Este trabalho tem por objetivo a composição e caracterização de um dosímetro à base de DL-Alanina e Ferro-ll em forma de gel para aplicações em dosimetría para campos de doses da radiação gama do Co-60 experimentadas em procedimentos de radioterapia. O aminoácido DL-Alanina é dissolvido em solução ácida contendo o Fe-ll e adicionado o gel. Procedeu-se a uma série de ensaios variando reagente a reagente e realizando procedimentos para avaliar o comportamento em função do tempo do gel dosimétrico obtido. Os espectros de absorção antes e após a irradiação apresentam máximos em 457 nm e 588 nm, respectivamente. Esses dois picos correspondem aos comprimentos de onda de absorção das espécies Fe-ll e Fe-lll, respectivamente; estando ambas as espécies em equilíbrio. Com a irradiação, ocorre a formação de radicais que oxidam o Fe-ll em Fe-lll, alterando com isso o balanço entre as duas espécies - daí o aumento da concentração de Fe-lll - fazendo com que mude a tonalidade do gel, sendo, portanto, possível de ser determinada a dose absorvida. Nas análises dos espectros e respectivas curvas dose-resposta observou-se que o gel dosimétrico apresenta linearidade no intervalo de doses entre 0,5 e 40 Gy. A partir dos resultados obtidos de linearidade, estabilidade e menor dose detectável - 0,3 Gy - conclui-se que o presente Gel Dosimétrico à base de DL-Alanina e Fe-ll apresenta excelente potencial para a finalidade que é proposto, qual seja a determinação do campo de doses em radioterapia e futura aplicação como padrão na determinação desses campos, em 3D, utilizando-se a técnica de Imagem por Ressonância Magnética - IRM. / The aim of this work is to develop a DL-Alanine, Fe-ll based gel dosimeter to be applied in the dosimetry of the Co-60 gamma-radiation fields in the dose range of radiation therapy procedures. The aminoacid DL-Alanine is dissolved in an acid solution containing the Fe-ll and added to the gel. A series of essays was performed with different chemicals and different procedures were made to evaluate the behavior of the obtained dosimetric gel as function of the time. The absorption spectra, before and after the irradiation, present maximum in 457 nm and 588 nm, respectively. These two peaks correspond to absorption wavelengths of the chemical species Fe-ll and Fe-lll, respectively, both species being in equilibrium. With the irradiation, the formation of the radicals that oxide the Fe-ll into Fe-lll occurs, altering the chemical balance of both species - hence the increase of the Fe-lll - and causing the gel to change its tonality, in such a way that it is possible to determine the absorved dose. In the analysis of the spectra and respective dose-response curves it was observed that the dosimetric gel shows linearity in dose range of 0.5 to 40 Gy. From the obtained linearity results, stability and lower detectable dose - 0,3 Gy - it is possible to conclude that the present DL-Alanine, Fe-ll based dosimetric gel presents an excellent potential to the application to which it is proposed, namely, the determination of the dose fields in radiation therapy and its future application as a standard in the determination of these fields, in 3D, using the Magnetic Resonance Imaging.

De acordo com os princípios da proteção radiológica, as práticas que envolvem radiações ionizantes devem ser planejadas e executadas de modo que os valores de doses individuais, o número de pessoas expostas e a probabilidade de exposições acidentais sejam tão baixos quanto razoavelmente exequíveis. Para tanto, faz-se necessário que na execução da dosimetria das radiações sejam utilizados medidores confiáveis de grandezas dosimétricas. Esta confiabilidade depende não só da calibração do medidor, mas também do seu desempenho em determinadas condições de teste. A International Standardization Organization (ISO), com o objetivo de promover a padronização e a coerência metrológica internacional, estabeleceu conjuntos de feixes de raios X de referência para calibração e testes de dosímetros, cuja implantação nos laboratórios de metrologia deve atender a requisitos técnicos específicos. Em baixas energias existem especificidades que precisam ser consideradas tanto na implantação dos feixes de referência quanto na sua utilização em calibração e testes. O presente trabalho faz uma análise dos procedimentos e critérios de implantação das radiações de referência ISO 4037, em baixas energias. Foram realizados experimentos que permitiram cálculos de parâmetros de caracterização dos feixes de referência do Laboratório de Calibração de Dosímetros do Centro de Desenvolvimento da Tecnologia Nuclear (LCD/CDTN). Alternativas às metodologias usuais de determinação da camada semirredutora foram estudadas. Espectros de feixes de referência foram simulados por meio de softwares e comparados com espectros medidos experimentalmente. Condições climáticas distintas foram reproduzidas em laboratório para análise dos seus efeitos sobre os parâmetros dos feixes. Incertezas em relação às medidas de parâmetros de implantação foram avaliadas. Os feixes de baixa energia, de acordo com os critérios da norma ISO 4037, foram considerados implantados, permitindo a revisão dos valores dos coeficientes de conversão de kerma no ar para grandezas operacionais de proteção radiológica. / According to the radiological protection principles, practices involving ionizing radiation must be planned and carried out under the guarantee that the values of individual doses, the number of people exposed to radiation and the probability of accidental exposures are as low as reasonably achievable. Therefore, radiation dosimetry is required to be done with reliable instruments designed for measuring dosimetric quantities. The reliability of the dosimetry depends on both the calibration of the dosimeter and its proper performance under certain test conditions. The International Standardization Organization (ISO), in order to promote international standardization and metrological coherency, established sets of reference X-ray beams for dosimeter calibration and typing-test; they are expected to be implemented in metrology laboratories in compliance with specific technical requirements. At low energies there are specific requirements that need to be considered in both the implementation of the reference beams and their use in calibration and testing. The present study is an analysis of the procedures and criteria for ISO 4037 reference radiation implementation, at low energies. In the Dosimeter Calibration Laboratory of the Development Center of Nuclear Technology (LCD / CDTN), experiments were performed for determining the X-ray reference radiation parameters. Alternatives to the usual methods for half-value layer determination were studied. Spectra of reference beams were simulated with software and compared with experimental measurements. Different climatic conditions were reproduced in the Laboratory for analysis of its influence on the determination of the beam parameters. Uncertainties in the measurements of studied parameters were evaluated. According to the ISO 4037 criteria, the low energy X-ray beams were considered to be implemented; they allowed the determination of the conversion coefficients from air kerma to the operational radiation protection quantities.

