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Radiobiology for the Radiologist, Hall, 7th ed




Chapter 1. Physics and Chemistry of
       Radiation Absorption


                                                                   2012.03.14

                                                                Dahoon Jung
                                                 Korea Cancer Center Hospital
Overview
• Introduction
• Types of Ionizing Radiations
    – Electromagnetic Radiations
    – Particulate Radiations
•   Absorption of X-rays
•   Direct and Indirect Action of Radiation
•   Absorption of Neutrons, Protons, and Heavy Ions
•   Summary of Pertinent Conclusions
Introduction
• 1895, Wilhelm Conrad Röntgen,
        “a new kind of ray”  X-rays
Introduction
• The first medical use of x-rays
   – Lancet, Jan 23, 1896.
   – To locate a piece of a knife in the backbone of a drunken sailor.


• The first recorded biologic effect of radiation was due to
  Becquerel.
   – Left a radium container in his vest pocket.
   – 2 weeks later, he found skin erythema and ulceration.
Introduction

• Radiobiology is the study of the action of
  ionizing radiations on living things.
Types of Ionizing Radiations
• The absorption of energy from radiation in biologic material may
  lead to excitation or to ionization.




                                              Ionizing radiation
• The energy dissipated per ionizing event is about 33 eV.
    – Enough to break a strong chemical bond.
    – Cf. The energy associated with a C=C bond is 4.9 eV.
• Classify ionizing radiations as either electromagnetic or particulate.
1. Electromagnetic Radiations
• Most experiments with biologic systems have involved x- or γ-rays,
  two forms of electromagnetic radiation.
• Do not differ in nature or in properties.
    – X-rays are produced extranuclearly.
    – γ-rays are produced intranuclearly.




• Everything that is stated about x-rays in this chapter applies equally
  well to γ-rays.
1. Electromagnetic Radiations
• X-rays as waves of electrical and magnetic energy.
• Velocity = c
• Wavelength = λ
• Frequency(the number of waves passing a fixed point per second) =
  ν

                λ
                                            λν = c
                                            c = 3 x 1010 cm/s
1. Electromagnetic Radiations
• Radio waves, radar, radiant heat, and visible light are forms of
  electromagnetic radiation.
    – same velocity, different frequency.  different Energy.   E = ℎν
1. Electromagnetic Radiations
• X-rays as streams of photons, or “packets” of energy.
   – Each energy packet equal to hν.
   – λÅ = 12.4/E(keV)
       • for example, x-rays with wavelengths of 0.1Å correspond to a photon E of
         124 keV.

• The concept of x-rays being composed of photons is
  very important in radiobiology.
   – Energy absorbed in living material is deposited unevenly in
     discrete packets.
   – The individual packets, each of which is big enough to break a
     chemical bond and initiate the chain of events that culminates in
     a biologic change.
1. Electromagnetic Radiations
• The critical difference between nonionizing and
  ionizing radiation is the size of the individual packets
  of energy, not the total energy involved.

   – Total body dose of about 4 Gy of x-rays given to a human is
     lethal in about 50% of the individuals exposed.
       • To 70kg, this dose is only about 67 cal.
       • A temperature rise of 0.002℃
       • In the form of heat, drinking one sip of warm coffee.


   – Electomagnetic radiations are usually considered ionizing if they
     have a photon energy in excess of 124 eV (λ = 10-6 cm).
2. Particulate Radiations
• Electrons, protons, α-particles, neutrons, negative π-
  mesons, and heavy charged ions.
• Electrons : small negatively charged Betatron
                  ,               .       or               .
     Linear accelerator
  widely used for cancer therapy.
2. Particulate Radiations
• Protons : Positively charged
                           , relatively     massive times
                                              (2000
  greater than that of an electron),           .
                                          cyclotron




• Major hazard to astronauts.
2. Particulate Radiations
• α-particles : nuclei of helium
                               atoms. 2 protons and 2
  neutrons. Net positivecharge. Also emitted during the
  decay heavy radionuclides(uranium and radium)
      of
2. Particulate Radiations
• Neutrons : mass similar to that of protons, no electrical charge
                                                              . Cannot
  be accelerated in an electrical device. Emitted as a by-product if
  heavy radioactive atoms undergo fission. Important component of
  space radiation and contribute significantly to the exposure of high-
  flying jetliners.
2. Particulate Radiations
•   Heavy charged particles :
    nuclei of elements, such as
    carbon, neon, argon, or even
    iron, that are positively
    charged because some or all
    of the planetary electrons have
    been stripped from them.

