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The inner-shell electron is tightly bound to the nucleus. Thus, K-shell
electrons or inner-shell electrons have a higher binding energy than
outer-shell electrons. Tungsten is a large atom with 74 orbiting
electrons. As atomic complexity increases, the electrons in any given
shell are more tightly bound than in a less complex atom.
When the projectile electron ionizes a target atom by removing a K-
shell electron, a temporary electron void is produced in the K-shell. This
is a highly unnatural state for the target atom and is corrected by an
outer-shell electron falling into the void in the K shell. Tungsten, for
example, has electrons in shells out to the P shell, and when a K-shell
electron is ionized, its position can be filled with electrons from any of
the outer shells. The transition of an orbital electron from an outer shell
to an inner shell is accompanied by the emission of an X-ray.
X-ray Basics
The production of heat and characteristic X-rays involves interactions between the
projectile electrons and the electrons of target atoms. Another type of interaction in
which the projectile electron can lose its kinetic energy is an interaction with the nucleus
of a target atom. In this type of interaction the kinetic energy of the projectile electron is
converted into electromagnetic energy.
A projectile electron that completely avoids the orbital electrons as it passes through a
target atom may come sufficiently close to the nucleus of the atom to come under its
influence. Because the electron is negatively charged and the nucleus is positively
charged, there is an electrostatic force of attraction between them. The closer the
projectile electron gets to the nucleus, the more it is influenced by the electrostatic field
of the nucleus. This field is very strong because the nucleus contains many protons and
the distance between the nucleus and the projectile electron is very small. As the
projectile electron passes by the nucleus, it slows down, changes its course, and leaves
with reduced kinetic energy in a different direction. These types of X-rays are called
Bremsstrahlung X-rays. Bremsstrahlung is a German word for slowing down or braking.
No feedback of generated KV, mA/
open loop
High Skin Dose
Inferior image quality
Close loop regulations
No skin dose
Superior image quality
Micro-controller
Block Diagram Multi-pulse
DC
AC
DC
AC
DC
AC
Line Input
EMI Filter
Inverter High Voltage
Transformer
400 V » UDC = 566 V
IGBT: fres
= 30 - 100 kHz
U T
= 40 - 150 kV
I T
= 0,1 - 1000 mA
P Puls = 4 W - 100 kW
P 60s £ 40 kW
P 10min £ 10 kW
U Tube
ITube
IF
Tube Rotating Anode
Control
fan = 4 - 300 Hz IGBT
S = 10 - 20 kVA
PWM
fres
= 20 - 100 kHz
PH = 100 - 150 W
IGBT
3 »
UDC
mA Regulation/ Tube current
KV Regulation
Power Storage Generators
A grid
Diode
In brief
Hot Tube
HT of Line F Gen
HT of HF Gen
Light weight
Low Cost
KV Generation
Focusing cup
Voltage compensation at filament transformer
 A Crossed grid has two grids sandwiched together
with the result that the strips are usually both
parallel to and at right angles to the long
dimension of the grid.
 A focused grid is one in which the lead strips
are tilted progressively as they move away
from center. Lines through each of these strips
would converge at a point known as the grid
focus.
Grid Primary Transmission
The useful X-Rays which pass straight from
the X-Ray tube to the film are known as
Primary transmission is basically the
percentage of primary X-Rays which pass
through the grid and hit the film, and is thus
measured by using the same apparatus with
and without the grid in place.
Grid cutoff is an undesirable absorption of
primary x-ray beams by grid strips, which
prevents the useful x-rays from reaching the
image receptor. It is caused by improper
grid positioning and most often occurs with
parallel grids.
 The quantity of scattered radiation in an x-ray beam reaching a
receptor can be reduced by separating the patient's body and
receptor surface, as shown below. This separation is known as
an air gap. Scattered radiation leaving a patient's body is more
divergent than the primary x-ray beam. Therefore, scattered
radiation spreads out of the primary beam area. The reduction of
scattered radiation in proportion to primary radiation increases
with air-gap distance. Several factors must be considered when
using this method of scatter reduction. Patient exposure is increased
because of the inverse-square effect. The use of an air gap
introduces magnification. Therefore, a larger receptor size is
required to obtain the same patient area coverage. If the air gap is
obtained by increasing the tube-to-receptor distance, the x-ray
equipment must be operated at a higher output to obtain adequate
receptor exposure.