Este trabalho tem por objetivo a composição e caracterização de um dosímetro à base de DL-Alanina e Ferro-ll em forma de gel para aplicações em dosimetría para campos de doses da radiação gama do Co-60 experimentadas em procedimentos de radioterapia. O aminoácido DL-Alanina é dissolvido em solução ácida contendo o Fe-ll e adicionado o gel. Procedeu-se a uma série de ensaios variando reagente a reagente e realizando procedimentos para avaliar o comportamento em função do tempo do gel dosimétrico obtido. Os espectros de absorção antes e após a irradiação apresentam máximos em 457 nm e 588 nm, respectivamente. Esses dois picos correspondem aos comprimentos de onda de absorção das espécies Fe-ll e Fe-lll, respectivamente; estando ambas as espécies em equilíbrio. Com a irradiação, ocorre a formação de radicais que oxidam o Fe-ll em Fe-lll, alterando com isso o balanço entre as duas espécies - daí o aumento da concentração de Fe-lll - fazendo com que mude a tonalidade do gel, sendo, portanto, possível de ser determinada a dose absorvida. Nas análises dos espectros e respectivas curvas dose-resposta observou-se que o gel dosimétrico apresenta linearidade no intervalo de doses entre 0,5 e 40 Gy. A partir dos resultados obtidos de linearidade, estabilidade e menor dose detectável - 0,3 Gy - conclui-se que o presente Gel Dosimétrico à base de DL-Alanina e Fe-ll apresenta excelente potencial para a finalidade que é proposto, qual seja a determinação do campo de doses em radioterapia e futura aplicação como padrão na determinação desses campos, em 3D, utilizando-se a técnica de Imagem por Ressonância Magnética - IRM. / The aim of this work is to develop a DL-Alanine, Fe-ll based gel dosimeter to be applied in the dosimetry of the Co-60 gamma-radiation fields in the dose range of radiation therapy procedures. The aminoacid DL-Alanine is dissolved in an acid solution containing the Fe-ll and added to the gel. A series of essays was performed with different chemicals and different procedures were made to evaluate the behavior of the obtained dosimetric gel as function of the time. The absorption spectra, before and after the irradiation, present maximum in 457 nm and 588 nm, respectively. These two peaks correspond to absorption wavelengths of the chemical species Fe-ll and Fe-lll, respectively, both species being in equilibrium. With the irradiation, the formation of the radicals that oxide the Fe-ll into Fe-lll occurs, altering the chemical balance of both species - hence the increase of the Fe-lll - and causing the gel to change its tonality, in such a way that it is possible to determine the absorved dose. In the analysis of the spectra and respective dose-response curves it was observed that the dosimetric gel shows linearity in dose range of 0.5 to 40 Gy. From the obtained linearity results, stability and lower detectable dose - 0,3 Gy - it is possible to conclude that the present DL-Alanine, Fe-ll based dosimetric gel presents an excellent potential to the application to which it is proposed, namely, the determination of the dose fields in radiation therapy and its future application as a standard in the determination of these fields, in 3D, using the Magnetic Resonance Imaging.

Com o objetivo de monitorar o crescente número de trabalhadores potencialmente expostos à radiação de nêutrons, foi projetado e desenvolvido um dosímetro individual para campos mistos nêutron-gama. O dosímetro proposto foi caracterizado para o espectro de energia de uma fonte de Amerício-Berílio e para o intervalo de dose de interesse da proteção radiológica (até 20 mSv). Para tanto utilizou-se a dosimetria termoluminescente de albedo e a dosimetria de traços nucleares, técnicas consagradas na literatura internacional, empregando materiais de fabricação nacional e de baixo custo. Um policarbonato comercial, denominado SS-1, foi caracterizado para aplicação como detector sólido de traços nucleares. Os parâmetros para revelação química e ampliação dos traços, assim como a metodologia de avaliação dos detectores foram determinados. Estudou-se a resposta dos detectores TLD-600, TLD-700 e SS-1 em campos mistos nêutrongama de uma fonte de Amerício-Berílio e definiu-se um algoritmo para cálculo da dose de nêutrons e de radiação gama. A razão entre as respostas para nêutrons térmicos, de albedo e rápidos permite analisar o espectro ao qual o dosímetro foi submetido e corrigir a resposta do detector de traços para variações no ângulo de incidência da radiação. O novo dosímetro está pronto e apresenta desempenho para ser usado como dosímetro de nêutrons no Brasil. / An individual dosimeter for neutron-gamma mixed field dosimetry was design and developed aiming monitoring the increasing number of workers potentially exposed to neutrons. The proposed dosimeter was characterized to an Americium-Beryllium source spectrum and dose range of radiation protection interest (up to 20 mSv). Thermoluminescent albedo dosimetry and nuclear tracks dosimetry, traditional techniques found in the international literature, with materials of low cost and national production, were used. A commercial polycarbonate, named SS-1, was characterized for solid state tack detector application. The chemical etching parameters and the methodology of detectors evaluation were determined. The response of TLD-600, TLD-700 and SS-1 were studied and algorithms for dose calculation of neutron and gamma radiation of Americium- Beryllium sources were proposed. The ratio between thermal, albedo and fast neutrons responses, allows analyzing the spectrum to which the dosimeter was submitted and correcting the track detector response to variations in the radiation incidence angle. The new dosimeter is fully characterized, having sufficient performance to be applied as neutron dosimeter in Brazil.