•   Can be produced in only a few
    specialized facilities.

•   Major hazard to astronauts on
    long missions.
Absorption of X-rays
• Radiation may be classified as directly or
  indirectly ionizing.

• All of the charged particles are directly ionizing.
   can disrupt the atomic structure of the
  absorber through which they pass directly and
  produce chemical and biologic changes.
Absorption of X-rays
• Electromagnetic radiations(x- and γ-rays)
  are indirectly ionizing.
  – Do not produce chemical and biologic
    damage themselves.
  – When absorbed in the material, they give up
    their energy to produce fast moving charged
    particles that in turn are able to produce
    damage.
Absorption of X-rays
• The process by which x-ray photons are
  absorbed depends on the energy of the
  photons and the chemical composition of
  the absorbing material.
  – At radiotherapy, the Compton process
    dominates.
Absorption of X-rays

            Energy lost fraction vary
            from 0% to 80%.

            On a statistical basis, the
            net result is the production
            of several fast electrons.
            - break vital chemical
            bonds  biologic damage.
Absorption of X-rays
• For photon energies, characteristic of diagnostic radiology, both
  Compton and photoelectric absorption process occur.

                                                 In the PE process,
                                                 the x-ray photon
                                                 interacts with a
                                                 bound electron in.

                                                  KE = ℎν – EB
Absorption of X-rays
• The vacancy left in the atomic shell as a
  result of the ejection of an electron.

• Filling by another electron from an outer
  shell or by a conduction electron from
  outside the atom.
    – Decrease of potential energy.
    – “Characteristic” electromagnetic radiation.
    – Cf) in soft tissue, 0.5 kV.(of little biologic
      consequence)
Absorption of X-rays
• The Compton and photoelectric absorption process differ
  in several respects that are vital in the application of x-
  rays to diagnosis and therapy.

• The mass absorption coefficient for the Compton
  process is independent of the atomic number of the
  absorbing material.
• The mass absorption coefficient for photoelectric
  absorption varies rapidly with atomic number Z (Z3).
Absorption of X-rays

                       High Z




     Low Z
Absorption of X-rays
• For radiotherapy, high-energy photons in the
  megavoltage range are preferred because the
  Compton process is overwhelmingly important.
  – The absorbed dose is about the same in soft tissue, muscle, and
    bone.
  – So that differential absorption in bone is avoided(the early days’
    problem in RT).
Absorption of X-rays
• Although the differences among the various absorption
  processes are of practical importance in radiology, the
  consequences for radiobiology are minimal.

• Whether the PE or the Compton process, much of the
  absorbed energy is converted to the kinetic energy of a
  fast electron.
Direct and Indirect action of radiation
• The biologic effects of radiation result principally from damage to
  DNA, which is the critical target.
Direct and Indirect action of radiation
              Free radical(atom or molecule with an unpaired orbital electron)




                                             Easily modified by chemical
                                             means-either protectors or
                                             sensitizers- unlike direct action




                                            Dominant in high LET
                                            (neutrons or α-particles)
   Radical cylinder
Direct and Indirect action of radiation
(a) Production of hydroxyl radicals (OH) by ionizing radiation,
(b) Cleavage reaction of the DNA-backbone after hydrogen abstraction at the C4'-atom
by the electrophilic, highly reactive hydroxyl radical.
Direct and Indirect action of radiation

• The period between the breakage of chemical
  bonds and the expression of the biologic effect may
  be hours, days, months, years, or generations,
  depending on the consequences involved.

