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QUANTITIES AND UNITS USED
IN RADIATION PROTECTION
H.LANILRANJITH
HEAD, DIVISION OFRADIATION PROTECTION
ATOMIC ENERGYAUTHORITY
QUANTITIES:
ARE MEASURABLE CHARACTETISTICS
Eg LENGTH, DOSE ETC.
UNITS
ARE USED TO DESCRIBE THE QUANTITY
Eg METERS, GRAYS ETC.
RADIATION UNITS
• TO MEASURE RADIOACTIVITY
• TO EXPRESS ENERGY OF
RADIATION EMITED
• TO EXPRESS AMOUNT OF
ENERGY DEPOSITED IN THE
BODY
• TO QUANTIFY BIOLOGICAL
DAMAGES TO IRIDIATED
TISSUES
ACTIVITY
• NO.OF
DESINTEGRATIONS
PRE SECOND
• 1Bq = 1 dis/s
• ORDER OF
MAGNITUDE
THE CURIE
1 Curie (Ci) = Activity of 1g of 226
Ra
1g of 226
Ra disintegrate 3.7x1010
atoms per second
∴ 1 Ci = 3.7 x 1010
dis/s
∴ 1 Ci = 3.7 x 1010
Bq
1 Ci = 37 GBq
ENERGY OF RADIATION
ELECTRON VOLTS
1eV = 1.6 X 10 –19
J
COBALT- 60 RADIOACTIVE MATERIAL
EMITS TWO GAMMA RADIATIONS OF
ENERGIES 1.17 MeV AND 1.32 MeV.
DOSE
USES AS A GENERIC TERM THAT CAN
APPLY TO ANY OF THE RELEVANT
DOSIMETRIC QUANTIES
EXPOSURE
IN A GENERIC SENSE TO MEAN THE
PROCESS OF BEING EXPOSED TO
RADIATION
Exposure Unit
•Is a measure of ionization produced in air
•Is used only for X and γ radiation
•Is valid for quantum energy less than 3 MeV
X Unit
1 X unit = 1 C/kg air
One exposure unit is defined as that quantity
of x or gamma radiation that produces in air,
ions carrying 1 coulomb of change( of either
sign) per kg air.
Exposure
Exposure is measured under conditions of electronic
equilibrium
For photon energies above about 3 MeV, the ranges of
secondary electrons become a significant fraction of
the photon attenuation lengths and the departure from
equilibrium may be significant
Thus, exposure is not defined above photon energies
of 3 MeV
Roentgens (2/3)
• Is symbolized by R
• was used as the exposure unit before
SI system was adopted
• is still being used.
Roentgen
Is defined as the quantity of x or
gamma radiation that produces ions
carrying one statcoulomb of charge of
either sign per cubic centimeter of air
at STP.
Charge of the electron=1.6x10-19
C =4.8x10-10sC
1C =3x109
sC
13
KERMA
KERMA (Kinetic Energy Released in a Material):
– Is the sum of the initial kinetic energies of all charged
ionizing particles liberated by uncharged ionizing
particles in a material of unit mass
– For medical imaging use, KERMA is usually expressed
in air
SI unit = joule per kilogram (J/kg)
or gray (Gy)
1 J/kg = 1 Gy
14
Mean absorbed dose in a tissue or
organ
The mean absorbed dose in a tissue or organ DT is the
energy deposited in the organ divided by the mass of
that organ.
ABSORBED DOSE(1/2)
• MEASURES THE ENERGY
DELIVERED TO ANY MATERIAL
• IN RADIATION PROTECTION
THE MATERIAL CONCERNED IS
THE TISSUE OR ORGAN OF THE
HUMAN BODY
ABSORBED DOSE(2/2)
• DEFINED AS THE
“ENERGY ABSORBED
PER UNIT MASS OF
ANY MATERIAL”
• UNIT USED
“GRAY” OR
“RADS”
1GRAY (Gy) = 1J/kg
1RADS = 100 ergs/g
100 RADS = 1 Gy
EQUIVALENT DOSE(1/2)
QUANTIFY THE BIOLOGICAL
DAMAGE TO THE ORGAN OR
TISSUE IRRIDIATED
The same dose levels of different radiations
(ie photons and neutrons) do not have the
same level of biological effect
Radiation weighting factor, wR
(related to radiation quality)
EQUIVALENT DOSE(2/2)
• BIOLOGICAL
EFFECTS OF AN
EXPOSURE ON A
ORGAN OR TISSUE
DEPEND ON:
• ENERGY TRANSMITTED
TO THE ORGAN OR
TISSUE BY RADIATION
• HAMFULNESS OF THE
TYPE OF RADIATION
INVOLVED (DEGREE OF
POWER OF IONIZATION)
Radiation weighting factors,
wR
1
Type and energy ranges
Radiation
weighting
factor, wR
1
1
5
10
20
10
5
5
Photons, all energies
Electrons and muons, all energies
Neutrons, energy < 10 keV
10 keV to 100 keV
100 keV to 2 MeV
> 2 MeV to 20 MeV
> 20 MeV
Protons, other than recoil protons, energy > 2 MeV
Alpha particles, fission fragments, heavy nuclei 20
1) All values relate to the radiation incident on the body, or,
for internal sources, emitted from the source.