Dosimetry is a vital component of treatment planning in radiation therapy. Methods of radiation dosimetry currently include the use of: ionization chambers, thermoluminescent dosimeters (TLDs), solid-state detectors and radiographic film. However, these methods are inherently either 1D or 2D and their use involves the perturbation of the radiation beam. Although the dose distribution within tissues following radiation therapy treatments can be modeled using computerized treatment planning systems, a need exists for a dosimeter that can accurately measure dose distributions directly and produce 3D dose maps. Some radiation therapy and brachytherapy treatments require mapping the dose distributions in high-resolution (typically < 1 mm). A dosimetry technique that is capable of producing high resolution 3D dose maps of the absorbed dose distribution within tissues is required. Gel dosimetry is inherently a 3D integrating dosimeter that offers high spatial resolution, precision and accuracy. Polymer gel dosimetry is founded on the basis that monomers dissolved in the gel matrix polymerize due to the presence of free radicals produced by the radiolysis of water molecules. The amount of polymerization that occurs within a polymer gel dosimeter can be correlated to the absorbed dose. The gel matrix maintains the spatial integrity of the polymers and hence a dose distribution can be determined by imaging the irradiated polymer gel dosimeter using an imaging modality such as MRI, x-ray computed tomography (CT), ultrasound, optical CT or vibrational spectroscopy. Polymer gel dosimeters, however, suffer from oxygen contamination. Oxygen inhibits the polymerization reaction and hence polymer gel dosimeters must be manufactured, irradiated and scanned in hypoxic environments. Normoxic polymer gel dosimeters incorporate an anti-oxidant into the formulation that binds the oxygen present in the gel and allows the dosimeter to be made under normal atmospheric conditions. The first part of this study was to provide a comprehensive investigation into various formulations of polymer and normoxic polymer gel dosimeters. Several parameters were used to characterize and assess the performance of each formulation of polymer gel dosimeter including: spatial resolution and stability, temporal stability of the R2-dose response, optimal R2-dose response for changes in concentration of constituents and the effects of oxygen infiltration. This work enabled optimal formulations to be determined that would provide greater dose sensitivity. Further work was done to investigate the chemical kinetics that take place within normoxic polymer gel dosimeters from manufacture to post-irradiation. This study explored the functions that each of the constituent chemicals plays in a polymer gel dosimeter. Although normoxic polymer gel dosimeters exhibit very similar characteristics to polyacrylamide polymer gel dosimeters, one important difference between them was found to be a decrease in R2-dose sensitivity over time in the normoxic polymer gel dosimeter compared to an increase in the polyacrylamide polymer gel dosimeters. From an investigation into the function of anti-oxidants in normoxic polymer gel dosimeters, alternatives were proposed. Several alternative anti-oxidants were explored in this study that found that whilst some were reasonably effective, tetrakis (hydroxymethyl) phosphonium chloride (THPC) had the highest reaction rate. THPC was found not only to be an aggressive scavenger of oxygen, but also to increase the dose sensitivity of the gel. Hence, a formulation of normoxic polymer gel dosimeter was proposed, called MAGAT, that comprised: methacrylic acid, gelatin, hydroquinone and THPC. This formulation was examined in a similar fashion to the studies of the other formulations of polymer and normoxic polymer gel dosiemeters. The gel was found to exhibit spatial and temporal stability and an optimal formulation was proposed based on the R2-dose response. Applications such as IVBT require high-resolution dosimetry. Combined with high-resolution MRI, polymer gel dosimetry has potential as a high-resolution 3D integrated dosimeter. Thus, the second component of this study was to commission a micro-imaging MR spectrometer for use with normoxic polymer gel dosimeters and investigate artifacts related to imaging in high-resolutions. Using high-resolution MRI requires high gradient strengths that, combined with the Brownian motion of water molecules, was found to produce an attenuation of the MR signal and hence lead to a variation in the measured R2. The variation in measured R2 was found to be dependent on both the timing and amplitude of pulses in the pulse sequence used during scanning. Software was designed and coded that could accurately determine the amount of variation in measured R2 based on the pulse sequence applied to a phantom. Using this software, it is possible to correct for differences between scans using different imaging parameters or pulse sequences. A normoxic polymer gel dosimeter was irradiated using typical brachytherapy delivery and the resulting dose distributions compared with dose points predicted by the computerized treatment planning system.The R2-dose response was determined and used to convert the R2 maps of the phantoms to dose maps. The phantoms and calibration vials were imaged with an in-plane resolution of 0.1055 mm/pixel and a slice thickness of 2 mm. With such a relatively large slice thickness compared to the in-plane resolution, partial volume effects were significant, especially in the region immediately adjacent the source where high dose gradients typically exist. Estimates of the partial volume effects at various distances within the phantom were determined using a mathematical model based on dose points from the treatment planning system. The normalized and adjusted dose profiles showed very good agreement with the dose points predicted by the treatment planning system.