   – Cell killing  hours to days later(when the damaged cell
     attempts to divide).
   – Oncogenic  may be delayed for 40 yrs.
   – Mutation in a germ cell  may not be expressed for many
     generations.
Absorption of Neutrons, Protons,
          and Heavy Ions
• In contrast to x-rays, neutrons interact not with the
  planetary electrons, but with the nuclei of the atoms that
  make up the tissue resulting in recoil protons.
Absorption of Neutrons, Protons,
         and Heavy Ions
• In the case of higher energy neutrons
  – “Spallation products”
Absorption of
Neutrons, Protons, and Heavy Ions
• Protons interact with both planetary electrons to ionize the atoms,
  and also interact with the nuclei of atoms to produce heavier
  secondary particles.
Absorption of Neutrons, Protons,
          and Heavy Ions
• For neutrons or heavy ions, the direct action assumes
  greater importance.


• The indirect effect involving free radicals is most easily
  modified by chemical means.
   – Radioprotective compounds are quite effective for x- and γ- rays,
     not for neutrons, α-particles, or heavier ions.
Summary of Pertinent Conclusions
X- and γ-rays are indirectly ionizing; the first step in their absorption is the
production of fast recoil electrons.

Neutrons are also indirectly ionizing; the first step in their absorption is the
production of fast recoil protons, α-particles, and heavier nuclear
fragments.


Biologic effects of x-rays may be caused by direct action(the recoil
electron directly ionizes the target molecule) or indirect action(the recoil
electron interacts with water to produce an OH·, which diffuses to the
target molecule).
Summary of Pertinent Conclusions

About two thirds of the biologic damage by x-rays is caused by
indirect action.


DNA radicals produced by both the direct and indirect action of
radiation are modifiable with sensitizers or protectors.



DNA lesions produced by high-LET radiations involve large
numbers of DNA radicals. Chemical sensitizers and protectors are
ineffective in modifying such lesions.
Summary of Pertinent Conclusions
The physics of the absorption process is over in 10-15 second
; the chemistry takes longer because the lifetime of the DNA radicals is
about 10-5 second
; the biology takes hours, days, or months for cell killing, years for
carcinogenesis, and generations for heritable effects.
• Thank you for listening.

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Chap1 physics and chemistry of radiation absorption

