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S1003

ESTRO 36

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calculation time. We obtain a set of angular moments

equations, and we close thisset using the Boltzmann's

principle of entropy maximization on the two first

equations of the set. We show that this model has an

accuracy comparable to references Monte-Carlo

(MC)codes (Geant4, MCNPx, Penelope), and is less time-

consuming than these ones. We found out this method

applies to new approaches, as MRI-guided radiotherapy

which consists in irradiating a patient under the in uence

of a magnetic eld. We added the effect of the Lorentz

force into our code, and compared it to a reference full

MC code FLUKA.

Results

We obtain a good agreement between simulations from

our model and FLUKA. We are able to highlight some

effects that occur on the propagation of particles in the

matter, which modify the dose distribution on the

interface between materials of different densities in a

presence of a magnetic field of a few Tesla. These effects

have to be taken into account in order to prevent creation

of hot spots or a spread of energy distribution in a human

body, within computation times compatible with their use

in the clinical environment.

Conclusion

Our model could be applied to future clinical cases and

would allow a faster and more efficient way to plan a

viable treatment for a patient. We plan to validate our

results with an experimental campaign.This work takes

place in the framework of POPRA (Programme Optique

Physique et Radiothérapie en Aquitaine), which

involves

several laboratories around problematics on the topic

of cancer treatment.

EP-1832 Selecting head and neck cancer patients for

proton therapy: the influence of dosimetric thresholds

I.T. Kuijper

1

, M. Dahele

1

, A. Delaney

1

, B. Slotman

1

, W.

Verbakel

1

1

VU University Medical Center, Department of Radiation

Oncology, Amsterdam, The Netherlands

Purpose or Objective

Selecting head and neck cancer patients for proton

therapy should be based on objective parameter(s) that

indicate a reduced chance of toxicity, for example, on

the dosimetric benefit for swallowing and salivary gland

structures. We compared volumetric arc therapy photon

(VMAT) and intensity modulated proton plans (IMPT) in

order to estimate how many patients would be referred

for proton therapy using different thresholds of reduction

in organ at risk (OAR) dose.

Material and Methods

Non-robust IMPT plans were generated for 40 patients with

locally advanced head and neck cancer (Varian Medical

Systems, 3 fields, multi-field optimization, NUPO/PCS

V13.7.14) and compared with the clinical VMAT plans

(Varian Medical Systems, RapidArc, 2 arcs, 6MV photons,

Acuros V13.6.15). All patients had a simultaneous

integrated boost with a fractionation scheme of 35 x

1,55/2 Gy for PTV-elective/PTV-boost. For all plans, the

focus was on sparing of all individual salivary and

swallowing structures. Patients were categorized

according to the amount of additional OAR sparing

achieved with proton plans represented by the sum of

mean doses to (1) all swallowing structures, (2) parotid

gland(s) and (3) submandibular gland(s), if the mean dose

was <45Gy for any of these structures using IMPT and/or

VMAT.

Results

The range for the sum of the three mean doses for photon

plans was 37.2-180.8Gy (median 115.4), and for proton

plans 21.5-161.9Gy (median 92.1). Differences in total

mean dose between photon and proton plans ranged from

1.2-37.2Gy (median 16.9). Assuming a threshold of 10Gy

sparing in sum of mean doses (i.e. proton plan achieved at

least 10Gy reduction in total mean dose): 82.5% of proton

plans achieved this; threshold 15Gy: achieved by 67.5%

proton plans; threshold 20Gy: achieved by 40.0% proton

plans; threshold 25Gy: achieved by 17.5% proton plans.

Conclusion

The vast majority of patients had a dosimetric benefit

with protons as assessed by mean dose to swallowing and

salivary gland structures. The results show that the

number of patients who would be selected/referred for

protons is highly sensitive to the choice of threshold. This

has implications for activity levels in proton and photon

departments.

EP-1833 Bowel doses in cervical cancer patients

treated with a full bladder during radiotherapy.

A. Schouboe

1

, E. Kjaersgaard

1

, N. Jensen

1

, L. Fokdal

1

, L.

Nyvang

2

, M. Assenholt

2

, J. Lindegaard

1

, K. Tanderup

2

, A.

Vestergaard

2

1

Aarhus University Hospital, Department of Oncology,

Aarhus N, Denmark

2

Aarhus University Hospital, Department of Medical

Physics, Aarhus N, Denmark

Purpose or Objective

Large inter-fractional organ motion is a challenge in cervix

cancer radiotherapy. To reduce inter-fractional organ

motion, a bladder filling instruction aiming for a

comfortably full bladder has been introduced with daily

Cone Beam CT (CBCT). The purpose of the study is to

evaluate the correlation between bladder filling variation

and bowel dose.

Material and Methods

Eight consecutive patients with locally advanced cervical

cancer treated with chemo radiotherapy, were included in

the study. Dose planning and treatment was performed in

supine position. Prescribed dose was 45-50 Gy in 25-30

fractions to the pelvis, 5 fractions per week. Daily CBCT

with bony fusion and couch correction was performed. A

bladder filling protocol was applied with verbal and

written instructions, advising patients to drink 450 ml of

water in 15 minutes post micturition, 1 hour prior to each

treatment. All patients were retrospectively re-planned

with a uniform dose of 45 Gy in 25 fractions using VMAT.

Target and organs at risk were delineated on CT images

for dose planning and on every CBCT (n=210). The clinical

target volume (CTV) encompassed the gross tumour

volume (GTV), cervix, parametria, uterus, upper vagina

and the nodal CTV. A PTV margin of 1.5cm was applied for

the GTV, cervix, and uterus and 5mm for the nodal CTV

and parametria. Outer extension of bowel loops were

delineated including sigmoid in one volume (Bowel) on

each of the CBCTs. Based on a bony fusion, all structures

were transferred to the planning CT to asses bowel V30 Gy

and V43Gy for each fraction. Changes in bowel V30 and

V43 of bowel were evaluated as a function of changes in

bladder volume compared to the parameters on the

planning CT.

Results

A large variation in bladder filling was observed and was

found to be patient dependent. Large variation in bladder

volume and uterus position resulted in large variation in

V30 (Table 1). A linear correlation was found between

bowel V30 and V43 and bladder volume. Inter-fractional

bowel motion was observed due to changes in bladder

volume. Linear regression showed that with an increase of

100 cc in bladder volume, the bowel V30 is decreased by

a mean of 58 cc (range: 10 – 87 cc). For one patient, the

position of the uterus was not affected by bladder filling

changes and there was no clear correlation between

bladder volume changes and bowel irradiation (Fig 1).