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S771

ESTRO 36 2017

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i) collimator angle modified 1º, 2º and 3º, ii) X-jaws

modified +2 mm, +5 mm, -2 mm and +5 mm, iii) Y-jaws

modified 5 and -5 mm, iv) gantry modified 2º in 4 control

points (CP), 1º in 8 CP, 1º in all the control points and

finally 2º in all the control points, v) in other plans total

UM, that is, total dose, was modified by 1, 2, 3, 5 and 10%,

vi) UM for 4 individual CP were modified by 10%, 10% for 8

CP and 20% for 8 CP, vii) the position of all the leafs were

modified +0.5, -0.5, +1 and -1 mm, viii) in other plans leafs

were modified in each CP in a random way with a

maximum displacement of 1, 2 and 5 mm and finally ix)

leafs were modified in a random way with a maximum

displacement of 2, 5 and 10 mm but using the same

displacement for a particular leaf in all the CP. We have

compared the dose obtained with the EPID with that

calculated by the Pinnacle TPS collapsing the VMAT plans

and using the Epiqa software. The gamma 3%/3mm,

2%/2mm and 2%/1 mm have been obtained. We have

looked also for visual differences between the dose

obtained with the EPID and that obtained with the

Pinnacle TPS.

Results

The analysis of the data shows that some errors can be

detected, such as the collimator errors, some X and Y jaws

errors, leafs with a systematic displacement, plans with a

difference in total dose of 3, 5 and 10% error. Some errors

in plans were very hard to detect or undetectable such as

that plans with different UM in some control points,

different gantry positions, total dose difference of 1 or 2%,

and random errors in the leaves in each control point.

Conclusion

The aS1200 EPID of TrueBeam 2.0 Linac plus the Epiqa

software is capable to detect errors in the irradiation of

treatment plans although some other errors are

undetectable by this system. This makes EPID and

interesting dosimetric equipment for the QA of VMAT

plans.

EP-1461 Scintillator dosimetry reveals lung tumor size

dependency of 6 MV AAA dose calculations

W. Ottosson

1

, P. Sibolt

1,2

, C.F. Behrens

1

, C.E. Andersen

2

1

Herlev Hospital, Radiotherapy Research Unit-

Department of Oncology, Herlev, Denmark

2

Technical University of Denmark, Radiation Physics-

Center for Nuclear Technologies, Roskilde, Denmark

Purpose or Objective

Radiotherapy for lung cancer generally has a poor

prognosis. Motion during imaging and treatment is a major

challenge, but also other factors may contribute to the

poor prognosis. One such factor is the ability of current

treatment planning systems to accurately compute

absorbed dose to tumors in the thorax region where large

heterogeneities are present. The current study was

designed to experimentally address the question: What is

the agreement between actual delivered dose and

computed dose using the Anisotropic-Analytical-Algorithm

(AAA) in Eclipse treatment planning system for a thoracic-

like geometry with tumors of different sizes? This is an

important question given the widespread use of AAA and

the changes in tumor sizes both over the course of

treatment, and from patient-to-patient.

Material and Methods

An in-house developed thoracic-like phantom, enabling

measurements of radiotherapy under well-defined

conditions, was used. The phantom has a body of PMMA

and can be filled with inserts of various materials,

including simulated spherical lung tumors made of PMMA

(ranging from 1-8 cm in diameter) which are embedded in

low-density balsa wood that simulates lung-tissue. 14

different phantom setups underwent CT scanning,

structure delineation, and treatment planning. 56

isocentric treatments of different complexity and

phantom configurations were calculated using AAA.

Treatment techniques investigated included single

conventional field technique, four-field conventional box

technique, five-field intensity-modulated radiotherapy

and dual-arc volumetric-modulated arc technique. To

perform accurate dosimetry under these non-reference

conditions, point measurements were carried out using

water-equivalent, organic plastic scintillator detectors

(PSDs), positioned in the center of the PMMA tumors. Dose

differences between measurements and AAA calculations

were calculated.

Results

Considerable tumor-size dependence was observed. For

tumor sizes ≤ 2 cm, the dose deviations between AAA

calculations and PSD measurements were 7.4±1.8%

(median ± 1SD). For larger tumor sizes (3-8 cm in

diameter) corresponding dose deviations were 4.2±1.4%.

For the most homogeneous setup, the dose deviations

were insignificant (0.3±0.6%). The results were essentially

independent of treatment technique.

Conclusion

This study suggests a systematic tumor-size dependent

dose calculation error for treatment planning on small

tumor sizes in heterogeneous setups. This may originate

from imperfections in the AAA algorithm. The largest dose

deviations were observed for the smallest tumor sizes.

Although, it is well known that AAA has issues in

heterogeneous regions, we are not aware of any previous

experimental study demonstrating a similar systematic

tumor-size effect. The effect is large enough to

potentially have implications for lung cancer treatment

planning. Monte Carlo simulations are currently being

conducted in order to verify these findings.

EP-1462 The impact on VMAT optimization using Type

C vs B algorithms for patients with temporary gas

pockets

B. Smulders

1

, J. Thomsen

1

, P. Munck Af Rosenschöld

1

1

Rigshospitalet, Department of Oncology, Copenhagen,

Denmark

Purpose or Objective

In our clinic, we have introduced a type C (i.e. Monte

Carlo-like) dose calculation algorithm and dose to medium

as standard practice. Previous work has shown difference

between type B and type C calculation algorithms for dose

calculation in high and very low density areas. However,

little attention has been given to study the robustness of

the treatment plans optimized using type C algorithms

during the course of radiotherapy. In particular, the initial

CT scan used for radiotherapy treatment planning can

contain temporary gas pockets inside the target volume

for patients with tumours in the pelvis that later disappear

during the course of radiotherapy. In this study we are

interested to explore the dosimetric impact of applying

the type C dose calculation algorithm for patients treated

in the pelvic area using VMAT, where gas pockets appear

and disappear in the rectum.

Material and Methods

Ten clinical cervix cancer patients were selected for this

study. The patients had different sizes of gas pockets on

the planning CT. The treatment plans were optimized and

calculated using one type B and one type C dose

calculation algorithm (Eclipse, AAA and Acuros XB(Dose to

Medium), respectively). Gas pockets of these patients