  • 1. Radiobiology for the Radiologist, Hall, 7th ed Chapter 1. Physics and Chemistry of Radiation Absorption 2012.03.14 Dahoon Jung Korea Cancer Center Hospital
  • 2. Overview • Introduction • Types of Ionizing Radiations – Electromagnetic Radiations – Particulate Radiations • Absorption of X-rays • Direct and Indirect Action of Radiation • Absorption of Neutrons, Protons, and Heavy Ions • Summary of Pertinent Conclusions
  • 3. Introduction • 1895, Wilhelm Conrad Röntgen, “a new kind of ray”  X-rays
  • 4. Introduction • The first medical use of x-rays – Lancet, Jan 23, 1896. – To locate a piece of a knife in the backbone of a drunken sailor. • The first recorded biologic effect of radiation was due to Becquerel. – Left a radium container in his vest pocket. – 2 weeks later, he found skin erythema and ulceration.
  • 5. Introduction • Radiobiology is the study of the action of ionizing radiations on living things.
  • 6. Types of Ionizing Radiations • The absorption of energy from radiation in biologic material may lead to excitation or to ionization. Ionizing radiation • The energy dissipated per ionizing event is about 33 eV. – Enough to break a strong chemical bond. – Cf. The energy associated with a C=C bond is 4.9 eV. • Classify ionizing radiations as either electromagnetic or particulate.
  • 7. 1. Electromagnetic Radiations • Most experiments with biologic systems have involved x- or γ-rays, two forms of electromagnetic radiation. • Do not differ in nature or in properties. – X-rays are produced extranuclearly. – γ-rays are produced intranuclearly. • Everything that is stated about x-rays in this chapter applies equally well to γ-rays.
  • 8. 1. Electromagnetic Radiations • X-rays as waves of electrical and magnetic energy. • Velocity = c • Wavelength = λ • Frequency(the number of waves passing a fixed point per second) = ν λ λν = c c = 3 x 1010 cm/s
  • 9. 1. Electromagnetic Radiations • Radio waves, radar, radiant heat, and visible light are forms of electromagnetic radiation. – same velocity, different frequency.  different Energy. E = ℎν
  • 10. 1. Electromagnetic Radiations • X-rays as streams of photons, or “packets” of energy. – Each energy packet equal to hν. – λÅ = 12.4/E(keV) • for example, x-rays with wavelengths of 0.1Å correspond to a photon E of 124 keV. • The concept of x-rays being composed of photons is very important in radiobiology. – Energy absorbed in living material is deposited unevenly in discrete packets. – The individual packets, each of which is big enough to break a chemical bond and initiate the chain of events that culminates in a biologic change.
  • 11. 1. Electromagnetic Radiations • The critical difference between nonionizing and ionizing radiation is the size of the individual packets of energy, not the total energy involved. – Total body dose of about 4 Gy of x-rays given to a human is lethal in about 50% of the individuals exposed. • To 70kg, this dose is only about 67 cal. • A temperature rise of 0.002℃ • In the form of heat, drinking one sip of warm coffee. – Electomagnetic radiations are usually considered ionizing if they have a photon energy in excess of 124 eV (λ = 10-6 cm).
  • 12. 2. Particulate Radiations • Electrons, protons, α-particles, neutrons, negative π- mesons, and heavy charged ions. • Electrons : small negatively charged Betatron , . or . Linear accelerator widely used for cancer therapy.
  • 13. 2. Particulate Radiations • Protons : Positively charged , relatively massive times (2000 greater than that of an electron), . cyclotron • Major hazard to astronauts.
  • 14. 2. Particulate Radiations • α-particles : nuclei of helium atoms. 2 protons and 2 neutrons. Net positivecharge. Also emitted during the decay heavy radionuclides(uranium and radium) of
  • 15. 2. Particulate Radiations • Neutrons : mass similar to that of protons, no electrical charge . Cannot be accelerated in an electrical device. Emitted as a by-product if heavy radioactive atoms undergo fission. Important component of space radiation and contribute significantly to the exposure of high- flying jetliners.
  • 16. 2. Particulate Radiations • Heavy charged particles : nuclei of elements, such as carbon, neon, argon, or even iron, that are positively charged because some or all of the planetary electrons have been stripped from them. • Can be produced in only a few specialized facilities. • Major hazard to astronauts on long missions.
  • 17. Absorption of X-rays • Radiation may be classified as directly or indirectly ionizing. • All of the charged particles are directly ionizing.  can disrupt the atomic structure of the absorber through which they pass directly and produce chemical and biologic changes.
  • 18. Absorption of X-rays • Electromagnetic radiations(x- and γ-rays) are indirectly ionizing. – Do not produce chemical and biologic damage themselves. – When absorbed in the material, they give up their energy to produce fast moving charged particles that in turn are able to produce damage.
  • 19. Absorption of X-rays • The process by which x-ray photons are absorbed depends on the energy of the photons and the chemical composition of the absorbing material. – At radiotherapy, the Compton process dominates.