The risk of secondary cancer associated with low doses of ionizing radiation, is gaining new interest every day, especially in long term surviving patients. The unavoidable amount of the scattered dose, which is absorbed by radiosensitive tissues/organs away from the irradiated treatment site, known as peripheral dose (PD), is the outcome of secondary irradiation sources while it influences the treatment parameters. Since the associated cancer risk is likely to be much lower but not insignificant from such low doses this may affect the choice of treatment options adopted. In this study, we performed measurements in a water phantom in order to indicate the trends of the PD from conventional radiotherapy and to demonstrate the influence of typical treatment parameters, such as the distance, the depth, the field size and the energy using the mobileMOSFET dose verification system. The PD is given as a function of the above treatment parameters and a comparison was made with an ionization chamber. In the same way measurements are presented in an anthropomorphic phantom and a comparison of the results between the mobileMOSFET dose verification system and the treatment planning software is given. Finally, the PD measurements were performed in preselected areas outside the treatment field in patients undergoing 3D conformal radiotherapy treatment and since, modern treatment modalities such as the stereotactic radiosurgery/radiotherapy (SRS/SRT) procedures consolidate more and more in the treatment of benign and malignant disease, we investigated the PD in patients undergoing intracranial and extracranial treatment with Cyberknife, before and after the shielding upgrade, and demonstrated the influence of the monitor units (MU) and the size of the collimator. A discussion for the potential of stochastic radiation induced effects with both treatment modalities is also given. Peripheral dose (PD) is strongly dependent upon the irradiation parameters selected during the treatment planning procedure such as the distance, the depth, the field size and the energy of the photon beam. More specifically, PD decreases almost exponentially with the increase of distance. Close to the edge of the field, the internal scattered radiation from the patient is the predominant source of secondary scattered dose. As the distance from the field edge increases, the radiation scattered by the collimator, and the machine leakage become predominant. On the other hand, the PD is higher near the surface and drops to a minimum at the depth of dmax, and then the PD tends to become constant with depth. Closer to the field edge, where internal scatter from the phantom dominates, the PD increases with depth, because the ratio of the scatter to primary increases with depth. A few centimetres away from the field, where collimator scatter and leakage dominate, the PD decreases with depth, due to the attenuation by the water. Finally, PD is significantly higher for larger field sizes, due to the increase of the scattering volume and as the energy increase the PD increases too. According the results of PD measurements with the 3D conformal radiotherapy treatment, the mean PD in the thyroid gland, expressed as a percentage of the prescribed dose (%TD), was 1.43 %, 9.85 %, 7.27% and 2.02 %, corresponding to whole brain irradiation, mediastinum treatment, and breast treatment with and without the irradiation of supraclavicular and axillary nodes, respectively. The risk of radiation induced cancer to the thyroid gland was estimated to be at levels of 0.18 %, 1.19 %, 1.18 % and 0.33 % respectively. The mean PD of the breast, expressed as a % TD, was 5.90 %, 2.59 % and 3.14% corresponding to mediastimun treatment and breast treatment with and without the irradiation of supraclavicular and axillary nodes, respectively. The risk to the breast was estimated to be at levels of 3.97 %, 1.76 % and 1.45%, in mediastinum and breast treatment, with and without the supraclavicular irradiation, respectively. Although the results indicate that there is not an increased risk of secondary cancer in the thyroid gland and the breast after conventional radiotherapy (3D CRT), the significance of this risk has to be considered taking into account the existing pathology and the age of the patient as also further studies are needed to determine the weight of each contributor to the peripheral dose as also. As a concern, the results of the PD measurements during Cyberknife treatment, the mean preshielding PD, as a percentage of the prescribed dose (% TD) was 2.32 %, 0.63 % and 0.48 %, in the thyroid gland, the umbilicus and the pubic symphysis, respectively, since in the preshielding measurements the nipple was not monitored. The mean postshielding PD was 2.06 %, 0.65 %, 0.59 %, and 0.47 %, in the thyroid gland, the nipple, the umbilicus and the pubic symphysis, respectively. The risk for inducing secondary cancers can be considered low for the organs studied, by taking into account the existing pathology of the