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OER, LET and RBE Presented By: Dr. Vandana Dept. of Radiotherapy CSMMU, Lucknow
Oxygen Enhancement Ratio (OER) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
OER ,[object Object],[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
Nature of the Oxygen Effect 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Surviving Fraction Cells are much more sensitive to x-rays in the presence of molecular oxygen than in its absence (i.e., under hypoxia). The ratio of doses under hypoxic to aerated conditions necessary to produce the same level of cell killing is called the oxygen enhancement ratio (OER).
Oxygen Effect 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow ,[object Object],[object Object],[object Object]
Oxygen Fixation 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow CH 3 functional  group  CH 2 • free radical, unpaired electron  Generally, the free-radical reactions go like this: CH 2 • + O 2 CH 2 O 2  an organic peroxide “fixes” the indirect damage ion pairs free radicals (oxygen has no impact on  direct  damage)
Radio-sensitivity and O 2  Concentration ,[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Fig:  The dependence of radio-sensitivity on oxygen concentration
OER Effect ,[object Object],[object Object],[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Low-LET radiation
Other Radiations and the OER 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow ,[object Object],[object Object],High-LET radiation Dose, Gy 0.001 0.1 0.01 1.0 1.0 2.0 0 3.0 Dose, Gy    particles OER = 1.0 0.1 1.0 0 6 2 4 OER = 1.6 15 MeV Neutrons Hypoxic Aerated
Linear Energy Transfer (LET) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
LET ,[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
[object Object],[object Object],[object Object],[object Object],dispersion of energy low LET (  , x, ~  ) high LET (  , n, p) air tissue incident radiation greater radiotoxicity LET = linear energy transfer
Typical LET values 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Radiation   Linear Energy Transfer  ( keV/ µ m )   Cobalt-60  γ -rays   0.2   250-kV x-rays   2.0   10-MeV protons   4.7   150-MeV proton   0.5   14-MeV neutrons Track Avg. 12   Energy Avg. 100 2.5-MeV  α -particles   166   2-GeV Fe ions (space radiation )   1000  
The Optimal LET 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow ,[object Object],[object Object],[object Object]
Effect of LET on cell survival Fig:  Survival curves for cultured cells of human origin exposed to 250-kV X-rays,15-MeV neutrons, and 4-MeV alpha-particles. As the LET of the radiation increases, the survival curve changes: the slope of the survival curves gets steeper and the size of the initial shoulder gets smaller.
09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow ,[object Object],[object Object],[object Object],OER and LET
Relative Biologic Effectiveness (RBE) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
RBE In comparing different type of radiations , x-rays are used as the standard. Relative Biologic Effectiveness (RBE) of radiation  for producing a given biological effect  is given as below: Dose in Gy from 250 KeV X-rays  Dose in Gy from another radiation source  to produce the same biologic response RBE   =
RBE ,[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
Factors that determine RBE ,[object Object],[object Object],[object Object],[object Object]
Biologic system or endpoint ,[object Object],[object Object],[object Object]
RBE for different cells and tissues Figure below illustrates the difference in intrinsic radiosensitivity among various types of cells: ,[object Object],[object Object],[object Object],[object Object]
End Point ,[object Object],[object Object],[object Object],To measure the RBE of some test radiation, one first choose a biological system in which the effect of radiations may be scored quantitatively as well as choose an end point. For Example:  If We are measuring the RBE of fast neutrons compared with 250-kV X-rays, using the lethality of plant seedlings as a test system, groups of plants are exposed to a range of either X-rays or neutron doses. Note:  LD 50  is dose of radiation that result in death of half of the plants in a group.
Figure:   shows survival curves obtained if  mammalian cells in culture are exposed to a range of doses of either fast neutrons or 250-kV X-rays.  For surviving fraction of .01,  RBE =(10 Gy dose of x-rays)/ (6.6 Gy dose of neutrons)  =  1.5 For surviving fraction of 0.6,  RBE =(3 Gy dose of x-rays)/ (1Gy dose of neutrons)  =  3.0 Because the X-rays and neutron survival curves have different shapes, the X-ray survival curve having an initial shoulder and the neutron curve being an exponential function of dose, the resultant RBE depends on the level of  dose chosen.
Dose Level and fractionated doses For a surviving fraction of 0.01 the  RBE  for neutrons relative to X-rays is 2.6 (was 1.5 at single exposure). This is direct consequence of larger shoulder of x-ray curve.  The width of the shoulder represents a part of the dose that is “ wasted ”;  the larger the  number of fractions, the greater the extent of the wastage . Neutrons curve-almost no  shoulder. Net result is that neutrons become progressively more efficient than x-rays as the dose per fraction is reduced and the number of fraction is increased. The RBE generally increases as the dose is decreased.  The RBE for a fractionated regimen with neutrons is greater than for a single exposure, because a fractionated schedule consists of a number of small doses and the  RBE is large for small doses . Fractionation of radiation dose increases cell survival
The lower the dose rate, the higher the survival. RBE as a function of dose rate RBE can vary with the dose rate because the slope of the dose-response curve for sparsely ionizing radiations, such as x- or γ-rays, varies critically with a changing dose rate. In contrast, the biologic response to densely ionizing radiations depends little on the rate at which the radiation is delivered.