Neutron radiation weighting
factors30
25
20
15
10
5
0
wR
Neutron energy - MeV
10-8
10-7
10-6
10-5
10-4
10-3
10-2
10-1
1 10 102
ICRP Recommendation
ICRP Approximation
EFFECTIVE DOSE
Different body tissues have different
biological sensitivities to the same
radiation type and dose
Tissue weighting factor, wT
EFFECTIVE DOSE
• MEASURES THE RISK OF
BIOLOGICAL DAMAGE TO
WHOLE BODY TAKING THE
RADIOSENSITIVITIES OF
TISSUE IRRIDIATED IN TO
ACCOUNT
• MEASURES THE RISK
REGARDLESS OF EXPOSURE
INVOLVED.( INTERNAL,
EXTERNAL, PARTIAL OR
TOTAL)
• MEASURES IN THE UNIT OF.
“SIEVERT”( Sv )
Roentgen (3/3)
1R = 0.0087 J/kg of air
IR = 0.0087 Gy = .87 Rad
IR = 0.0096 J/kg in Tissue
IR = 0.0096 Gy in Tissue
IR = .96 Rad in Tissue
1 R = 1 Rad
for x and γ rays
IR = 1 rem = .01 Sv
Multipliers of the equivalent dose to an organ or tissue to
account for the different sensitivities to the induction of
stochastic effects of radiation.
Tissue or organ wT Tissue or organ wT
Gonads 0.20 Bone marrow (red) 0.12
Colon 0.12 Lung 0.12
Stomach 0.12 Bladder 0.05
Breast 0.05 Liver 0.05
Oesophagus 0.05 Thyroid 0.05
Skin 0.01 Bone surface 0.01
Remainder 0.05 TOTAL 1.00
Tissue weighting factors
Committed Dose
Is a useful subsidiary dosimetric quality
to express dose to body during certain
time following an intake of radioactive
material to the body.
Note : The dose delivery to the body
during the above period is at
varying rates.
Committed Equivalent Dose
Defined as the time integral of the equivalent dose
rate and denoted by HT( τ )
τ = integration time in years following
the intake.
If t is not specified
Integration time is taken as
50 years for adults
70 years for children
Committed equivalent dose:
The quantity H(τ), defined as;
where to
is the time of intake, HT
(t) is the equivalent dose
rate at time t in an organ or tissue T and τ is the time elapsed
after an intake of radioactive substances.When τ is not
specified it will be taken to be 50 years for adults and to age
70 years for intakes by children.
( ) ( )H H t dtT
t
t
o
o
τ
τ
=
+
∫
.
Committed effective dose:
The quantity E(τ), defined as ;
where HT
(τ) is the committed equivalent dose to tissue T
over the integration time τ and WT
is the tissue weighting
factor for tissue T.
When τ is not specified it will be taken to be 50 years for
adults and to age 70 years for intakes by children.
( ) ( )E W HT T
T
τ τ= ∑ .
Collective Dose(1/2)
Is used to express dose to a
group or a population.
Takes account of the no of
people exposed to a source and
the average dose to the
individual.
COLLECTIVE DOSE(2/2)
DEFINED AS,
THE PRODUCT OF THE NUMBER OF
INDIVIDUAL EXPOSED TO A SOURCE AND
THEIR AVERAGE DOSE
UNIT: MAN SIEVERT (man Sv)
Is there
RADIATION
in this room?
Background Radiation
•Natural Background Radiation
•Background Radiation Due to
Man Made Sources.