patients undergoing Cyberknife treatment. However, it should not be completely disregarded, especially in long term surviving patients, who are being treated for benign diseases or for curatively non metastatic malignancies. We also concluded that the increase of the collimator size during Cyberknife treatment corresponds to an increase of the PD and becomes less significant at larger distances, indicating that at these distances the PD is predominate due to the head leakage and the collimator scatter. Weighting the effect of the number of monitor units and the collimator size can be effectively used during the optimization procedure of Cyberknife in order to choose the most suitable treatment plan that will deliver the maximum dose to the tumor, while being compatible with the dose constraints for the surrounding organs at risk. Attention is required in defining the thyroid gland as a structure of avoidance in the treatment plan especially in patients with benign diseases. The most important advantages of the mobileMOSFET dosimeter are its small size, as it can be easily placed on the patient’s skin and the almost direct estimation of the dose during exposure. Moreover, its sensitivity and reproducibility make it suitable for measurements of low PD, as it provides an adequate measure of dose at low dose levels for high-energy photon beam irradiations used for therapy applications. However, attention should be given to the utilized Calibration Factor (CF), since its sensitivity is affected by the accumulated dose during its lifetime. / Σύμφωνα με τη παγκόσμια έκθεση καρκίνου, περίπου 50% όλων των ασθενών με καρκίνο θα υποβληθούν σε ακτινοθεραπεία σε κάποια φάση της θεραπείας τους. Ο κίνδυνος εμφάνισης δευτερογενούς καρκίνου σε σχέση με τις χαμηλές δόσεις της ιοντίζουσας ακτινοβολίας μπορεί να είναι μικρός αλλά όχι αμελητέος, κερδίζοντας ένα ιδιαίτερο ενδιαφέρον στην επιστημονική κοινότητα της ακτινοθεραπείας, επηρεάζοντας τον τρόπο επιλογής των υιοθετημένων θεραπειών. Η σκεδαζόμενη δόση, που αναπόφευκτα απορροφάται από τα ακτινοευαίσθητα όργανα που κείτονται εκτός του όγκου/στόχου, αναφέρεται στην βιβλιογραφία ως περιφερική δόση. Η περιφερική δόση είναι αποτέλεσμα διαφόρων δευτερογενών πηγών ακτινοβολίας. Συγκεκριμένα, προέρχεται από τη σκεδαζόμενη ακτινοβολία εσωτερικά του ασθενούς, από τη διαρρέουσα και σκεδαζόμενη ακτινοβολία από τα μηχανικά μέρη που συνθέτουν το γραμμικό επιταχυντή όπως είναι ο πρωτεύον και δευτερεύον κατευθυντήρας, το φίλτρο επιπεδότητας, οι τροποποιητές δέσμης (σφήνες, μπλοκς, πολλαπλά φύλλα κατευθυντήρα), καθώς επίσης από τη σκεδαζόμενη ακτινοβολία από τους τοίχους, το ταβάνι και το πάτωμα του χώρου όπου στεγάζεται το ακτινοθεραπευτικό μηχάνημα αλλά και τη διαρρέουσα ακτινοβολία από τα δευτερογενή νετρόνια που παράγονται από τις φωτοπυρηνικές αλληλεπιδράσεις όταν η ενέργεια των φωτονίων είναι μεγαλύτερη των 10 MV. Όλο και περισσότερες μοντέρνες τεχνικές χρησιμοποιούνται στην ακτινοθεραπεία τόσο καλοήθη όσο και κακοήθη όγκων, όπως είναι η στερεοτακτική ακτινοχειρουργική και ακτινοθεραπεία, όπου υψηλή δόση δίδεται στον όγκο/στόχο ανά συνεδρία (υποκλασματοποίηση), διατηρώντας σε πολύ χαμηλά επίπεδα την δόση στους υγιείς ιστούς. Η εκτίμηση της περιφερικής δόσης με αυτές τις τεχνικές γίνεται ένα από τα σημαντικότερα δοσιμετρικά θέματα που απασχολούν την ακτινοθεραπευτική κοινότητα και κυρίως εστιάζεται σε ασθενείς νεαρής ηλικίας, σε ασθενείς με καλοήθη όγκο καθώς επίσης σε ασθενείς με μεγάλο χρόνο βιωσιμότητας. Συγκεκριμένα, αυτή η διδακτορική διατριβή είναι η πρώτη μελέτη που αναφέρεται σε μέτρηση της περιφερικής δόσης σε ασθενείς που υποβλήθηκαν σε ενδοκρανιακή και εξωκρανιακή στερεοταξία με το ρομποτικό σύστημα του Cyberknife. Επίσης είναι η πρώτη μελέτη όπου οι μετρήσεις της περιφερικής δόσης διεξήχθησαν με το δοσίμετρο MOSFET, χρησιμοποιώντας το δοσιμετρικό σύστημα mobileMOSFET. Τα σημαντικότερα πλεονεκτήματα του δοσιμέτρου MOSFET είναι το μικρό του μέγεθος, δεδομένου ότι μπορεί εύκολα να τοποθετηθεί στο δέρμα του ασθενούς, καθώς και η σχεδόν άμεση εκτίμηση της δόσης στα ακτινοευαίσθητα όργανα κατά τη διάρκεια της έκθεσης τους. Επιπλέον, η ευαισθησία και η επαναληψημότητά του, το καθιστούν κατάλληλο δοσίμετρο για τη μέτρηση χαμηλού επιπέδου δόσεων, όπου συγκαταλέγεται και η περιφερική δόση. Δεν απαιτούνται πολλοί παράγοντες διόρθωσης, ωστόσο, ιδιαίτερη προσοχή πρέπει να δοθεί στο συντελεστή βαθμονόμησης (CF), καθώς η ευαισθησία του, επηρεάζεται από τη συσσωρευμένη δόση κατά τη διάρκεια της ζωής του. Αρχικά πραγματοποιήθηκαν μετρήσεις σε ομοίωμα νερού, προκειμένου να αναδειχθεί η συμπεριφορά της περιφερικής δόσης με την επίδραση διαφόρων παραμέτρων της θεραπείας όπως είναι η απόσταση (από την άκρη του πεδίου) και το βάθος, καθώς και από το μέγεθος του πεδίου και την ενέργεια φωτονίων που χρησιμοποιήσαμε, κάνοντας στη συνέχεια σύγκριση των αποτελεσμάτων μας με το θάλαμο ιονισμού. Έγιναν μετρήσεις περιφερικής δόσης σε ανθρωπόμορφο ομοίωμα, για πέντε κλινικές περιπτώσεις (ολοκρανιακή ακτινοβόληση, ακτινοβόληση