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Chapter 1. Dosimetry Prof François Bochud Institut de radiophysique (IRA) UNIL / CHUV

Chapter 1. Dosimetry

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Page 1: Chapter 1. Dosimetry

Chapter 1. Dosimetry

Prof François Bochud Institut de radiophysique (IRA) UNIL / CHUV

Page 2: Chapter 1. Dosimetry

Kerma (Kinetic energy released per unit mass)

– Energy transferred (∆Etr) from the photons to the electrons within an element of mass (∆m)

– Units: Energy / mass = J/kg = Gy

• Defines a photon field in one point (not its effect) • Has to be defined for a particular material

– for instance: "air kerma"

∆=

∆trE

Km

Page 3: Chapter 1. Dosimetry

Absorbed dose

• Energy deposited locally per unit mass

– Units: Energy / mass = J/kg = Gy

• Used for any kind of radiation • Defines a physical effect of the beam in matter • Has to be defined for a particular material

– for instance "absorbed dose to water"

∆=

∆E

Dm

Page 4: Chapter 1. Dosimetry

photon

ionization

excitation

heat

desexcitation

recombinaison

photon

Photon- mater

interaction

photon

brems-strahlung

permanent effects

electron

Energy deposit: photons

Page 5: Chapter 1. Dosimetry

Dose equivalent

Same absorbed dose D0

D = D0

neutrons photons

D = D0

Page 6: Chapter 1. Dosimetry

Dose equivalent

Same absorbed dose D0

– Different effects

D = D0

neutrons photons

D = D0

Page 7: Chapter 1. Dosimetry

The biological effect is quantified by the relative biological effect (RBE), which depends on the linear energy transfer (LET)

photon

ELET

x∆

=∆

Large for alpha particles

Smaller for electrons

Page 8: Chapter 1. Dosimetry

electrons

ICRU-86

Page 9: Chapter 1. Dosimetry

ICRU-86

alpha

Page 10: Chapter 1. Dosimetry

• Low LET – Many cells,

not much touched – Reparation possible – Global effect not important (at a given absorbed dose)

• High LET – Few cells,

much touched – Reparation less easy – Global effect

important (at a given absorbed dose)

LET 10 keV/μm low RBE high RBE

Page 11: Chapter 1. Dosimetry

Relative biological effect: RBE

• Exercise 2 – Estimate the number of ionizations produced

when a 1 MeV proton passes through a cell? • Cell diameter: approximately 1 µm • We assume that an ionization requires 30 eV

– Same question for an electron of 1 MeV

Page 12: Chapter 1. Dosimetry

Reminder: mass stopping power of charged particles

Page 13: Chapter 1. Dosimetry

Equivalent dose: H

Weighting factor for radiation R ("RBE")

Absorbed dose from radiation R

[ ]1R RH w D J kg Sv [sievert]− = ⋅ = =

1 5

5 - 20 20

Radiation W R

X rays, γ , electrons protons neutrons α-particles

Page 14: Chapter 1. Dosimetry

Dose equivalent

• Exercise 4

20 mGy

XXXX

Page 15: Chapter 1. Dosimetry

Dose equivalent

• Exercise 5

Page 16: Chapter 1. Dosimetry

Estimation of the equivalent dose

• The equivalent dose is not directly measurable – no laboratory reference standard for this

quantity

• We need operational quantities – that can be used for practical measurements – used as substitutes to the equivalent dose H

Page 17: Chapter 1. Dosimetry

Ambient dosimetry: ICRU sphere • Everybody has a different

morphology • A radiation protection

instrument should be based on quantities that are simple and reproducible

• Modelization with a sphere of tissue equivalent – ICRU sphere

(density 1 g/cm3) – composition

• 76.2% oxygen • 11.1% carbon • 10.1% hydrogen • 2.6% nitrogen

diameter 30 cm

Page 18: Chapter 1. Dosimetry

H*(10) & H'(0.07) • Ambient dose equivalent

H*(10) – dose equivalent at 10 mm

depth • in the ICRU sphere

– good approximation of the equivalent dose received by an organ located in depth

– not negligible for a penetrating radiation

• Directional dose equivalent H'(0.07) – dose equivalent at 0.07 mm

de depth • in the ICRU sphere

– good approximation of the equivalent dose received by the basal cells of the skin

– essentially useful for low-penetrating radiations

The instruments shows a value "as if the ICRU sphere were

present"

Page 19: Chapter 1. Dosimetry

Hp(10) & Hp(0.07) • Personal deep dose

equivalent Hp(10) – dose equivalent in

soft tissue beneath a thickness of 10 mm at the chest

• Personal surface dose equivalent Hp(0.07) – dose equivalent in

soft tissue beneath a thickness of 0.07 mm at the chest

Page 20: Chapter 1. Dosimetry

Summary of operational quantities

skin (0.07) eye (3)

internal organ (10)

Ambient monitoring

Personal monitoring

Low penetrating radiations

H*(0.07), H*(3) H'(0.07, Ω), H'(3, Ω) Hp(0.07), Hp(3)

Penetrating radiations

H*(10) H'(10, Ω) Hp(10)

ICRU sphere without dosimeter

ISO phantoms with dosimeter

chest (whole body)

finger

Page 21: Chapter 1. Dosimetry

H*(10) & H'(0.07)

• Values of ORaP / StSV

Page 22: Chapter 1. Dosimetry

Effective dose

• Weighted sum of equivalent dose HT to the irradiated organs and tissues T

T TT

E w H= ⋅∑

Organ or tissue Tw TT

w∑

Surface of the bone, skin 0.01 0.02

Bladder, breast, liver, esophagus, thyroid, remainder1

0.05 0.30

Bone marrow, colon, lung, stomach 0.12 0.48

Gonads 0.20 0.20

Total 1.00

Page 23: Chapter 1. Dosimetry

Intake

• Committed effective dose

• depends on – physical half-life of the radionuclide – physiological mechanisms (biological half-life) – spatial distribution of the activity

( )o

o

t 50 years

50t

E E t dt+

= ∫

50 inh inh

50 ing ing

E e A

E e A

= ⋅

= ⋅

ORap/StSV values

Page 24: Chapter 1. Dosimetry

Intake: E50

• Values of ORaP / StSV

Page 25: Chapter 1. Dosimetry

Operational quantities & effective dose

• External irradiation

• Intake

• Total

( ) ( )ext pE H 10 or H* 10=

( ) ( )skin pH H 0.07 or H' 0.07=

inc 50E E=

ext incE E E= +