ELECTRON BEAM RADIOTHERAPY

kanhucpatro 1,691 views 46 slides Feb 09, 2021
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About This Presentation

ELECTRON BEAM RADIOTHERAPY


Slide Content

DR.K.C PATRO
ELECTRON BEAM THERAPY

DEFINITION
Itisatypeofparticulatebeam
radiationtherapyusedforthe
treatmentofSuperficialtumors

BEAM
PHOTON
PARTICULATE
X ray
γ ray
α,β,proton,e,He,C

WHY ELECTRON BEAM
No exit dose like X-ray
Delivery of reasonably uniform dose from skin to a specific
depth
abrupt dose fall off after 90% to 80% isodose curve to near
zero level

Photon BeamPit Falls we want
Exit dose
No 100% Skin sparing
No 100% skin dose
No 100% tumor control
No normal tissue sparing
Side scatter
Low LET
High OER
Low RBE
No exit dose
100% Skin sparing
100% skin dose
100% tumor control
Normal tissue sparing
No Side scatter
High LET
Low OER
High RBE

PHOTON vs. ELECTRON
Exit dose
Near 100% Skin sparing
No 100% skin dose
High penetration
No DOSE uniformity
No exit dose
near 100% skin dose
abrupt dose fall off after
80% isodose curve
High scatter
Dose uniformity

MACHINES
Van De Graff generator.
Betatron
Linear accelerator –a device that uses
high frequency EM waves to accelerate
charged particles viz. electrons to a high
energy through a linear tube

Mechanism of production

X-ray Mode/ electron Mode

Parts of treatment head
1.Primary Collimator
2.Scattering foil
3.Flattening filter
4.Ionization chamber
5.Secondary collimator
6.Tertiary collimator ( trimmer , electron
cone, auxiliary collimator )

SCATTERING FOIL
1.The scattering foils are made up of high
dense material interposed in electron beam
2.Different scattering foils are used for
different e-energy
3.The electron beam edges can be sharply
defined only if the collimator extended
towards the skin of the pt by attachment of
trimmers/applicators
4.The electron beam trimmers are optimally
designed to give uniform fluency

ELECTRON BEAM FROM
MACHINE TO PATIENT
The energetic electron beam emerging from
accelerators is pencil beam.it is not suitable for
treatment
Hence the beam has to be spread to a larger area
for treatment.
Spread can be done by-electromagnetic scattering
device or scattering foil
To further spreading electron applicator is used

Mechanism of interaction of electron with matter
Inelastic collision with atomic electron
Inelastic collision with nuclei
elastic collision with atomic electron
elastic collision with nuclei

Fundamental questions before EBT
Indication of EBT
Goal of EBT
Planned Treatment Volume
Planned Treatment dose
Planned Treatment Technique

Indications
Treating skin cancers.
Chest wall irradiation in Ca breast.
Boosting to neck node after 45 Gy.
Total skin irradiation in mycosis fungoides.
Total limb irradiation
Total scalp irradiation
Craniospinal irradiation
Intracavitary irradiation

Dosimetry
Measured by pencil beam algorithm
Accurate in water at standard and extended
SSD
Correctly predicts changes in Penumbra
Predict changes in dose in oblique incidence
or irregular surfaces

Isodose Curves

Isodose curve characteristic
Rapid dose falloff below 80% isodose
Bulging towards bottom
Ballooning towards edge

Isodose curve in slopping
surface

Determination of absorbed dose-
Calorimeter
TLD
Solid state diode
Ionization chamber

Depth dose characteristic/isodose
characteristic
There is a abrupt fall of doses beyond 90% to
80% of isodose curve
80% or 90% isodose curve is taken as standard
dose for prescription
Depth (cm)of 90% isodose=E(Mev)/4
Depth (cm)of 80% isodose=E(Mev)/3
Electron beam penetrates a finite depth with clear
cut range,the photon beam in other hand proceeds
infinite range.

Dose dependence on incident energy

Dose dependence on field size

Depth Dose dependence on SSD

d
max
Maximum dose is not on skin
It is somehow away from skin
It is due to electronic equilibrium
6Mev-10mm
9Mev-15mm
12Mev-19mm
Approximation

Range of depth
Roughly E/2
E=energy
E.g –for 6Mev range is 6/2=3cm

Surface dose in 10x10 cm field
For 5mev=74%
10mev=82%
16mev=93%
25mev=96%
It depends upon energy,field size and
thickness of scattering foil

Energy range
6-20 Mev
6,9,12,15,18,20 mev

Selection of energy
Ep
0(MeV) = 3.3 x R
90(cm) [R
90exceeds max
depth of PTV]
Ep
0(MeV) = 2 x R
p [R
p is the practical range
of electrons ]

Ideal condition for EBT
Electron beam incidence normal to flat
surface
Underlying homogenous soft tissue
(provide uniform dose in penumbra from
surface to R
90after which there is rapid
dose fall off)

USE OF BOLUS
To flatten out irregular surface
Reduce the penetration of electrons in part of the field
Increase the surface dose
To act as a missing tissue compensator
Thickness of bolus required increases as the surface dose
increases e.g
–6-10mev=1cm
–10-15mev=0.5cm
–>15mev=no bolus

BOLUS MATERIAL
Paraffin wax,polysterene,lucite,superstoff,superflab
Flexible bolus that confirms to surface is desirable
Large air gap between the absorber and the surface
would result in scattering of e-outside the field and
reduction in dose that may not be easily predictable
unless specially measured for this condition

MLC vs. BLOCK
No MLC
Wooden MLC
Wax MLC
Customized block

BLOCKING MATERIAL
Usually Cerroband
Cerroband-Pb+Bi+Sn+Cu
Melting point=
Customized block
Thickness of block required to use as block
=E/2 e.g for 6mev=6/2=3cm

Monitor unit
CGy/MU

Decelerators
Aplateoflowatomicwt.materialsuchas
luciteandpolystereneissometimesusedto
reducetheenergyofelectronbeamknown
asdecelerators
Itmustbeplacedinclosecontactwith
patientsurfacewithbolus

Electron arc
therapy

Electron field-photon field
combination

Total skin irradiation-

Total scalp irradiation

Craniospinal irradiation

Total limb irradiation
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