πνεύμονα, ακτινοβόληση μαστού με και χωρίς τους υπερκλείδιους και μασχαλιαίους αδένες, ακτινοβόληση του ορθού και του προστάτη) προκειμένου να εκτιμηθεί η πιθανότητα εμφάνισης δευτερογενούς καρκίνου στα μάτια, στο θυροειδή αδένα, τις ωοθήκες και τις γονάδες. Πραγματοποιήθηκε σύγκριση των μετρήσεων του δοσιμετρικού συστήματος mobileMOSFET με τους υπολογισμούς περιφερικής δόσης του συστήματος σχεδιασμού πλάνου ISIS 3D. Σε πενήντα (50) ασθενείς που προσήλθαν στο Πανεπιστημιακό νοσοκομείου του Ρίου, προκειμένου να υποβληθούν σε τρισδιάστατη σύμμορφη ακτινοθεραπεία, πραγματοποιήθηκαν μετρήσεις περιφερικής δόσης σε δυο ιδιαίτερα ακτινοευαίσθητα όργανα όπως είναι ο θυροειδής αδένας και ο μαστός, προκειμένου να εκτιμηθεί η πιθανότητα εμφάνισης δευτερογενούς καρκίνου σε αυτά, με βάση το μοντέλο που προτείνει η Διεθνής Επιτροπή Ακτινοπροστασίας (ICRP 103). Τέλος, πραγματοποιήθηκαν μετρήσεις της περιφερικής δόσης σε 35 ασθενείς που υποβλήθηκαν σε ενδοκρανιακή και εξωκρανιακή στερεοταξία με το ρομποτικό στερεοτακτικό σύστημα του Cyberknife είτε για καλοήθης (ακουστικό νευρίνωμα, μηνιγγίωμα, αδένωμα υποφύσεως κτλ.) είτε για κακοήθης ασθένειες (αρτηριοφλεβώδης δυσπλασία, οστικές και εγκεφαλικές μεταστάσεις, γλοιώματα κτλ.), προκειμένου να εκτιμηθεί η πιθανότητα εμφάνισης δευτερογενούς καρκίνου στο θυροειδή αδένα, το μαστό, και στα όργανα που βρίσκονται στην περιοχή του οφαλού και της ηβικής σύμφυσης. Επίσης μελετήθηκε η συμπεριφορά της περιφερικής δόσης με και χωρίς την αναβάθμιση της θωρακίσεως του ρομποτικού συστήματος, καθώς επίσης και με την επίδραση του αριθμού των monitor units και του μεγέθους του κατευθυντήρα. Σύμφωνα με τα αποτελέσματα των μετρήσεων στο ομοίωμα του νερού, η περιφερική δόση εξαρτάται από τις παραμέτρους ακτινοβόλησης όπως είναι η απόσταση από την άκρη του πεδίου και το βάθος, καθώς επίσης από το μέγεθος του πεδίου και την εκάστοτε ενέργεια των φωτονίων που χρησιμοποιήθηκε. Κοντά στην άκρη του πεδίου ακτινοβόλησης, η εσωτερική σκέδαση του ασθενούς είναι η κυρίαρχη πηγή δευτερογενούς ακτινοβολίας ενώ όσο απομακρυνόμαστε από το πεδίο η σκεδαζόμενη ακτινοβολία από τα διάφορα μέρη του ακτινοθεραπευτικού μηχανήματος καθώς και η διαρρέουσα ακτινοβολία είναι οι σημαντικότερες πηγές δευτερογενούς ακτινοβολίας. Η περιφερική δόση μειώνεται σχεδόν εκθετικά με την απόσταση. Συγκεκριμένα, η περιφερική δόση είναι μεγάλη κοντά στην επιφάνεια, εν συνεχεία μειώνεται μέχρι το βάθος της μέγιστης δόσης και στη συνέχεια παραμένει σχεδόν σταθερή. Η αύξηση του μεγέθους του ακτινοβολούμενου πεδίου συνεισφέρει σε μεγαλύτερη περιφερική δόση λόγω του μεγαλύτερου όγκου σκέδασης ενώ μεγαλύτερη περιφερική δόση έχουμε και με την αύξηση της ενέργειας των φωτονίων που χρησιμοποιούμε. Από τις μετρήσεις που έγιναν με ανθρωπόμορφο ομοίωμα, προκύπτει ότι το σύστημα σχεδιασμού θεραπείας ISIS 3D υπερεκτιμά την περιφερική δόση σε σημεία που είναι αρκετά μακριά από τον εκάστοτε όγκο στόχο. Σύμφωνα με τα αποτελέσματα του μετρήσεων στους ασθενούς που υποβλήθηκαν σε τρισδιάστατη σύμμορφη ακτινοθεραπεία, η μέση περιφερική δόση στο θυρεοειδή αδένα, ως ποσοστό της χορηγηθήσας δόσης, είναι 1.43 %, 9.85 %, 7.27 % και 2.02 %, στην ολοκρανιακή ακτινοβολία, στην ακτινοβόληση του μεσοθωρακίου και στην ακτινοβόληση του μαστού με και χωρίς την ακτινοβόληση των υπερκλειδίων και των μασχαλιαίων αδένων, αντίστοιχα. Η πιθανότητα εμφάνισης δευτερογενούς καρκίνου στο θυρεοειδή αδένα εκτιμήθηκε στα επίπεδα του 0.18 %, 1.19 %, 1.18 % και 0.33 % αντίστοιχα. Η μέση περιφερική δόση του μαστού μετρήθηκε αντίστοιχα 5.90 %, 2.59 % και 3.14 % για την ακτινοβόληση του μεσοθωρακείου και την ακτινοβόληση του μαστού με και χωρίς την ακτινοβόληση των υπερκλειδίων και μασχαλιαίους, αντίστοιχα. Η πιθανότητα εμφάνισης δευτερογενούς καρκίνου στο μαστό εκτιμήθηκε στα επίπεδα του 3.97 %, 1.76 % και 1.45 %, αντίστοιχα. Αν και τα αποτελέσματα δείχνουν ότι δεν υπάρχει ιδιαίτερα αυξημένος κίνδυνος εμφάνισης δευτερογενούς καρκίνου στο θυρεοειδή αδένα και το μαστό με την τρισδιάστατη σύμμορφη ακτινοθεραπεία, ιδιαίτερη έμφαση πρέπει να δοθεί στους ασθενείς που είναι νέοι ηλικιακά καθώς και σε αυτούς που έχουν μεγάλη επιβιωσιμότητα. Τα αποτελέσματα των μετρήσεων στους ασθενείς που υποβλήθηκαν σε ενδοκρανιακή στερεοταξία με το ρομποτικό σύστημα του Cyberknife, είναι τα ακόλουθα. Η μέση περιφερική δόση, ως ποσοστό της χορηγηθήσας δόσης, πριν την αναβάθμιση της θωρακίσεως του συστήματος, μετρήθηκε σε 2.32 %, 0.63 % και 0.48 %, στο θυρεοειδή αδένα, την περιοχή του ομφαλού και της ηβικής σύμφυσης, αντίστοιχα. Η μέση περιφερική δόση, μετά την αναβάθμιση της θωρακίσεως του συστήματος, μετρήθηκε σε 2.06 %, 0.65 %, 0.59 %, και 0.47 %, στο θυρεοειδή αδένα, το μαστό, την περιοχή του ομφαλού και της ηβικής σύμφυσης, αντίστοιχα. Η πιθανότητα εμφάνισης δευτερογενούς καρκίνου στο θυροειδή αδένα και στο μαστό, εκτιμήθηκε περίπου σε 0.12 % και 0.14 %, αντίστοιχα, μετά την αναβάθμιση θωρακίσεως του συστήματος Cyberknife. Γενικά η πιθανότητα δευτερογενούς καρκίνου και στα δύο όργανα υψηλού κινδύνου είναι μικρή αν αναλογιστούμε και την εκάστοτη