 A bucky is typically used for table or wall
mounted x-raysystems and holds the x-
ray cassette and grid. A bucky, is a device
found underneath the exam table, a drawer like
device that the cassette and grid is slid into
before shooting x-ray.
Two Pulse generators
Control Console
Control Panel
Image intensifier
Oil in x-ray tube and HV Transformer
for cooling and Insulation
That is stable at high temperatures and has
excellent electrical insulating properties Its
functions are
To insulate,
suppress corona ,
Supress arcing, and to serve as a coolant.
What is Arcing
An AEC system uses a physically thin
radiation
An AEC system uses a physically thin radiation ionization
detector "AEC detector" which is positioned between the
patient being x-rayed and the x-ray film cassette. X-rays
passing through the patient also pass through this "AEC
detector" before they strike the x-ray film.
A weak ionization signal from the AEC detector is
integrated as a ramp shaped voltage waveform. This ramp
signal rises until it matches a pre-set threshold. At this
point the x-ray exposure is terminated. AEC devices are
calibrated to ensure that similar exams have linearity in
exam densities. This is due to the fact that a milliamperage
station is no longer selected and instead relies upon the
ionization within the selected chambers

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BMET X-ray.pdf

  • 1.
  • 2.
  • 3.
  • 4. The inner-shell electron is tightly bound to the nucleus. Thus, K-shell electrons or inner-shell electrons have a higher binding energy than outer-shell electrons. Tungsten is a large atom with 74 orbiting electrons. As atomic complexity increases, the electrons in any given shell are more tightly bound than in a less complex atom. When the projectile electron ionizes a target atom by removing a K- shell electron, a temporary electron void is produced in the K-shell. This is a highly unnatural state for the target atom and is corrected by an outer-shell electron falling into the void in the K shell. Tungsten, for example, has electrons in shells out to the P shell, and when a K-shell electron is ionized, its position can be filled with electrons from any of the outer shells. The transition of an orbital electron from an outer shell to an inner shell is accompanied by the emission of an X-ray. X-ray Basics
  • 5.
  • 6.
  • 7. The production of heat and characteristic X-rays involves interactions between the projectile electrons and the electrons of target atoms. Another type of interaction in which the projectile electron can lose its kinetic energy is an interaction with the nucleus of a target atom. In this type of interaction the kinetic energy of the projectile electron is converted into electromagnetic energy. A projectile electron that completely avoids the orbital electrons as it passes through a target atom may come sufficiently close to the nucleus of the atom to come under its influence. Because the electron is negatively charged and the nucleus is positively charged, there is an electrostatic force of attraction between them. The closer the projectile electron gets to the nucleus, the more it is influenced by the electrostatic field of the nucleus. This field is very strong because the nucleus contains many protons and the distance between the nucleus and the projectile electron is very small. As the projectile electron passes by the nucleus, it slows down, changes its course, and leaves with reduced kinetic energy in a different direction. These types of X-rays are called Bremsstrahlung X-rays. Bremsstrahlung is a German word for slowing down or braking.
  • 8.
  • 9.
  • 10.
  • 11.
  • 12.
  • 13.
  • 14.
  • 15.
  • 16.
  • 17. No feedback of generated KV, mA/ open loop High Skin Dose Inferior image quality
  • 18.
  • 19. Close loop regulations No skin dose Superior image quality Micro-controller
  • 21. DC AC DC AC DC AC Line Input EMI Filter Inverter High Voltage Transformer 400 V » UDC = 566 V IGBT: fres = 30 - 100 kHz U T = 40 - 150 kV I T = 0,1 - 1000 mA P Puls = 4 W - 100 kW P 60s £ 40 kW P 10min £ 10 kW U Tube ITube IF Tube Rotating Anode Control fan = 4 - 300 Hz IGBT S = 10 - 20 kVA PWM fres = 20 - 100 kHz PH = 100 - 150 W IGBT 3 » UDC
  • 25.