NATURAL BACKGROUND
RADIATION
• TERRESTRIAL SOURCES
• EXTRA TERRESTRIAL SOURCES
( COSMIC RADIATION )
Natural sources of radiation…
(2.4 mSv.
y-1
)
Cosmic…
(0.4 mSv.
y-1
)
…from earth’s crust
(0.4 mSv.
y-1
)
…via ingestion
(0.3 mSv.
y-1
)
…via inhalation
(1.3 mSv.
y-1
)
C. Torudd ; Swedish Radiation Protection Institute
...internal
External terrestrial irradiation
0.4 mSv y-
Varies considerably with soil and rock type
Unusually high background in a few places
in e.g.
•Esperito Santos, Brazil
•Kerala, India
•Guandong province, China
Up to 50 µGy h-1
compared to 0.1 µGy h-1
External extra
terrestrial radiation
(Cosmic radiation)
Estimated spectrum
of secondary
particles in the
atmosphere from
cosmic radiation
Heinrich et al 1999 (0.4 mSv.
y-1
)
Cosmic radiation
Dose and ambient dose equivalent during a
flight from Bangkok to Copenhagen
External irradiation: Natural background
dose rates from external sources (mSv.
y-1
)
Internal irradiation
via inhalation, 1.2 mSv.
y-1
(mainly indoor radon)
Reasons for elevated levels of
indoor radon
•elevated levels of 238
U and 232
Th series in
the ground
•building material with elevated levels of
238
U and 232
Th series
•tight houses (cold climate…)
Internal irradiation
via ingestion
40
K
•abundance 0.0188% in potassium (K)
(0.15 mSv.
y-1
)
Also
•uranium and thorium series
(0.15 mSv.
y-1
)
Man-made Radiation
• Cigarette smoke
• Consumer products
– Building materials
– Smoke detectors
• Industrial use
• Medical use
• Nuclear power
• Nuclear fall out
…and artificial sources of
radiation
Medical examinations…
(0.4 mSv.
y-1
)
C. Torudd ; Swedish Radiation Protection Institute
…and more artificial sources of radiation
...and nuclear
weapons
(0.005 mSv.
y-1
atmospherical
tests)
Nuclear fuel
cycle…
(0.0002 mSv.
y-1
)
C. Torudd ; Swedish Radiation Protection Institute
Nuclear power
Nuclear weapons
© Chernobylinterninform 1996
Chernobyl accident, April, 1986
Practical concequencies of Chernobyl
accident
Effects of radiation and accident situation
•600,000-800,000 persons in cleaning up work
•Approximately 200,000 persons evacuated
•Large areas of land abandoned (30 km zone etc.)
Other effects:
•Cost estimated to 100 billion USD
Health concequencies of Chernobyl accident
Effects of radiation and accident situation
Seen:
•Immediate death of 30 persons
•1800 children diagnosed with thyroid cancer (1998)
Statistically:
•15,000 deaths in cancer (global)
Other factors influencing health:
•Poor food supply, social concequencies, anxiety
Source Mean effective dose (mSv)
Natural background 2,4
Medical examinations 0,4
Nuclear tests in the atmosphere 0,005
Chernobyl accident 0,002
Nuclear fuel cycle 0,0002
Individual exposure of the world’s population
due to ionising radiation, year 2000
UNSCEAR
DO WE NEED
RADIATION PROTECTION ?
Drinking Hot Coffee
Excess Temperature = 60º - 37 = 23º
1 sip= 3ml
3x 23= 69 calories
Lethal Dose= 4Gy
LD 50/60 = 4 Gy
For man of 70 kg
Energy absorbed = 4 x 70 = 280 Joules
= 280/418= 67 calories
= 1 sip
X-ray
We live with
1-3 mSv
Can kill
4000 mSv
Radiation
Where to stop, where is the safe point?
What are the effects of radiation?
What can radiation do?
Death
Cancer
Skin Burns
Cataract
Infertility
Genetic effects
Rp002 anil quantities1 l1

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Rp002 anil quantities1 l1

  • 1. QUANTITIES AND UNITS USED IN RADIATION PROTECTION H.LANILRANJITH HEAD, DIVISION OFRADIATION PROTECTION ATOMIC ENERGYAUTHORITY
  • 2. QUANTITIES: ARE MEASURABLE CHARACTETISTICS Eg LENGTH, DOSE ETC. UNITS ARE USED TO DESCRIBE THE QUANTITY Eg METERS, GRAYS ETC.
