physical interaction of x ray with matter

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  • The smaller the field larger the escape angle.
  • physical interaction of x ray with matter

    1. 1. PRESENTATION BY: DR. CHARUSMITA CHAUDHARY
    2. 2. Dual characteristics of X-rays X-rays belong to a group of radiation called electromagnetic radiation . Electromagnetic radiation has dual characteristic, comprises of both  Wave  Particle Wave concept : Propagated through space in the form of waves. Waves of all types have associated wavelength and frequency Relationship : c=λν. c=velocity of light λ=wavelength ν=frequency The wavelength of diagnostic X-rays is very short around 0.1 to 1A. Wave concept explains why it can be reflected.
    3. 3.  Particle concept of EM radiation: Short EM waves such as X- rays predominantly react with matter as if they were particles rather than waves. At high frequencies electrons interact with EM radiation as if the EM radiation were an energy bundle. These particles are actually discrete bundles of energy and each of these bundles is called a quantum or photon. Particle concept used to describe interaction between radiation & matter .The amount of energy carried by each quantum is given by E=h ν E=photon’s energy h=planck’s constant ν =frequency c= νλ or ν=c/λ so substituting c/ λ for ν we get E=hc/ λ h=4.13x 10-18 keV/sec c=3 x 108 m/sec E=12.4E=Energy in keV. λ=wavelength in A0
    4. 4. METHODS OF INTERACTIONS Photons : absorbed / scattered. Attenuation : Reduction of intensity. Difference in attenuation gives the radiographic image. Absorbed : completely removed from the x-ray beam & cease to exist. Scattered : Random course. No useful information. No image only darkness. Adds noise to the system. Film quality affected : “film fog”. About 1% of the x rays that strike a patients body emerge from the body to produce the final image. The radiographic image is formed on a radiographic plate that is similar to the film of a camera. Remaining 99% of the x-rays --- Scattered / Absorbed.
    5. 5. ATOMIC STRUCTUREX-ray photons may interact either with orbital electrons or with the nucleus. In the diagnostic energy range, the interactions are always with orbital electrons.The molecular bonding energies ,however are too small to influence the type and number of interactions .The most important factor is the atomic make up of a tissue and not its molecular structure.
    6. 6. Atomic structure Basic structure of an ATOM : PROTON ( +ve charge ) An atom is made up of NUCLEUS NEUTRON ( neutral ) ORBITAL ELECTRONS ( -ve charge ) ORBITS / SHELLS ( K, L, M, N etc. ) K shell : 2 electrons L shell : 8 electrons Each shell has a specific binding energy & closer the shell is to the nucleus, the tighter it is bound to the nucleus. The electrons in the outermost shell are loosely bound to the nucleus & are hence called “free electrons”.
    7. 7.  Energy value of electronic shells is also determined by the atomic number of the atom. K-shell electron are more tightly bound in elements of high atomic number. Pb : 88keV while Ca : 4keV. Electrons in the K -shell are at a lower energy level than electrons in the L-shell. If we consider the outermost electrons as free ,than inner shell electrons are in energy debt. The energy debt is greatest when they are close to nucleus in an element with a high atomic number.
    8. 8. BASIC INTERACTIONS BETWEEN X-RAYS AND MATTER There are 12 mechanism, out of which five basic ways in which an x-ray photon may interact with matter. These are :Broadly classified on the basis of- A: PHOTON B: PHOTON DISAPPEARANCE SCATTERING: - PHOTOELECTRIC - COHERENT EFFECT SCATTERING - PAIR - COMPTON PRODUCTION SCATTERING - PHOTODISINTEGR ATION
    9. 9. 1. COHERENT SCATTERING Radiation undergoes Only Change in direction. No change in wavelengththats why sometime called “ unmodified scattering”Coherent scattering of X-rays is an interaction of the wavetype in which the X-ray is deflected.Coherent Scattering occurs mainly at low energies.It is oftwo types :Both type described in terms of “ wave Particle Interaction” ( also called “ Classical scattering”)  Thomson scattering : Single electron involved in the interaction.  Rayleigh scattering : Co-operative interaction of all the electrons.
