electron beam therapy - jpneylon.github.io

Post on 21-May-2022

10 Views

Category:

Documents

0 Downloads

Preview:

Click to see full reader

TRANSCRIPT

2

Electron Beam Therapy 2009

ASTRO’s view on physics teaching

3

Electron Beam Therapy 2009

Select the correct answer:

The percent depth dose at 5 cm for a 6 MeV beam is approximately: 100%, 90%, 80%, 50%, <5%?

To treat a lesion extending to a depth of 5 cm you will use: 6 MeV, 10 MeV, 15 MeV, 20 MeV?

What is the approximate range of a 6 MeV beam in lung overlaying 1 cm of tissue: 1-3 cm, 7-9 cm, > 12 cm?

A 4x8 cut-out is placed in a 10x10 beam cone for 20 MeV treatment. What changes is: 90% depth, cGy/MU, d_max, skin dose, all of the preceding?

4

Electron Beam Therapy 2009

Outline

• Production of electron beams

• Interactions of electron beams with matter

• Electron beam characteristics

• Treatment planning

5

Electron Beam Therapy 2009

Electron Beam Production

6

Electron Beam Therapy 2009

Field Flatness and Uniformity

Primary scattering foil

Secondary scattering foil

Primary collimator

Secondary collimator

Dual foil system for producing a uniform electron beam

Monoenergetic e– beam

Energy spectrum broadened

Energy spectrum broadened

7

Electron Beam Therapy 2009

Primary Scattering Foil

Secondary Scattering Foil

Ionization Chamber

Photon Jaws

Electron Cone

Electron Beam Production

8

Electron Beam Therapy 2009

Charged particle interactions

Incoming radiation

Bremsstrahlung

Main e- track

9

Electron Beam Therapy 2009

Electron-Matter Interactions

Collisional losses Inelastic (excitation, ionization)

Elastic

col

S

ρ

10

Electron Beam Therapy 2009

Electron-Matter Interactions

Radiative losses :Bremsstrahlung

Total mass stopping power radcoltot

SSS

+

=

ρρρ

rad

S

ρ

11

Electron Beam Therapy 2009

Electron Scattering

Pencil electron beam tracks in a bubble chamber

12

Electron Beam Therapy 2009

Relation of Absorbed Dose to Fluence

med

Φ is the differential fluence in energy of identical

charged particles L/ρ is the restricted mass collision stopping power with a

cutoff energy

( ) dEELDcol

E

E∆∆

Φ= ∫

,

max

ρ

13

Electron Beam Therapy 2009

Electron Dose Measurement

colkcolkk dx

dTSD,,

1

=

Φ=

ρρ colmedcolmedmed dx

dTSD,,

1

=

Φ=

ρρ

colkcolmedk

med SSD

D

,,

=

ρρ

med med

Bragg-Gray Cavity Theory

colkcolkk dx

dTSD,,

1

=

Φ=

ρρ colmedcolmedmed dx

dT1SD,,

=

Φ=

ρρ

14

Electron Beam Therapy 2009

The Bragg-Gray Cavity Theory

The ionization produced in a gas-filled cavity placed in a medium is related to the energy absorbed in the surrounding medium.

When the cavity is sufficiently small, electron fluence does not change.

colkcolmedk

med SSD

D

,,

=

ρρ

15

Electron Beam Therapy 2009

The Bragg-Gray Cavity: stopping power ratios

17

Electron Beam Therapy 2009

Energy specification and measurement

18

Electron Beam Therapy 2009

Energy specification and measurement

Measure PDD

for a broad beam

=> 20 cm x 20 cm

19

Electron Beam Therapy 2009

Energy specification and measurement

( )2

21

21

2p3p210p

MeVcm00250CMeVcm981CMeV220C

RCRCCE−− ===

×+×+=

. ;. ;.

,

20

Electron Beam Therapy 2009

Energy specification and measurement

( ) 500 RcmMeV332E ×= /.

