The document discusses the interaction of X-rays with matter, including different types of interactions such as photoelectric effect, Compton scattering, and pair production. It outlines the atomic structure relevant to these processes and explains concepts like binding energy, ionization, excitation, and radiation effects on biological systems. Additionally, it addresses the differential absorption of X-rays in medical imaging and the deterministic and stochastic effects of radiation exposure.
Introduction to X-ray interactions, types of atomic structures, and contents overview.
Details on atomic composition, atomic models, binding energy specific to the atom.
Details on atomic composition, atomic models, binding energy specific to the atom.
Definitions of ionization and excitation processes in atoms due to energy.
Different mechanisms of photon interaction with matter and the dual nature of light.
Coherent scattering, Compton scattering effects, and probabilities based on electron interactions.
Photoelectric effect essentials, advantages, disadvantages, and differential absorption details.
Pair production and photodisintegration, emphasizing their non-importance in diagnostic radiology. Photoelectric effect essentials, advantages, disadvantages, and differential absorption details.
Photoelectric effect essentials, advantages, disadvantages, and differential absorption details.
The concept of exponential attenuation of X-rays passing through tissue and its significance.
Deterministic effects of radiation, including acute lethality and local tissue damage.
Cytogenetic damage, stochastic effects, risk estimation methods, and radiation-induced malignancies.
Cytogenetic damage, stochastic effects, risk estimation methods, and radiation-induced malignancies.
ATOM
Matter is anythingthat occupies space , is made
up of atom which is composed of nucleon (i.e.
neutron and proton) and electron.
Neutrons are electrically neutral and protons have
positive charge ,both are found in nucleus.
Electrons are negatively charge and circulate
around the nucleus .
The Atomic numer (Z) is the no. of protons in the
nucleus , it is equal to the no. of electrons .
Total no. of protons and neutrons in the nucleus is
known as Mass number(A).
4.
ATOMIC STRUCTURE
According toBohr’s atomic model :
1. Positively charged nucleus surround and revolve by
the negatively charged electrons in a fixed orbits
2. Electron orbit shells are given the codes for
identification K,L,M,N, and so forth from closest to
nucleus to farthest from nucleus .
3. Maximum number of electrons that can exist in each
shell increases with increase in distance from the
nucleus i.e. 2n^2 where ‘n’ is the shell number .
6.
Binding energy
It isenergy acquired by the electrons due to
strong electrostatic pull of attraction by the
nucleus
Energy required to remove an electron from an
atom is called electron binding energy
It is unique for each shell of each element
It depend on the distance of an electron from
5ye nucleus i.e. inner shell electrons have high
binding energy than outer shell electron
Ionization
Removal of oneor more electrons form the neutral
atom leaving behind a positive ion .
Electromagnetic radiation with sufficient energy to
eject atomic electron is called ionizing radiation
9.
EXICITATION
Electrons of anatom move from inner shell to outer shell
when energy is supplied to neutral atom is called
excitation
Photon beam interctaction
Attenuation: removal of intensity of the radiation
when it passes through the matter
Absorption:transfer of energy from radiation to the
medium
Scattering :refers to change indirection of photons
Transmission : x ray energy that penetrate through
matter without any of above process
12.
DUAL NATURE OFLIGHT
X ray belongs to a group of radiation called
Electromagnetic radiation .
Electromagnetic radiation has dual characteristics i.e. it
comprises both particle and wave
Wave concept
Propagate through space in the form of wave
Waves of all type have wavelength and frequency
C = / . V Where v= frequency , /= wavelength, c=
speed of light
13.
Electromagnetic wave kogif fig
Wave theory of light explains phenomenon like
interference , diffraction, polarization and coherent
scattering
14.
Particle concept
When metalsurface is irradiated with light , an
electron is ejwcted
Depends on its energy( frequency) not its
intensity
The phenomenon of photoelectric effect and
compton effect is explained on the basis of light
consisting photons or quanta.
Gif of duality
15.
Interaction of xray with matter
x ray interacts with matter through 5 different
mechanism .
They are :
1. Coherent scattering
2. Compton scattering
3. Photoelectric scattering
4. Pair production
5. photodisintegration
16.
COHERENT SCATTERING
Incident xray energy below 10kev interacts with the
target atom causing it to become excited and release
the excess energy as a scattered x ray
Also called classical scattering or Thompson scattering
There are two types of coherent scattering
1. Thomson scattering
2. Rayleigh scattering
Scattered x ray is change in direction and wave length
is equal to that of the incident x ray and therefore equal
energy
No ionization occurs as no transfer of energy of occurs
/no ejection of the electrons .