    10. 10. 1. COHERENT SCATTERINGWhat happens in coherent scattering ? Low energy radiation encounters electrons Electrons are set into vibration Vibrating electron, emits radiation. Atom returns to its undisturbed state Fig : Rayleigh scattering
    11. 11. 1. COHERENT SCATTERING No ionization --- why??? because, no energy transfer. Only change of direction. Only effect is to change direction of incident photon. Less than 5%. Not important in diagnostic radiology. Produces scattered radiation but of negligible quantity.
    12. 12. 2. PHOTOELECTRIC EFFECT What happens in Photoelectric effect ? An incident PHOTON encounters a K shell electron and ejects it from the orbit The photon disappears, giving up ( nearly) all its energy to the electron The electron ( now free of its energy debt) flies off into space as a photoelectron carrying the excess energy as kinetic energy. The K shell electron void filled immediately by another electron and hence the excess energy is released as CHARACTERISTIC RADIATION. The atom is ionised.
    13. 13. PHOTOELECTRIC EFFECT
    14. 14. Percentage of photoelectric reactionsRadiation Water Compact Sodiumenergy(keV) bone iodide20 65 89 9460 7 31 95100 2 9 88
    15. 15. CHARACTERISTIC RADIATIONCharacteristic radiation generated by the photoelectric effect is exactly the sameThe only difference in the modality used to eject the inner shell electron. In x ray tube a high speed electron ejects the bound electron, while In photoelectric effect an X ray photon does the trick. In both casesthe atom is left with an excess of energy = the binding energy of an ejected electron Usually referred to as Secondary Radiation to differentiate It from scatter radiation…… End result is same for both, “A Photon that is deflected from its original path”
    16. 16. Characteristic radiation How does this happen ? After the electron has been ejected, the atom is left with a void in the K shell & an excess of energy equivalent to the binding energy. This state of the atom is highly unstable & to achieve a low energy stable state ( as all physical systems seek the lowest possible energy state ) an electron immediately drops in to fill the void. As the electron drops into the K shell, it gives up its excess energy in the form of an x-ray photon. The amount of energy released is characteristic of each element & hence the radiation produced is called Characteristic radiation.
    17. 17. 2. PHOTOELECTRIC EFFECT Thus the Photoelectric effect yields three end products :  Characteristic radiation  A -ve ion ( photoelectron )  A+ve ion (atom deficient in one electron )
    18. 18. 2. PHOTOELECTRIC EFFECTProbability of occurrence : The incident photon energy > binding energy of the electron. Photon energy similar to electron binding energy Photoelectric effect  1 (energy)³ The probability of a reaction increases sharply as the atomic no. increases Photoelectric effect  (atomic no.)³
    19. 19.  Low atomic number : interaction mostly at the K shell. High atomic number : interaction mostly at L and M shell. In summary, Photoelectric reactions are most likely to occur with low energy photons and elements with high atomic numbers provided the photons have sufficient energy to overcome the forces binding the electrons in their cells.
    20. 20. For eg : I2K shell :33.2keVL-shell : 4.9keVM shell 0.6 Kev.From L-shell to K-shell a 28.3 kev(33.2-4.9=28.3) keV photonis released.The void in the L-shell is then filledwith a photon fromthe M shell with theproduction of a ( 4.9-0.6 KeV)4.3 keVphoton.
    21. 21. K-shell electron binding energies of elements important indiagnostic radiologyAtom Atomic number K-shell binding energy(keV)Calcium 20 4.04Iodine 53 33.2Barium 56 37.4Tungsten 74 69.5Lead 82 88.O
    22. 22. 2. PHOTOELECTRIC EFFECT :Applications in diagnostic radiology : Disadvantage: Advantages :  Maximum radiation exposure. Excellent radiographic images :  No scatter radiation.  All the energy is absorbed by the patient whereas in other reactions only part of the incident photon’s  Enhances natural tissue energy is absorbed. contrast. Depends on 3rd power of the atomic no., so it magnifies the difference in tissues composed of different elements, such as bone & soft tissue  Lower energy photons : total absorption. Dominant upto 500 keV.
