Ns. Patel et al., The use of cylindrical coordinates for treatment planning parameters of anelongated Ir-192 source, INT J RAD O, 51(4), 2001, pp. 1093-1102
Citations number
19
Categorie Soggetti
Radiology ,Nuclear Medicine & Imaging","Onconogenesis & Cancer Research
Journal title
INTERNATIONAL JOURNAL OF RADIATION ONCOLOGY BIOLOGY PHYSICS
Purpose: The doses given to the intima, media, and adventitia are very cruc
ial quantities in intravascular brachytherapy. To facilitate accurate compu
terized treatment planning calculations, we have determined dose distributi
ons in away-and-along table format around an Ir-192 wire source and develop
ed pertinent dosimetric parameters in cylindrical coordinates.
Methods and Materials: The Monte Carlo method (MCNP4C code) was used to cal
culate the dose distributions for the AngioRad Ir-192 wire source (model SL
-77HS, Interventional Therapies). The calculations were carried out for pho
ton, beta, and electron (conversion and Auger) contributions for radial dis
tances from 0.03 to 2.0 cm with 0.01-cm increments, and up to 2.24 cm from
the source center in the longitudinal direction with 0.04-cm resolution. Do
se rate values are determined in away-and-along format (cylindrical coordin
ates) and then converted to spherical coordinate format. Dosimetric paramet
ers, such as the geometry factor, G(r, theta), and anisotropy function, F(r
, theta), are generated in both cylindrical (R, Z, phi) and spherical (r, t
heta, phi) coordinates. The use of a cylindrical coordinate system for trea
tment planning parameters is proposed as a more suitable approach for accur
ate calculations.
Results: The photon contribution to dose varies nearly inversely with radia
l distance (from the source center) along the perpendicular bisector with 0
.199 X 10(-3) cGy U-1 s(-1) (0.802 cGy Ci(-1) s(-1)) at I cm. The beta and
electron contributions start at very high values of about 35.5 X 10(-3) cGy
U-1 s(-1) and 11.0 x 10(-3) cGy U-1 s(-1), respectively, at 0.03 cm and fa
ll off exponentially to negligible amount near 0.2 cm. The total dose rate
at 0.2 cm is 1.428 X 10(-3) cGy U-1 s(-1) (5.754 cGy Ci(-1) s(-1)). The rad
ial dose function, g(R), is nearly unity between 0.2 cm and 2 cm. Due to th
e beta and electron dose contributions, g(R) increases steeply to 5.5 as ra
dial distance decreases from 0.2 cm down to 0.03 cm. The F(R, Z) values are
close to unity for the majority of the region of interest. In contrast, F(
r, theta) experiences a steep rise as shallow angles are approached (closer
to the source), related to the beta dose contributions. Accurate treatment
planning calculations would be possible with linear interpolation of F(R,
Z), but difficult with F(r, theta) in the spherical coordinate system and t
he original normalization point as recommended in the American Association
of Physicists in Medicine Task Group 60 (AAPM TG-60) formalism.
Conclusion: The AngioRad Ir-192 wire source, model SL-77HS, was completely
characterized dosimetrically using Monte Carlo methods. The use of cylindri
cal coordinates and a modified anisotropy function normalization point for
dosimetric parameters of an elongated Ir-192 source is more suitable for ac
curate computerized treatment planning calculations in intravascular brachy
therapy. (C) 2001 Elsevier Science Inc.