Radiation
What is radiation?
Radiation: is the transfer of energy in the form of
particles or waves.
Energy: the ability to do work (Force·Distance)
X-rays are
electromagnetic radiation. Electromagnetic
radiation is a form of pure energy which is carried by waves of
photons. Electromagnetic radiation is also known as light.
Visible light, Radio and X-rays are all forms
of electromagnetic radiation which vary in energy and
thereby wavelength and frequency as well (Figure 1-1).
Figure 1-1: Forms of Electromagnetic Radiation
Courtesy of Phil Rauch and Laura Smith, 2000
Ionizing Radiation
X-ray radiation contains more energy than ultraviolet, infrared,
radio waves, microwaves or visible light. X-ray radiation has
sufficient energy (>30 eV) to cause ionizations. An ionization is a
process whereby the radiation removes an outer shell electron from
an atom (Figure 1-2).
Figure 1-2: The Ionization Process
Alan Jackson, 2001
Non-ionizing radiation does not contain sufficient energy (30 eV)
to cause ionizations (Figure 1-3). While some non-ionizing radiation
can be harmful, the
ionization process is clearly able to
cause chemical changes in important changes to biologically
important molecules (e.g. DNA).
Figure 1-3: Non-Ionizing Radiations
Courtesy of Alan Jackson, 2001
X-ray Production
X-rays are produced when high velocity electrons are decelerated
(slowed or stopped) or by a nucleus of an atom especially by high
atomic number material, such as the tungsten target (anode) in a
X-ray tube. An electrically heated filament (cathode) within the
X-ray tube generates electrons that are accelerated from the
filament to the tungsten target by the application of a high voltage
to the tube. The energy gained by the electron is equal to the
potential difference (voltage) between the anode and cathode. This
electron energy is typically expressed in kilovolts (kV). The
accelerated electron interacts with the target (anode) nucleus. As
the electric field of the electron interacts with nucleus, the
electron releases energy in the form of X-rays. This method of of
x-ray production is called
bremsstrahlung or braking
radiation (Figure 1-4).
FIgure 1-4: X-ray Production (Bremstrahlung)
Courtesy of the University of Michigan Student
Chapter of the Health Physics Society
Since the degree of interaction of the accelerated electron with
the target nucleus can vary, the energy spectrum, or distribution of
energy, of the X-rays produced by the bremsstrahlung process is
continuous.
As smaller number of
characteristic x-rays are also
produced as excited electrons interact with the electrons of the
target atoms. The X-rays produced from this interaction, with a
given orbital electron, have a single specific energy (discrete)
instead of a continuous spectrum. Mammographic x-ray tubes are
designed to maximize characteristic production to optimize breast
tissue imaging. The amount of characteristic X-rays in a
fluoroscopy beam is relatively low.
The lower energy X-rays are absorbed within the X-ray tube. This
reduces the number of lower energy X-rays in the resultant spectrum
since the lower energy X-ray are less penetrating. The beam is
considered "harder" when there is more filtration. Most X-ray
manufacturers add filtration, commonly consisting of aluminum, since
lower energy X-rays do not contribute to images and add to patient
dose.
The resulting x-ray spectrum energy (Figure 1-5) is a mixture of
the characteristic and bremsstrahlung radiation, less the primarily
low energy X-rays absorbed by the X-ray tube (and added
filtration). The maximum energy of the X-ray produced is equal
to the maximum potential applied across the x-ray tube. This peak
X-ray energy is usually described with the unit
kVp (kilovolt
peak or kilovolt potential). The type of target anode, potential (kVp)
and added filtration produce a beam of a given "
quality"
which implies specific shape of an X-ray spectrum.
Figure 1-5: Simplified X-ray Spectrum
Alan Jackson, 2001
X-ray Machine Parameters
The
quantity of electron flow (
current) in the
X-ray tube is described in units of
milliamperes (mA). The
rate of X-ray production is directly proportional to the X-ray tube
current. Higher mA values indicate more electrons are striking the
tungsten target, thereby producing more X-rays. The voltage (
kVp)
primarily determines the maximum X-ray energy produced but also
influences the number of X-rays produced. Increasing the kVp
attracts more electrons from the filament increasing the rate of
X-ray production. However, this relationship is not directly
proportional but higher kVp setting will result in a substantial
increase in the number of X-rays produced. The total number of
X-rays produced at a set kVp depends directly on the product of the
mA and exposure time and is typically described in terms of mA-s or
mAs. Fluoroscopy is usually performed using 2 to 5 mA current at a
peak electrical potential of 75 to 125 kVp.