    23. 23. 3. COMPTON EFFECT The Compton effect occurs when the incident x-ray photon with relatively high energy ejects an electron from an atom and a x-ray photon of lower energy is scattered from the atom.The reaction produces an ion pair A +ve atom A –ve electron ( recoil electron )
    24. 24. COMPTON SCATTERINGAlmost all the scatter radiation that we encounteredIn diagnostic radiology comes from Compton Scattering
    25. 25. 3. COMPTON EFFECT Kinetic energy of recoil electron Energy of photon distributed Retained by the deflected photon. Two factors determine the amount of energy the photon transmits :  The initial energy of the photon.  Its angle of deflection. 1.Initial energy :- Higher the energy more difficult to deflect. High energy : Travel straight retaining most of the energy. Low energy : Most scatter back at angle of 180º 2. Angle of deflection :- Greater the angle, lesser the energy trasmitted. With a direct hit, maximum energy is transferred to the recoil electron. The photon retains some energy & deflects back along its original path at an angle of 180º.
    26. 26. ENERGY OF COMPTON SCATTERED PHOTONSThe change in wavelength of a scattered photon is calculated as : Δλ = 0.024 ( 1 – cos θ ) , where Δλ = change in wavelength θ = angle of photon deflection
    27. 27. 3. COMPTON EFFECTProbability of occurence : It depends on :-  Total number of electrons : It further depends on density and number of electrons per gram of the absorber. All elements contain approx. the same no. of electrons per gram, regardless of their atomic no. Therefore the no. of Compton reactions is independent of the atomic no. of the absorber.  Energy of the radiation : The no. of reactions gradually diminishes as photon energy increases, so that a high energy photon is more likely to pass through the body than a low energy photon.Two subsequent points should also be noted: Firstly, the photoelectron can cause ionizations along its track. Secondly, X-ray emission can occur when the vacancy left by the photoelectron is filled by an electron from an outer shell of the atom.
    28. 28. 3. COMPTON EFFECTDisadvantages of Compton reaction : Scatter radiation : Almost all the scatter radiation that we encounter in diagnostic Radiology comes from Compton scattering. In the diagnostic energy range, the photon retains most of its original energy. This creates a serious problem, because photons that are scattered at narrow angles have an excellent chance of reaching an x- ray film & producing fog. Exceedingly difficult to remove – ► cannot be removed by filters because they are too energetic. ► cannot be removed by grids because of narrow angles of deflection. It is also a major safety hazard. Even after 90˚ deflection most of its original energy is retained. Scatter radiation as energetic as the primary radiation. Safety hazard for the radiologist, personnel and the patient.
    29. 29. 4. PAIR PRODUCTIONNo importance in diagnostic radiology.What happens in Pair production ?A high energy photon interacts with the nucleus of an atom.The photon disappears & its energy is converted into matter in the formof two particles  An electron  A positron (particle with same mass as electron, but with +ve charge.)Mass of one electron is 0.51 MeV.2 electron masses are produced.So the interaction cannot take place with photon energy less than 1.02 MeV.
    30. 30. 4. PAIR PRODUCTION Positron annihilation. What happens to the Positron ? Slowly moving Positron combines with a free electron to produce two photons of radiation. 2 mass units are converted, giving a total energy of 1.022 MeV. To conserve momentum, two photons each with 0.511 MeV energy are ejected in opposite direction.
    31. 31. 5. PHOTODISINTEGRATION A photon with extremely high energy ( 7-15 MeV), interacts directly with the nucleus of an atom. May eject a neutron, proton or on rare occasions even an alpha particle. No diagnostic importance. We rarely use radiation >150 KeV in diagnostic radiology.What happens in Photodisintegration ? A high energy photon encounters the nucleus of an atom.Part of the nucleus which may be a neutron, a proton, an alpha particle or a cluster of particles, is ejected.
    32. 32. RELATIVE FREQUENCY OF BASIC INTERACTIONS Coherent scattering : About 5% . Minor role throughout the diagnostic energy range. Compton scattering : Dominant interaction in water. Water is used to represent tissues with low atomic nos. such as air, fat and muscle. Photoelectric reaction : usually seen in the contrast agents because of their high atomic numbers.  Bone is intermediate between water & the contrast agents. At low energies, Photoelectric reactions are more common, while at high energies, Compton scattering is dominant.