It is little importance to the diagnostic radiology
COMPTON SCATTERING
Incident xray interact with the outer shell electron
target atom , thereby ionizing the atom .
Ejected electron is called Compton electron
Energy of Compton scattered x ray is equal to
difference between the energy of incident x ray and
ejected electron .
This reaction produces an ion pair , a positive atom
and a negative electron known as recoil electron
It contributes around 20% in diagnostic radiography
20.
Scatter photon hasless energy than the
incident photon .
Wavelength is longer than the incident
photon
Scatter photon undergo additional tissue
interaction
22.
Direction of scatterradiation
Scatter radiation travel in a new direction
depending upon deflection angle with the
electron.
It may be as great as 180 degree ( back
scattering )
I. Back scatter can cause artefacts ,such as
cassette strap image .
II. These photons pose major radiation hazard
to the staff ( especially during fluoroscopic
examination )
23.
Probabilty of occurrence
Mostlikely to occur
With outer shell electron and loosely bound electron
As x ray energy increases
Reduce probability of Compton effect
As atomic number of matter increases
No effect
As mass density of matter increase
More Compton scatter
24.
PHOTOELECTRIC EFFECT
• Incidentx ray interact with the innershell electron
and is fully absorbed thereby ejecting an electron
from its shell
• the ejected electron escapes with the KE equal to
difference between energy of incident x ray and the
binding energy of the electron.
26.
• Earned alberteinstein the 1921 nobel prize in physics .
• For low atomic number atom , photoelectron eject
with KE is equal to the energy of incident x ray .
• For high atomic number atom , KE of photoelectron is
proportionately lower in compared to binding energy
of target atom .
27.
The photoelectric effectyields
1. photo electron (-ve ion )
2.Positive atom(+ve ion)
3.Characteristic x ray
- •Energy of characteristics x ray are produces when
the void in the k-shell is filled by the subsequent
shell electrons , generally L- shell electrons .
•Energy of characteristics x ray is equal to the
difference of binding energy of both shells
• It acts as secondary radiation and contributes
nothing of diagnostic
Probabilty of occurrence
Incidentx ray must have energy equal or
greater than the binding energy of k shell
electron
Inversely proportional to the third power of x
ray energy
Directly proportional to the third power of
the atomic number of an atom.
31.
Advantages of photoelectriceffect
Contributes around 75% to the medical
imaging .
Does not produce scattered radiation
Enhances natural tissue contrast
I. Since the probability of interaction is proportional
to the third power of atomic number , it
magnifies the difference in tissue composed of
different atomic numbers
II. For example bone and soft tissue
32.
Disadvantage of photoelectric
Increasein patient radiation dose , since all
the energy of incident photon is absorbed by
the patient in the photoelectric interaction.
33.
Pair production
Production ofan electron and positron pair after
complete absorption of the x ray photon.
The energy equivalence of the mass of both
particle is equal of 0.51MeV
That’s why it only Occurs when incident photon
has energy of atleast 1.02MeV
Energy in excess of 1.02MeV is distributed
equally as a kinetic energy
It is unimportant in x ray imaging but is very
much of important in PET imaging in nuclear
imaging
Photodisintegration
X ray ofenergy greater than 10Mev escapes
interaction with the electron and nuclear
electrostatic field and absorbed directly by
the nucleus
nucleus is raised to excited state and emits
nucleon or nuclear fragments .
It does not occur in diagnostic radiology
DIFFERENTIAL ABSORPTION
• Xrays that undergo photoelectric interaction provides
diagnostic information as they do not reach the IR and
produces light areas
• whereas x ray transmitted through the patient without
interaction produces the dark areas of a radiograph
• this difference in absorption of x ray interacrion is called
Differential absorption .
• Both, x rays that are transmitted to the IR and that are
absorbed photoelectrically are equally important
• If all the x rays are transmitted then iimage would be
uniformly black and also if all the x ray photons are
absorbed then it will cause uniformly white . Neither of
cases are appreiciated in diagnostic radiology .
38.
• Differential absorptiondepends on following factors ;
1.Atomic number (Z)
2.Mass density
1. Atomic number
• Probabilty of an x ray undergoing photoelectric is
proportional the third power of At no. of the tissue and
inversely proportional to the third power of x ray energy
• So decrease in compton scattering is not as rapid as
photoelectric with increase in energy .
•
Contd ...
40.
2.Mass density
• Interactionof x ray with tissue is proportional to the
mass demsity of the tissue regardless of type of
interaction .
• Mass denity is quantity of matter per volume.
• We could image bone even if differential absorption
is not (Z) related because bone has higher mass
density than soft tissue .