RBE as a function of LET ,[object Object],[object Object],[object Object],[object Object]
In the case of sparsely ionizing X-rays the probability of a single track causing a  DSB is low, thus X-rays have a low RBE. At the other extreme, densely ionizing radiations (ex. LET of 200 keV/  μm) readily produce DSB, but energy is “wasted” because the ionizing events are too close together. Thus, RBE is lower than  optimal LET radiation.
OER & RBE as a function of LET ,[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Variation of the OER and the RBE as a function of LET. The two curves are virtually mirror image of each other. The optimal RBE and the rapid fall of OER occur at about the same LET value, 100 keV/µm
Conclusion ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
09/13/11 Thank You

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LET, RBE & OER - dr vandana

  • 1. OER, LET and RBE Presented By: Dr. Vandana Dept. of Radiotherapy CSMMU, Lucknow
  • 2. Oxygen Enhancement Ratio (OER) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
  • 3.
  • 4. Nature of the Oxygen Effect 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Surviving Fraction Cells are much more sensitive to x-rays in the presence of molecular oxygen than in its absence (i.e., under hypoxia). The ratio of doses under hypoxic to aerated conditions necessary to produce the same level of cell killing is called the oxygen enhancement ratio (OER).
  • 5.
  • 6. Oxygen Fixation 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow CH 3 functional group CH 2 • free radical, unpaired electron Generally, the free-radical reactions go like this: CH 2 • + O 2 CH 2 O 2  an organic peroxide “fixes” the indirect damage ion pairs free radicals (oxygen has no impact on direct damage)
  • 7.
  • 8.
  • 9.
  • 10. Linear Energy Transfer (LET) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
  • 11.
  • 12.
  • 13. Typical LET values 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow Radiation   Linear Energy Transfer ( keV/ µ m )   Cobalt-60 γ -rays   0.2   250-kV x-rays   2.0   10-MeV protons   4.7   150-MeV proton   0.5   14-MeV neutrons Track Avg. 12   Energy Avg. 100 2.5-MeV α -particles   166   2-GeV Fe ions (space radiation )   1000  
  • 14.
  • 15. Effect of LET on cell survival Fig: Survival curves for cultured cells of human origin exposed to 250-kV X-rays,15-MeV neutrons, and 4-MeV alpha-particles. As the LET of the radiation increases, the survival curve changes: the slope of the survival curves gets steeper and the size of the initial shoulder gets smaller.
  • 16.
  • 17. Relative Biologic Effectiveness (RBE) 09/13/11 Presented by: Dr. Vandana, CSMMU, Lucknow
  • 18. RBE In comparing different type of radiations , x-rays are used as the standard. Relative Biologic Effectiveness (RBE) of radiation for producing a given biological effect is given as below: Dose in Gy from 250 KeV X-rays Dose in Gy from another radiation source to produce the same biologic response RBE =
  • 19.
  • 20.
  • 21.
  • 22.
  • 23.
  • 24. Figure: shows survival curves obtained if mammalian cells in culture are exposed to a range of doses of either fast neutrons or 250-kV X-rays. For surviving fraction of .01, RBE =(10 Gy dose of x-rays)/ (6.6 Gy dose of neutrons) = 1.5 For surviving fraction of 0.6, RBE =(3 Gy dose of x-rays)/ (1Gy dose of neutrons) = 3.0 Because the X-rays and neutron survival curves have different shapes, the X-ray survival curve having an initial shoulder and the neutron curve being an exponential function of dose, the resultant RBE depends on the level of dose chosen.
  • 25. Dose Level and fractionated doses For a surviving fraction of 0.01 the RBE for neutrons relative to X-rays is 2.6 (was 1.5 at single exposure). This is direct consequence of larger shoulder of x-ray curve. The width of the shoulder represents a part of the dose that is “ wasted ”; the larger the number of fractions, the greater the extent of the wastage . Neutrons curve-almost no shoulder. Net result is that neutrons become progressively more efficient than x-rays as the dose per fraction is reduced and the number of fraction is increased. The RBE generally increases as the dose is decreased. The RBE for a fractionated regimen with neutrons is greater than for a single exposure, because a fractionated schedule consists of a number of small doses and the RBE is large for small doses . Fractionation of radiation dose increases cell survival
  • 26. The lower the dose rate, the higher the survival. RBE as a function of dose rate RBE can vary with the dose rate because the slope of the dose-response curve for sparsely ionizing radiations, such as x- or γ-rays, varies critically with a changing dose rate. In contrast, the biologic response to densely ionizing radiations depends little on the rate at which the radiation is delivered.
  • 27.
  • 28. In the case of sparsely ionizing X-rays the probability of a single track causing a DSB is low, thus X-rays have a low RBE. At the other extreme, densely ionizing radiations (ex. LET of 200 keV/ μm) readily produce DSB, but energy is “wasted” because the ionizing events are too close together. Thus, RBE is lower than optimal LET radiation.
  • 29.
  • 30.
  • 31.