  • 27.
  • 28. Diode
  • 29.
  • 30.
  • 31.
  • 32.
  • 33.
  • 35.
  • 36.
  • 37.
  • 38.
  • 40.
  • 41.
  • 42. HT of Line F Gen HT of HF Gen Light weight Low Cost
  • 44.
  • 45.
  • 46.
  • 47.
  • 48.
  • 49.
  • 50.
  • 51.
  • 52.
  • 53.
  • 54. Focusing cup Voltage compensation at filament transformer
  • 55.
  • 56.
  • 57.
  • 58.
  • 59.
  • 60.
  • 61.
  • 62.
  • 63.
  • 64.
  • 65.
  • 66.
  • 67.
  • 68.
  • 69.
  • 70.
  • 71.
  • 72.
  • 73.
  • 74.
  • 75.
  • 76.
  • 77.  A Crossed grid has two grids sandwiched together with the result that the strips are usually both parallel to and at right angles to the long dimension of the grid.
  • 78.  A focused grid is one in which the lead strips are tilted progressively as they move away from center. Lines through each of these strips would converge at a point known as the grid focus.
  • 79.
  • 80.
  • 81.
  • 82. Grid Primary Transmission The useful X-Rays which pass straight from the X-Ray tube to the film are known as Primary transmission is basically the percentage of primary X-Rays which pass through the grid and hit the film, and is thus measured by using the same apparatus with and without the grid in place.
  • 83.
  • 84.
  • 85.
  • 86.
  • 87.
  • 88.
  • 89. Grid cutoff is an undesirable absorption of primary x-ray beams by grid strips, which prevents the useful x-rays from reaching the image receptor. It is caused by improper grid positioning and most often occurs with parallel grids.
  • 90.
  • 91.
  • 92.
  • 93.  The quantity of scattered radiation in an x-ray beam reaching a receptor can be reduced by separating the patient's body and receptor surface, as shown below. This separation is known as an air gap. Scattered radiation leaving a patient's body is more divergent than the primary x-ray beam. Therefore, scattered radiation spreads out of the primary beam area. The reduction of scattered radiation in proportion to primary radiation increases with air-gap distance. Several factors must be considered when using this method of scatter reduction. Patient exposure is increased because of the inverse-square effect. The use of an air gap introduces magnification. Therefore, a larger receptor size is required to obtain the same patient area coverage. If the air gap is obtained by increasing the tube-to-receptor distance, the x-ray equipment must be operated at a higher output to obtain adequate receptor exposure.
  • 94.
  • 95.  A bucky is typically used for table or wall mounted x-raysystems and holds the x- ray cassette and grid. A bucky, is a device found underneath the exam table, a drawer like device that the cassette and grid is slid into before shooting x-ray.
  • 96.
  • 97.
  • 98.
  • 99.
  • 100.
  • 103.
  • 104.
  • 106.
  • 107.
  • 109.
  • 110.
  • 111.
  • 112.
  • 113. Oil in x-ray tube and HV Transformer for cooling and Insulation That is stable at high temperatures and has excellent electrical insulating properties Its functions are To insulate, suppress corona , Supress arcing, and to serve as a coolant.
  • 114.
  • 116. An AEC system uses a physically thin radiation An AEC system uses a physically thin radiation ionization detector "AEC detector" which is positioned between the patient being x-rayed and the x-ray film cassette. X-rays passing through the patient also pass through this "AEC detector" before they strike the x-ray film. A weak ionization signal from the AEC detector is integrated as a ramp shaped voltage waveform. This ramp signal rises until it matches a pre-set threshold. At this point the x-ray exposure is terminated. AEC devices are calibrated to ensure that similar exams have linearity in exam densities. This is due to the fact that a milliamperage station is no longer selected and instead relies upon the ionization within the selected chambers