παθολογία των ασθενών που υποβλήθηκαν σε ενδοκρανιακή στερεοταξία με το ρομποτικό σύστημα του Cyberknife. Ωστόσο δε θα πρέπει να αγνοηθεί για τους ασθενείς που είναι νέοι ή έχουν καλοήθη πάθηση ή μεγάλο χρόνο βιωσιμότητας. Στην περίπτωση του θυροειδούς αδένα, όπου κείτεται κοντά στην περιοχή ακτινοβόλησης, η πιθανότητα αυτή μπορεί να αυξηθεί δραματικά αν οι δέσμες εξόδου περάσουν μέσα από αυτόν. Επομένως, ένα ερώτημα που τίθεται είναι αν ο θυροειδής αδένας κατά το σχεδιασμό της θεραπείας πρέπει να θεωρηθεί ή όχι ως όργανο κινδύνου. Τέλος, καθώς επιβεβαιώθηκε ότι η περιφερική δόση είναι ανάλογη του αριθμού των monitor units, η εκτίμησή της μπορεί να γίνει έμμεσα από τα monitor units για δεδομένη απόσταση που βρίσκεται το εκάστοτε όργανο κινδύνου από τον όγκο στόχο. Παράλληλα συμπεράναμε ότι όσο αυξάνεται το μέγεθος του κατευθυντήρα η περιφερική δόση αυξάνεται. Είναι προφανές λοιπόν ότι η επίδραση αυτών των δυο παραμέτρων στη περιφερική δόση πρέπει να ληφθεί υπόψη κατά τη διάρκεια σχεδιασμού ενός πλάνου θεραπείας από τον ακτινοφυσικό, προκειμένου να κάνει τη βελτιστοποίησει του πλάνου θεραπείας, επιλέγοντας εκείνο που θα δώσει την μέγιστη δόση στον όγκο/ στόχο χωρίς να υπερβεί τα όρια δόσης ανοχής των υγιών ιστών.

Este trabalho foi motivado por um estudo maio, proposto pela Agência Internacional de Energia Atômica (IAEA). O objetivo do trabalho foi estimar o kerma incidente (Ki) e a dose glandular média (Dg) em pacientes submetidas a mamografias nas projeções crânio-caudal (CC) e médio-lateral-oblíqua (MLO), nos sistemas de aquisição de imagens analógico e digital CR. A estimativa foi realizada através de cálculos matemáticos, tendo como base estudos computacionais utilizando simulações de Monte Carlo. Este estudo fez parte de um estudo maior em mamografia, coordenado pela IAEA, cujos dados fizeram parte da representação dos dados brasileiros no estudo da América Latina. Foram escolhidas mamografias cuja mama exposta tinha aproximadamente 50% de glandularidade e 50% de adiposidade. Dados da técnica radiográfica utilizada nos exames, assim como a espessura da mama comprimida, foram registrados em planilhas especificas e o cálculo foi realizado com base em testes de rendimento do tubo de raios X dos mamógrafos. Além disso, as mamografias acompanhadas foram analisadas quanto a critérios de qualidade da imagem. Foram acompanhadas 100 exposições, sendo 50 analógicas e d 50 digitais. Os resultados mostraram que as imagens foram predominantemente aceitas quanto aos critérios de qualidade da imagem estabelecidos pala IAEA, com melhores resultados do sistema digital. Os valores de Ki e Dg encontrados para o objeto simulador estavam de acordo com o recomendado, mas os calculados para as pacientes estavam mais altos, principalmente o Ki. O sistema digital obteve doses mais baixas e melhor qualidade de imagem. Os resultados sugerem que os exames devem ser realizados com o devido cuidado, de maneira a oferecer qualidade de imagem para o diagnóstico em doses tão baixas quanto razoavelmente exeqüíveis. O treinamento contínuo dos profissionais da mamografia deve ser realizado de maneira e oferecer exames adequados ao diagnóstico, protegendo os pacientes e mantendo a qualidade do serviço a todos. / This work has been motivated by a larger study, proposed by the International Atomic Energy Agency (IAEA). The aim of this work was to estimate the incident kerma (Ki) and mean glandular dose (Dg) in patients who underwent mammograms in craniocaudal projections (CC) and mediolateral-ablique (MLO), at analog and digital systems. The estimation was performed using mathematical calculations based on computational studies using Monte Carlo simulations. This study was part of a larger study in mammography, coordinated by the IAEA, whose data were included in the representation of Brazilian data in the study of Latin America. Mammograms with 50% of glandular tissue and 50% of fat were selected. Data from the radiographic technique used in the examinations, as well as the compressed breast thickness were recorded in spreadsheets and specific calculation was made based on output tests of the X-ray tube for mammography. In addition, the mammograms were analysed with the criteria of image quality. The amount of examinations was 100 mammograms, 50 analog and 50 digital. The results showed that the images were largely accepted as the criteria for image quality established by the IAEA, with better results from digital system. The values of Ki and Dg for the phantom were according to the recommended, but those calculate for the patients were higher, especially the Ki. Digital system produced lower dosis and better results on image quality. The results suggests that the examinations must be conducted with due care in order to offer image quality in dosis as low as reasonably achievable. The permanent training of mammographers should be conducted in a manner to provide exams with quality, protecting the patient and maintaining the quality of service to all patients treated.