X-ray Production Efficiency and Heat Loading
The production of x-rays is a relatively inefficient process so
that only a small fraction of the energy imparted by the
decelerating electrons is converted into X-rays. The remaining
energy is converted to heat. Thus, the production and dissipation of
heat in the X-ray tube is a serious consideration. Thus, most x-ray
machines have rotating anodes to spread out the heat to prevent
anode melting. This is the reason why you can hear an X-ray machine
make noise. Most fluoroscopic x-ray machine anodes are primarily
based on tungsten due to tungsten's high melting point, excellent
heat transmission, and high atomic number. In spite of tungsten's
favorable qualities, with sufficiently high usage, X-ray production
is prevented by the system to protect the tube. Substantial
improvements have been recently made in the ability of fluoroscopic
X-ray equipment to remove waste heat and thereby maintain high beam
outputs.
Figure 1-6: Heat Production
Courtesy of: Phil Rauch and Laura Smith, 2000
Divergent Nature of X-ray Radiation
Once generated, the X-rays are emitted in all directions in a
uniform manner (
isotropically). The lead housing surrounding
the X-ray tube limits X-ray emission through a small opening or port
in the X-ray tube. The resulting primary beam of useful radiation is
shaped by additional lead shutters, or collimators, that can be
adjusted to provide different beam shapes or sizes.
Inverse-Square-Law (Radiation intensity with distance)
Since the initial beam travels in straight but divergent
directions, geometry in a three dimensional world dictates that the
radiation intensity will decrease with the inverse square of the
distance. Consequently, the number of X-rays traveling through a
unit area decreases with increasing distance. Likewise, radiation
level decreases with increasing distance since exposure is directly
proportional to the number of X-rays interacting in a unit area. The
intensity of the radiation is described by the inverse square law
equation:
Where X
A is the radiation exposure rate at distance D
A
compared with the exposure rate (X
B) at some other
distance (D
B).
This effect is shown graphically in Figure 1-7:
Figure 1-7: Inverse Square Law
Courtesy of Scott Sorenson, 2000
1-Meter Distance: 1,000 X-rays pass through a
unit area. The amount of X-rays per unit area is
1,000.
2-Meter Distance: With increasing distance, the
beam diverges to an area 4 times the original area.
The same 1,000 X-rays are evenly distributed
over the new area (4 times the original). Thus the
amount of X-rays per unit area is 250 or 1/4 the
original. The resulting radiation exposure is 1/4
less.
This relationship indicates that
doubling the distance from a
radiation source decreases the radiation level by a factor of four.
Conversely,
halving the distance, increases the radiation level
by a factor of four. Intelligent application of inverse square
law principles can yield significant reductions in both patient and
operator radiation exposures.
Example 1:
An operator normally stands 1 meter away from the patient during
cineangiography. The exposure rate at this point is 15 mrem/min
(this unit will be explained later) and total cineangiography time
is 2 min. What is the reduction should the operator stand 1.2 meters
away?
Solution 1:
The original exposure was 30 mrem (15 mrem/min for 2 min). The new
exposure would be:
A 31% percent reduction in radiation exposure is achieved in this
example.
X-rays Interactions with matter
X-rays have several fates as they traverse tissue. These fates fall
into 3 main categories (Figure 1-8):
Figure 1-8: X-ray Interaction-Imaging Considerations
Courtesy of Scott Sorenson, 2000
No interaction: X-ray passes completely throughtissue and
into the image recording device. Producing an image
Complete absorption: X-ray energy is completely absorbed
by the tissue. This produces radiation dose to the patient.
Partial absorption with scatter: Scattering involves a
partial transfer of energy to tissue, with the resulting scattered
X-ray having less energy and a different trajectory. This
interaction does not provide any useful information (degrades image
quality) and is the primary source of radiation exposure to staff.
X-ray Interaction with Matter
The probability of X-ray interaction is a function of tissue
electron density, tissue thickness, and X-ray energy (kVp). Electron
dense material like bone and contrast dye attenuates more X-rays
from the X-ray beam than less dense material (muscle, fat, air). The
differential rate of interaction provides the contrast that forms
the image.
Tissue Electron Density Interaction Effects:
As electron density increases, the interaction with X-rays
substantially increases. Higher atomic number materials have
increased electron density. Thus, bone, which is substantially
comprised of calcium, produces more attenuation, than tissue, which
is comprised of carbon, hydrogen and oxygen (all of which have a
lower electron density or atomic number than calcium). Thus, the
image of bone and soft tissue has
contrast, or difference,
between bone and soft tissue.
The concept of contrast and electron density X-ray interaction
can be shown in Figure 1-9.
Assume 1,000 X-rays strike the following body portions. The
number of X-rays reaching the recording media (film, TV monitor)
directly effect the image's brightness.
Figure 1-9: Electron Density and Image Contrast
Courtesy of Scott Sorenson, 2000
In this example, 900 X-rays are capable of penetrating the soft
tissue, while only 400 penetrate the bone (Higher electron density
compared with soft tissue). The contrast between the bone and soft
tissue is (900-400)/900 = 0.56.