the kVp for the exposure.
4. timer circuit - this part of the circuit stops the exposure.
5. high-voltage step-up transformer - this transformer bumps the voltage up so that the x-
ray tube has very high voltage to make the electrons have enough energy to form x-rays.
6. four-diode rectification circuit - this makes the current only go in one direction through
the x-ray tube.
7. filament circuit variable resistor - this variable resistor adjusts the current going to the
filament.
8. filament step-down transformer - this transformer steps the voltage down and therefore
the current up.
9. x-ray tube - this is where the x-rays are created.
10. rotor stator - this rotates the anode.
Slide 32 of 4
Chapter 3: X-RAY PRODUCTION
b) Filament Circuit
Control Factor Electrical Device and Location in Circuit
kVp Selection kVp LevelAutotransformer (between incoming line and
exposure switch)
mA Selection Filament CurrentVariable resistor (in filament circuit between
incoming line and step-down transformer)
Time Selection Length of exposureTimer circuit (between exposure switch and
step-up transformer)
Rotor Switch Speed of rotating anodeStator (separate circuit from stator of anode
motor)
Exposure Switch Moment of exposureSwitch (between autotransformer and timer
circuit)
Slide 33 of 4
Chapter 3: X-RAY PRODUCTION
References
John Ball, Adrian D. Moore, Steve Turner (2008) Essential Physics for
Radiographers, Blackwell
Richard R. Carlton, Arlene McKenna Adler (2005) Principles of
Radiographic Imaging, Delmar