21

Electron Beam Therapy 2009

Energy specification and measurement

( ) ( ) )/( p0pzp Rz1EE −=

22

Electron Beam Therapy 2009

Electron and Photon Beams

Photon beams indirectly ionizing exponential attenuation

Electron beams directly ionizing definite range

23

Electron Beam Therapy 2009

Electron Depth Dose: Rules of thumb

90%

(E/3.2) cm

80% (E/2.8) cm

50% (E/2.33) cm

R_p (E/1.98) cm

24

Electron Beam Therapy 2009

Electron and Photon Depth Dose

25

Electron Beam Therapy 2009

Depth doses for 20 MeV electrons compared to 15 MeV X-Rays

Electron and Photon Depth Dose

26

Electron Beam Therapy 2009

6 MeV electrons 6 MeV X-rays

Electron and Photon Depth Dose

27

Electron Beam Therapy 2009

Central Axis PDDs: field size dependence 6 MeV electrons

2x2

25x25 4x4

Little changes beyond field radius exceeding

0pp E880R ,.≅

28

Electron Beam Therapy 2009

Central Axis PDDs: field size dependence 16 MeV electrons

2 3

4

6 10-25 Little changes beyond field radius exceeding

0pp E880R ,.≅

29

Electron Beam Therapy 2009

Central Axis PDDs: energy dependence

Energy

(MeV) 4 6 9 12 16 20

Surface Dose

(% of maximum) 73.8 74.3 80.0 84.9 90.5 90.8

30

Electron Beam Therapy 2009

Electron Dose Distributions

4x4 field

2x2 field 4x2 field

6 MeV electrons

31

Electron Beam Therapy 2009

Electron Dose Distributions

16 MeV electrons

4x4 field

10x10 field

32

Electron Beam Therapy 2009

Central Axis PDD: SSD dependence

33

Electron Beam Therapy 2009

Dose profiles, at 15 mm depth at Ep,0 = 9 MeV

Profiles: SSD dependence

34

Electron Beam Therapy 2009

Dose Distributions: SSD dependence

Increased penumbra

35

Electron Beam Therapy 2009

Central axis depth dose curves plotted as a function of the angle of incidence of the beam

Angular dependence

36

Electron Beam Therapy 2009

Curved Surface Dose Distributions

Must correct predicted dose distributions for:

• Scatter of electron beam in tissue (angular dependence) • Air gap (inverse square falloff in exposure)

* SSD

Air gap

Water-equivalent materials can be used as “bolus” to smooth out uneven target surfaces

37

Electron Beam Therapy 2009

Tissue Inhomogeneity

38

Electron Beam Therapy 2009

Irregular Surface Dose Distributions

39

Electron Beam Therapy 2009

Tissue Inhomogeneity

)( CET1zdDeff −−=

CET: Coefficient of Equivalent Thickness

P

d z

Compact bone CET: 1.65

Lung CET: 0.2-0.25

40

Electron Beam Therapy 2009

Tissue inhomogeneity

uncorrected calculation corrected calculation

41

Electron Beam Therapy 2009

16 MeV electrons

Tissue Inhomogeneity

42

Electron Beam Therapy 2009

Tissue Inhomogeneity

43

Electron Beam Therapy 2009

Lead shielding for electrons

Thickness (mm) = E (MeV)/2 +1

45

Electron Beam Therapy 2009

Electron Backscatter

Solution: place a low atomic number absorber (bolus) on the surface of the shield to absorb the dose due to backscatter

Beam matching

47

Electron Beam Therapy 2009

Summary

Electron beam depth dose characteristics offer advantages for treating superficial lesions

Tissue inhomogeneities, and surface irregularities alter dose distributions significantly.

Modern treatment planning systems and dose-calculation algorithms open the possibility of wider use of electron beams as a treatment modality.

48

Electron Beam Therapy 2009

Select the correct answer:

The percent depth dose at 5 cm for a 6 MeV beam is approximately: 100%, 90%, 80%, 50%, <5%?

To treat a lesion extending to a depth of 5 cm you will use: 6 MeV, 10 MeV, 15 MeV, 20 MeV?

What is the approximate range of a 6 MeV beam in lung overlaying 1 cm of tissue: 1-3 cm, 7-9 cm, > 12 cm?

A 4x8 cut-out is placed in a 10x10 beam cone for 20 MeV treatment. What changes is: 90% depth, cGy/MU, d_max, skin dose, all of the preceding?

top related