  • 3. RADIATION UNITS • TO MEASURE RADIOACTIVITY • TO EXPRESS ENERGY OF RADIATION EMITED • TO EXPRESS AMOUNT OF ENERGY DEPOSITED IN THE BODY • TO QUANTIFY BIOLOGICAL DAMAGES TO IRIDIATED TISSUES
  • 4. ACTIVITY • NO.OF DESINTEGRATIONS PRE SECOND • 1Bq = 1 dis/s • ORDER OF MAGNITUDE
  • 5. THE CURIE 1 Curie (Ci) = Activity of 1g of 226 Ra 1g of 226 Ra disintegrate 3.7x1010 atoms per second ∴ 1 Ci = 3.7 x 1010 dis/s ∴ 1 Ci = 3.7 x 1010 Bq 1 Ci = 37 GBq
  • 6. ENERGY OF RADIATION ELECTRON VOLTS 1eV = 1.6 X 10 –19 J COBALT- 60 RADIOACTIVE MATERIAL EMITS TWO GAMMA RADIATIONS OF ENERGIES 1.17 MeV AND 1.32 MeV.
  • 7. DOSE USES AS A GENERIC TERM THAT CAN APPLY TO ANY OF THE RELEVANT DOSIMETRIC QUANTIES EXPOSURE IN A GENERIC SENSE TO MEAN THE PROCESS OF BEING EXPOSED TO RADIATION
  • 8. Exposure Unit •Is a measure of ionization produced in air •Is used only for X and γ radiation •Is valid for quantum energy less than 3 MeV
  • 9. X Unit 1 X unit = 1 C/kg air One exposure unit is defined as that quantity of x or gamma radiation that produces in air, ions carrying 1 coulomb of change( of either sign) per kg air.
  • 10. Exposure Exposure is measured under conditions of electronic equilibrium For photon energies above about 3 MeV, the ranges of secondary electrons become a significant fraction of the photon attenuation lengths and the departure from equilibrium may be significant Thus, exposure is not defined above photon energies of 3 MeV
  • 11. Roentgens (2/3) • Is symbolized by R • was used as the exposure unit before SI system was adopted • is still being used.
  • 12. Roentgen Is defined as the quantity of x or gamma radiation that produces ions carrying one statcoulomb of charge of either sign per cubic centimeter of air at STP. Charge of the electron=1.6x10-19 C =4.8x10-10sC 1C =3x109 sC
  • 13. 13 KERMA KERMA (Kinetic Energy Released in a Material): – Is the sum of the initial kinetic energies of all charged ionizing particles liberated by uncharged ionizing particles in a material of unit mass – For medical imaging use, KERMA is usually expressed in air SI unit = joule per kilogram (J/kg) or gray (Gy) 1 J/kg = 1 Gy
  • 14. 14 Mean absorbed dose in a tissue or organ The mean absorbed dose in a tissue or organ DT is the energy deposited in the organ divided by the mass of that organ.
  • 15. ABSORBED DOSE(1/2) • MEASURES THE ENERGY DELIVERED TO ANY MATERIAL • IN RADIATION PROTECTION THE MATERIAL CONCERNED IS THE TISSUE OR ORGAN OF THE HUMAN BODY
  • 16. ABSORBED DOSE(2/2) • DEFINED AS THE “ENERGY ABSORBED PER UNIT MASS OF ANY MATERIAL” • UNIT USED “GRAY” OR “RADS”
  • 17. 1GRAY (Gy) = 1J/kg 1RADS = 100 ergs/g 100 RADS = 1 Gy
  • 18. EQUIVALENT DOSE(1/2) QUANTIFY THE BIOLOGICAL DAMAGE TO THE ORGAN OR TISSUE IRRIDIATED The same dose levels of different radiations (ie photons and neutrons) do not have the same level of biological effect Radiation weighting factor, wR (related to radiation quality)
  • 19. EQUIVALENT DOSE(2/2) • BIOLOGICAL EFFECTS OF AN EXPOSURE ON A ORGAN OR TISSUE DEPEND ON: • ENERGY TRANSMITTED TO THE ORGAN OR TISSUE BY RADIATION • HAMFULNESS OF THE TYPE OF RADIATION INVOLVED (DEGREE OF POWER OF IONIZATION)
  • 20. Radiation weighting factors, wR 1 Type and energy ranges Radiation weighting factor, wR 1 1 5 10 20 10 5 5 Photons, all energies Electrons and muons, all energies Neutrons, energy < 10 keV 10 keV to 100 keV 100 keV to 2 MeV > 2 MeV to 20 MeV > 20 MeV Protons, other than recoil protons, energy > 2 MeV Alpha particles, fission fragments, heavy nuclei 20 1) All values relate to the radiation incident on the body, or, for internal sources, emitted from the source.