    33. 33. RELATIVE FREQUENCY OF BASIC INTERACTIONS
    34. 34. X-ray photon Photoelectric Compton scatter Pair production%energy absorption % % 10 keV 95 5 0 25 keV 50 50 0(Mammography 60 keV 7 93 0 (Diagnostic)150 keV 0 100 0 0 94 64 MeV10 MeV 0 77 23(Therapy)24 MeV 0 50 50
    35. 35. Scatter Radiation
    36. 36. Scatter Radiation Definition  A type of secondary radiation composed of photons of lower energy than the photons that produced them and which travel in a different direction.  The term scatter radiation is synonymous with secondary radiation in the context of x-rays
    37. 37. Scatter radiation & Contrast - overview  Radiographic images are maps of radiation attenuation. Bones attenuate the most, air in lungs the least.  Good radiograph : maximum contrast difference between different tissues. X-Ray beam enters body. Large number of interactions producing scatter radiation. Image contrast reduced depending on scatter radiation content reaching film.
    38. 38. CONTRAST REDUCTIONAssumed that the object shown here is not penetrated and would produce 100% contrast if no scatter radiation.
    39. 39. Sources of scattered radiation  Transmitted scatter constitutes greater portion of scattered radiation and originates from the patient under examination.  Scatter from cassette  Side scatter Side scatter originates from walls, or objects on the source side of the film  Reflection scatter or Back scatter It is often called backscatter when it comes from objects behind the film.  Undercut Undercut occurs due to scattering within the film
    40. 40. Factors affecting scatter radiation  Field size  Kilo voltage (kVp)  Anatomical volume (Part thickness)
    41. 41. Factors affecting scatter radiation Scatter radiation is maximum with high kvp technique, large field , and thick parts---- Unfortunately, this is what we usually deal with in diagnostic radiology. The only variable we can control is kvp , but we have less control .
    42. 42. Factors affecting scatter radiation Field Size  Most important factor in the production of scatter radiation.  A small x ray field usually called Narrow beam irradiates less tissue and generates fewer scattered photons.Contrast Improvement byReducing X-Ray Beam Size
    43. 43. Factors affecting scatter radiation Kvp The effect of kvp on the production of scatter radiation is probably not as important as part thickness , and as field size.
    44. 44. Factors affecting scatter radiationKvP Photoelectric Less Low Kvp effect scattering Higher Compton More Kvp effect scattering
    45. 45. Factors affecting scatter radiation  Part thickness  Scatter radiation is directly proportional to the part thickness.  The operator has no control over this parameter.
    46. 46. Effects of scatter radiation Reduction of contrast: Scattered photons  Carry no useful information  Contribute to film blackness(film fog) Increased patient dose Increased risk to personnel
    47. 47. Control of scatter radiationBackscatter : „B‟ is industrycode.Lead „B‟ behind cassette toassess backscatter.If the letter "B" shows as a"ghost" image on the film, asignificant amount ofbackscatter radiation isreaching the film.Control of backscatter radiationby : Backing film in thecassette with a sheet of leadthat is at least 0.010 inch thick.Industry practice : 0.005" leadscreen in front and a 0.010"screen behind the film.
    48. 48. Prevention of scatter radiationDifferent techniques are used to keep thescatter radiation from reaching the films.  X ray filters  X ray beam restrictors  Grids (most important)
    49. 49. SUMMARYOnly two interactions are important in diagnostic radiology, the Photoelectric effect & Compton scattering.  The Photoelectric effect is the predominant interaction with low energy radiation & high atomic no. absorbers. It generates no significant scatter radiation & produces high contrast in the x-ray image.  But, unfortunately it exposes the patient to a great deal of radiation. Compton scattering  is the most common interaction at higher diagnostic energies.  responsible for almost all scatter radiation.  radiographic image contrast is less compared to photoelectric effect.  Coherent scattering is numerically unimportant.  Pair production & Photodisintegration occur at energies above the useful energy range.
    50. 50. SUMMARY Scatter Radiation  secondary radiation composed of photons of lower energy than the photons that produced them and which travel in a different direction.  Factors affecting it :  Field size  Kilo voltage (kVp)  Anatomical volume (Part thickness)  No useful information, causes film fog and increases patient exposure.
    51. 51. Thank you Have A nice day THANK YOU

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