  • 20. Absorption of X-rays Energy lost fraction vary from 0% to 80%. On a statistical basis, the net result is the production of several fast electrons. - break vital chemical bonds  biologic damage.
  • 21. Absorption of X-rays • For photon energies, characteristic of diagnostic radiology, both Compton and photoelectric absorption process occur. In the PE process, the x-ray photon interacts with a bound electron in. KE = ℎν – EB
  • 22. Absorption of X-rays • The vacancy left in the atomic shell as a result of the ejection of an electron. • Filling by another electron from an outer shell or by a conduction electron from outside the atom. – Decrease of potential energy. – “Characteristic” electromagnetic radiation. – Cf) in soft tissue, 0.5 kV.(of little biologic consequence)
  • 23. Absorption of X-rays • The Compton and photoelectric absorption process differ in several respects that are vital in the application of x- rays to diagnosis and therapy. • The mass absorption coefficient for the Compton process is independent of the atomic number of the absorbing material. • The mass absorption coefficient for photoelectric absorption varies rapidly with atomic number Z (Z3).
  • 24. Absorption of X-rays High Z Low Z
  • 25. Absorption of X-rays • For radiotherapy, high-energy photons in the megavoltage range are preferred because the Compton process is overwhelmingly important. – The absorbed dose is about the same in soft tissue, muscle, and bone. – So that differential absorption in bone is avoided(the early days’ problem in RT).
  • 26. Absorption of X-rays • Although the differences among the various absorption processes are of practical importance in radiology, the consequences for radiobiology are minimal. • Whether the PE or the Compton process, much of the absorbed energy is converted to the kinetic energy of a fast electron.
  • 27. Direct and Indirect action of radiation • The biologic effects of radiation result principally from damage to DNA, which is the critical target.
  • 28. Direct and Indirect action of radiation Free radical(atom or molecule with an unpaired orbital electron) Easily modified by chemical means-either protectors or sensitizers- unlike direct action Dominant in high LET (neutrons or α-particles) Radical cylinder
  • 29. Direct and Indirect action of radiation (a) Production of hydroxyl radicals (OH) by ionizing radiation, (b) Cleavage reaction of the DNA-backbone after hydrogen abstraction at the C4'-atom by the electrophilic, highly reactive hydroxyl radical.
  • 30. Direct and Indirect action of radiation • The period between the breakage of chemical bonds and the expression of the biologic effect may be hours, days, months, years, or generations, depending on the consequences involved. – Cell killing  hours to days later(when the damaged cell attempts to divide). – Oncogenic  may be delayed for 40 yrs. – Mutation in a germ cell  may not be expressed for many generations.
  • 31. Absorption of Neutrons, Protons, and Heavy Ions • In contrast to x-rays, neutrons interact not with the planetary electrons, but with the nuclei of the atoms that make up the tissue resulting in recoil protons.
  • 32. Absorption of Neutrons, Protons, and Heavy Ions • In the case of higher energy neutrons – “Spallation products”
  • 33. Absorption of Neutrons, Protons, and Heavy Ions • Protons interact with both planetary electrons to ionize the atoms, and also interact with the nuclei of atoms to produce heavier secondary particles.
  • 34. Absorption of Neutrons, Protons, and Heavy Ions • For neutrons or heavy ions, the direct action assumes greater importance. • The indirect effect involving free radicals is most easily modified by chemical means. – Radioprotective compounds are quite effective for x- and γ- rays, not for neutrons, α-particles, or heavier ions.
  • 35. Summary of Pertinent Conclusions X- and γ-rays are indirectly ionizing; the first step in their absorption is the production of fast recoil electrons. Neutrons are also indirectly ionizing; the first step in their absorption is the production of fast recoil protons, α-particles, and heavier nuclear fragments. Biologic effects of x-rays may be caused by direct action(the recoil electron directly ionizes the target molecule) or indirect action(the recoil electron interacts with water to produce an OH·, which diffuses to the target molecule).
  • 36. Summary of Pertinent Conclusions About two thirds of the biologic damage by x-rays is caused by indirect action. DNA radicals produced by both the direct and indirect action of radiation are modifiable with sensitizers or protectors. DNA lesions produced by high-LET radiations involve large numbers of DNA radicals. Chemical sensitizers and protectors are ineffective in modifying such lesions.
  • 37. Summary of Pertinent Conclusions The physics of the absorption process is over in 10-15 second ; the chemistry takes longer because the lifetime of the DNA radicals is about 10-5 second ; the biology takes hours, days, or months for cell killing, years for carcinogenesis, and generations for heritable effects.
  • 38. • Thank you for listening.