  • 21. Neutron radiation weighting factors30 25 20 15 10 5 0 wR Neutron energy - MeV 10-8 10-7 10-6 10-5 10-4 10-3 10-2 10-1 1 10 102 ICRP Recommendation ICRP Approximation
  • 22. EFFECTIVE DOSE Different body tissues have different biological sensitivities to the same radiation type and dose Tissue weighting factor, wT
  • 23. EFFECTIVE DOSE • MEASURES THE RISK OF BIOLOGICAL DAMAGE TO WHOLE BODY TAKING THE RADIOSENSITIVITIES OF TISSUE IRRIDIATED IN TO ACCOUNT • MEASURES THE RISK REGARDLESS OF EXPOSURE INVOLVED.( INTERNAL, EXTERNAL, PARTIAL OR TOTAL) • MEASURES IN THE UNIT OF. “SIEVERT”( Sv )
  • 24. Roentgen (3/3) 1R = 0.0087 J/kg of air IR = 0.0087 Gy = .87 Rad IR = 0.0096 J/kg in Tissue IR = 0.0096 Gy in Tissue IR = .96 Rad in Tissue 1 R = 1 Rad for x and γ rays IR = 1 rem = .01 Sv
  • 25. Multipliers of the equivalent dose to an organ or tissue to account for the different sensitivities to the induction of stochastic effects of radiation. Tissue or organ wT Tissue or organ wT Gonads 0.20 Bone marrow (red) 0.12 Colon 0.12 Lung 0.12 Stomach 0.12 Bladder 0.05 Breast 0.05 Liver 0.05 Oesophagus 0.05 Thyroid 0.05 Skin 0.01 Bone surface 0.01 Remainder 0.05 TOTAL 1.00 Tissue weighting factors
  • 26. Committed Dose Is a useful subsidiary dosimetric quality to express dose to body during certain time following an intake of radioactive material to the body. Note : The dose delivery to the body during the above period is at varying rates.
  • 27. Committed Equivalent Dose Defined as the time integral of the equivalent dose rate and denoted by HT( τ ) τ = integration time in years following the intake. If t is not specified Integration time is taken as 50 years for adults 70 years for children
  • 28. Committed equivalent dose: The quantity H(τ), defined as; where to is the time of intake, HT (t) is the equivalent dose rate at time t in an organ or tissue T and τ is the time elapsed after an intake of radioactive substances.When τ is not specified it will be taken to be 50 years for adults and to age 70 years for intakes by children. ( ) ( )H H t dtT t t o o τ τ = + ∫ .
  • 29. Committed effective dose: The quantity E(τ), defined as ; where HT (τ) is the committed equivalent dose to tissue T over the integration time τ and WT is the tissue weighting factor for tissue T. When τ is not specified it will be taken to be 50 years for adults and to age 70 years for intakes by children. ( ) ( )E W HT T T τ τ= ∑ .
  • 30. Collective Dose(1/2) Is used to express dose to a group or a population. Takes account of the no of people exposed to a source and the average dose to the individual.
  • 31. COLLECTIVE DOSE(2/2) DEFINED AS, THE PRODUCT OF THE NUMBER OF INDIVIDUAL EXPOSED TO A SOURCE AND THEIR AVERAGE DOSE UNIT: MAN SIEVERT (man Sv)
  • 33. Background Radiation •Natural Background Radiation •Background Radiation Due to Man Made Sources.
