Standard Applicator Inserts |
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The first task is simple but time-consuming: calculating all combinations of energy and applicator with the default inserts that come with the applicators (not home-made inserts) using the standard SSD of 100cm. The goal is to check relative dose distributions and absolute dose (MU), with the calculation settings given above. | |||||||||||||||||||||||||||||||||||||||||||||||||
The planning is easy because the field sizes are exact (except for the corners, which have 8mm triangles filled out). This can be seen in the following calculation(blue) and measurement (red) of isodoses parallel to the surface in 20mm depth, for a 20MeV field and field size 4x4cm: | |||||||||||||||||||||||||||||||||||||||||||||||||
It is interesting to see that for 20MeV, the low dose region outside the field (still under the cerrobend cutout material) is a little underestimated by eMC: the measurement (red) is higher. The reason could be in the measurement (higher sensitivity of the electron diode for low-energy scatter) or the algorithm (IPS model, see eMC1.htm). All our home-made cutouts (see below) are molded a little thicker, so the verification of these could answer the question. |
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Anyway, taking into account that this is the smallest field size we allow and the highest energy, the agreement here is still very good: | |||||||||||||||||||||||||||||||||||||||||||||||||
The following table shows the number of particle histories that had to be processed until 1% accuracy was reached: | |||||||||||||||||||||||||||||||||||||||||||||||||
(Values in bold were recalculated with Eclipse 8.1 using the Distributed Calculation Framework with a parallelization factor between 6 and 12). |
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The calculation times given in the next table are taken from the "Calculation Log". They are realistic in the sense that the calculations were done mid-day, under normal clinical conditions, between all other photon calculations. Since the workload on the calculation servers is not constant, there may be large variations in calculation time, for the same field. Conditions for calculation were: 3D-image with 300 slices (slice thickness 1mm), grid 2.5mm, 1% accuracy, low 3D-gaussian smoothing. |
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Dividing the two above tables gives the number of particle histories per second (note the increase in performance for the DCF-calculated fields in bold): | |||||||||||||||||||||||||||||||||||||||||||||||||
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Home-Made Applicator Inserts | |||||||||||||||||||||||||||||||||||||||||||||||||
For the home-made inserts, which are usually rectangular or round, having all kinds of field sizes and which are sometimes asymmetric, care has to be taken when planning the field in Eclipse. The actual field sizes in isocenter somtimes differ a little (up to 3mm) from the nominal field sizes. This is due to the molding process. To avoid misinterpretation of the results, it is therefore a good idea first to do the measuement, determine the actual field size, and then calculate the field with the field size determined in the water phantom. The following images show a typical comparison of a calculated (blue) and a measured (red) crossplane distribution along the depth axis, for a 4x8cm asymmetric applicator insert and 12MeV. The Gantry is at 0°: |
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Rotating the Gantry to 25° gives oblique incidence on the water surface (9MeV, SSD100, 6x6orig insert): | |||||||||||||||||||||||||||||||||||||||||||||||||
The Gamma Index is used here to evaluate the agreement. The profiles cut vertically and horizontally through the "failed" region (blue is the calculation): | |||||||||||||||||||||||||||||||||||||||||||||||||
The gamma criterium used was 2mm/2%, but with a suppression of doses below 5%: | |||||||||||||||||||||||||||||||||||||||||||||||||