42.
EXPONENTIAL ATTENUATION
When xray interact with any type of tissue ,
interaction occurs through any 5 mechanism but in
diagnostic radiology only 2 types of interaction are
important .
these interaction depend on atomic no of tissue
atoms , mass density and x ray energy.
The reduction in beam intensity after penetration
through a given thickness of tissue is called
attenuation i.e. they are reduced in number by a
certain percentage of each increment in thickness of
the tissue they go through
43.
Deterministic effect ofthe radiation
The effect which have threshold value below
which the effect doesn’t occur
Once the threshold value has been reach the
severity of an effect increase with radiation
dose
It includes
1. Acute radiation lethality
2. Local tissue damage
3. hematologic depression
4. Cytogenic depression
44.
Acute radiation lethality
sequenceof events followed by high
radiation exposure leading to death within
days or weeks is called acute radiation
syndrome .
Three lethal syndrome associated with acute
radiation lethality are ;
I. Prodromal period (immediate response )
II. Latent period ( no response )
III. Manifest illness ( haematologic, GI ,CNS syndrome )
Local tissue damage
skin
Dependson the intrinsic radiosensitivity , cell
proliferation and maturation .
Local tissues that are affected immediately
are skin, gonads and bone marrow
Damage to basal cells results in earliest
manifestation of radiation injury to the skin .
The resultant skin damage is seen as
erythema and desquamation
Gonads
Human gonads arecritically important target
and responds to doses as low as 100mGyt
Even such low dose can reduce the number of
spermatozoa in male testes and suppress
menstruation in female
Dose of approximately 2Gyt causes temporary
infertility and 5Gyt cause permanent infertility
Moderate such as 250mGy is sufficient to
cause genetic mutation
52.
Haemopoietic system
highly radiosensitivesystem ,consists of bone
marrow ,circulating blood and lymphoid tissue
Derived from pluripotent stem cells which
produce many stem cells like lymphocytes
,granulocytes ,thrombocytes ,erythrocytes.
Cytogenetic effects
Cytogenetic isthe study of cell ,particularly
cell chromosome .
Radiation induced chromosome aberrations
follow non threshold dose response
relationship
Radiation may damage chromosome by
following
i. chromatid deletion –single hit
ii. Dicentric / ring chromosome – multi hit
iii. Reciprocal translocation –multi hit
57.
Ring chromosome areproduced if two hits occur on the same
chromosome.
Dicentrics are produced when adjacent chromosome sustain
one hit amd recombine .
58.
It results inno loss of genetic material, simoly rearrangement
of genes in incorrect sequence .
59.
Stochastic effect
Effects ofradiation that may occur by chance
and are result of low dose delivered over a
long period of time
It follows linear ,non-threshold dose response
relationship
The principle stochastic effects are radiation
induced malignancy and genetic effects .
60.
Local tissue effects
Chronicirradiation of skin can result in severe
non-malignant changes such as development
of very callaused , discolored ,weathered
apperances in the skin
Even a low dose can produce chromosome
aberration that may not be visible even after
many years of exposure
61.
usually the radiationprotection guides are
based on the stochastic effects of radiation
and on linear non threshold dose relationship
Consequently the precise dose response
relationship are often not possible to
formulate .
hence, we resort Risk Estimates. They are :
1. Relative risk
2. Excess risk
3. Absolute risk
62.
1. Relative risk
Ifone observe a large population for stocjastic
radiation effects without having precise
knowledge of radiatiom dose which they are
exposed .
It is computed by comparing the number of
irradiated populations showing stochastic
effect by the number of unexposed population
showing the same stochastic effect
Relative risk =observed case /expected
cases
63.
2. Excess risk
Itis difference between observed risk and
expected risk
Observed risk-Expected risk =Excess risk
Leukemia is known to occur in non irradiated
population but if leukemia incidence in
irradiated population exceeds more than
expected then difference betn observed cases
and expected cases would be excess risk .
64.
3. Absolute risk
Ifat least two dose levels are known , it may
be possible to determine the possible risk
factors
It consist unit of case / population / dose
According to the National committee on
biological effects of Ionizing radiation , this
value is 8*10^2
This is the risk coefficient used by the scientist
to predict stochastic radiation response in
exposed populations
65.
Radiation Induced Malignancy
Allthe radiation induced malignancy follow
linear non threshold dose response
relationship expect the radiation induced skin
cancer
Radiation induced malignancy like leukemia
,cancer increases with the increase in
radiation dose
66.
References
Text book ofRadiology for Residents and
Technicians
Radiologic science for technologist