  • 34. NATURAL BACKGROUND RADIATION • TERRESTRIAL SOURCES • EXTRA TERRESTRIAL SOURCES ( COSMIC RADIATION )
  • 35. Natural sources of radiation… (2.4 mSv. y-1 ) Cosmic… (0.4 mSv. y-1 ) …from earth’s crust (0.4 mSv. y-1 ) …via ingestion (0.3 mSv. y-1 ) …via inhalation (1.3 mSv. y-1 ) C. Torudd ; Swedish Radiation Protection Institute ...internal
  • 36. External terrestrial irradiation 0.4 mSv y- Varies considerably with soil and rock type Unusually high background in a few places in e.g. •Esperito Santos, Brazil •Kerala, India •Guandong province, China Up to 50 µGy h-1 compared to 0.1 µGy h-1
  • 37. External extra terrestrial radiation (Cosmic radiation) Estimated spectrum of secondary particles in the atmosphere from cosmic radiation Heinrich et al 1999 (0.4 mSv. y-1 )
  • 38. Cosmic radiation Dose and ambient dose equivalent during a flight from Bangkok to Copenhagen
  • 39. External irradiation: Natural background dose rates from external sources (mSv. y-1 )
  • 40. Internal irradiation via inhalation, 1.2 mSv. y-1 (mainly indoor radon)
  • 41. Reasons for elevated levels of indoor radon •elevated levels of 238 U and 232 Th series in the ground •building material with elevated levels of 238 U and 232 Th series •tight houses (cold climate…)
  • 42. Internal irradiation via ingestion 40 K •abundance 0.0188% in potassium (K) (0.15 mSv. y-1 ) Also •uranium and thorium series (0.15 mSv. y-1 )
  • 43. Man-made Radiation • Cigarette smoke • Consumer products – Building materials – Smoke detectors • Industrial use • Medical use • Nuclear power • Nuclear fall out
  • 44. …and artificial sources of radiation Medical examinations… (0.4 mSv. y-1 ) C. Torudd ; Swedish Radiation Protection Institute
  • 45. …and more artificial sources of radiation ...and nuclear weapons (0.005 mSv. y-1 atmospherical tests) Nuclear fuel cycle… (0.0002 mSv. y-1 ) C. Torudd ; Swedish Radiation Protection Institute
  • 49. Practical concequencies of Chernobyl accident Effects of radiation and accident situation •600,000-800,000 persons in cleaning up work •Approximately 200,000 persons evacuated •Large areas of land abandoned (30 km zone etc.) Other effects: •Cost estimated to 100 billion USD
  • 50. Health concequencies of Chernobyl accident Effects of radiation and accident situation Seen: •Immediate death of 30 persons •1800 children diagnosed with thyroid cancer (1998) Statistically: •15,000 deaths in cancer (global) Other factors influencing health: •Poor food supply, social concequencies, anxiety
  • 51. Source Mean effective dose (mSv) Natural background 2,4 Medical examinations 0,4 Nuclear tests in the atmosphere 0,005 Chernobyl accident 0,002 Nuclear fuel cycle 0,0002 Individual exposure of the world’s population due to ionising radiation, year 2000 UNSCEAR
  • 52. DO WE NEED RADIATION PROTECTION ?
  • 53. Drinking Hot Coffee Excess Temperature = 60º - 37 = 23º 1 sip= 3ml 3x 23= 69 calories
  • 54. Lethal Dose= 4Gy LD 50/60 = 4 Gy For man of 70 kg Energy absorbed = 4 x 70 = 280 Joules = 280/418= 67 calories = 1 sip X-ray
  • 55.
  • 56.
  • 57.
  • 58. We live with 1-3 mSv Can kill 4000 mSv Radiation Where to stop, where is the safe point? What are the effects of radiation?
  • 59. What can radiation do? Death Cancer Skin Burns Cataract Infertility Genetic effects

Hinweis der Redaktion

  1. Electronic equilibrium is discussed in more detail in another session, but basically, when the same number of electrons are set in motion in a given volume by the primary radiation as come to rest in that same volume, we say that “electronic equilibrium” has been attained. For electronic equilibrium to exist, the attenuation of the primary radiation beam must be negligible in a distance equal to the mean range of the electrons.
  2. The second major reason that physical quantities are not used directly is that the same quantity (absorbed dose) of different types of radiation may have significantly different degrees of radiation damage – a factor of 10 or more. The term given to this quantity is relative biological effect (RBE). This is due to the differences in microdosimetric distribution of energy deposition. The difference is characterized by the quantity linear energy transfer (LET). In the past, the quality factor was used to compensate for RBE differences. However, the ICRP felt that quality factor implied a level of precision that was not justified, and it was replaced with radiation weighting factor, wR.
  3. The main impact of radiation weighting factor is on neutron dosimetry since fast neutron interactions are characterized by high LET values. However, as defined by the ICRP, wR for neutron is an energy dependent step function. Those who perform neutron dosimetry calculations, particularly fluence to “dose” conversion coefficients find such step functions disagreeable because of the discontinuities that result. Therefore, a smooth approximation has been developed that eliminates these discontinuities. It is accepted by the ICRP as long as it is understood that it is an approximation and that wR is defined by the values in the table.
  4. One of the primary reasons that the physical quantities are not used directly for radiation protection is that different body tissues have different levels of radiation sensitivity and different degrees of susceptibility to radiation induced stochastic effects such as cancer. This table was developed by the ICRP to reflect the relative tissue sensitivity to radiation induction of these effects.