Estudos recentes têm indicado o aumento da incidência de opacidade do cristalino para baixas doses de radiação. Considerando os dados epidemiológicos, a Comissão Internacional de Proteção Radiológica (ICRP) emitiu um comunicado que mudou o limite de dose absorvida para o cristalino. A publicação também recomenda a redução dos limites de dose equivalente para os indivíduos ocupacionalmente expostos, agora considerado de 20 mSv em um ano, em média, ao longo de cinco anos. Como consequência, algumas exposições planejadas requerem o uso de dosímetro adicional para estimar a dose no cristalino em profissionais. Este é o caso dos profissionais de radiologia intervencionista. Atualmente, as normas nacionais e internacionais, carecem de uma metodologia específica para a dosimetria em Hp(3). A recomendação ICRP provocou o debate sobre a adequação da grandeza equivalente de dose e sobre os métodos para as suas medições. Os objetivos deste trabalho foram: estudar a metodologia para a calibração de dosímetros pessoais em Hp(3) e monitorar profissionais durante os procedimentos de radiologia intervencionista. Diretrizes internacionais e recomendações da literatura recente foram adotadas para os procedimentos de calibração e testes. Para calibração, o sistema de dosimetria, que consiste em um suporte e um detector termoluminescente LiF:Mg,Cu,P (TLD-100H), foi exposto a radiações de referência em um fantoma cilíndrico preenchido com água, que se simulou a cabeça. Os fatores de calibração foram determinados para o potencial de tubo 20-150 kV da série 4037 estreito espectro de ISO. A monitoração individual foi realizada durante procedimentos vasculares de angioplastia e angiografia. Os resultados mostraram-se satisfatórios comparados à literatura. / Recent studies have indicated the increase of the incidence of lens opacities for low radiation doses. Considering epidemiological data, the International Commission on Radiological Protection (ICRP) issued a statement that changed the absorbed dose threshold for the eye lens. The statement also recommends a reduction in the dose limits to the eye lens for occupationally exposed persons; now it is considered to be 20 mSv in a year averaged over five years. As consequence, some planned exposures require the use of additional dosemeter for estimating eye lens dose in professionals; it is the case of the staff in interventional radiology. Nowadays, in the national and international standards there is a lack of specific methodology for eye lens dosimetry. The ICRP recommendation raised the debate on the adequacy of dose equivalent quantities of radiological protection and on the methods for their measurements. The objectives of this research were to study the methodology for calibrating personal dosemeters in Hp (3) and monitor professionals during interventional radiology procedures. International guidelines and recent literature were adopted for the calibration procedures and tests. For calibration, the dosimetric system, consisting of a holder and thermoluminescent detector LiF:Mg,Cu,P (TLD-100H), was exposed to standard radiation fields on a cylindrical water phantom that simulated the head. The calibration coefficients of the dosimetric system were determined for tube potential from 20 to150 kV of the ISO 4037 narrow spectrum series. The individual monitoring was performed during vascular procedures - angiography and angioplasty. The results were satisfactory were compared to the literature

<p>Traditional dosimetric devices are inherently point dose dosimeters (PDDs) and can only measure the magnitude of the radiation exposure; hence, they are one-dimensional (1D). To measure the magnitude and spatial location of dose within a volume either several PDDs must be used at one time, or one PDD must be translated from point-to-point. Using PDDs for spatially distributed, two-dimensional (2D), dosimetry is laborious, time consuming, limited in spatial resolution, susceptible to positioning errors, and the currently accepted approach to measuring dose distribution in 2D. This work seeks to expand the current limits of indirectly ionizing radiation dosimetry by using radiochromic film (RCF) for a high-resolution, accurate dosimetry system. Using RCF will extend the current field of radiation dosimetry to spatially quantitative 2D and three-dimensional (3D) measurements. </p> <p>This work was generalized into two aims. The first aim was the development of the RCF dosimetry system; it was accomplished by characterizing the film and the readout devices and developing a method to calibrate film response for absolute dose measurements. The second aim was to apply the RCF dosimetry system to three areas of dosimetry that were inherently volumetric and could benefit from multiple dimensional (2D or 3D) dose analysis. These areas were representative of a broad range of radiation energy levels and were: low-mammography, intermediate-computed tomography (CT), and high-radiobiologcal small animal irradiation and cancer patient treatment verification. The application of a single dosimeter over a broad range of energy levels is currently unavailable for most traditional dosimeters, and thus, was used to demonstrate the robustness and flexibility of the RCF dosimetry system.</p> <p>Two types of RCF were characterized for this work: EBT and XRQA film. Both films were investigated for: radiation interaction with film structure; light interaction with film structure for optimal film readout (densitometry) sensitivity; range of absorbed dose measurements; dependence of film dose measurement response as a function of changing radiation energy; fractionation and dose rate effects on film measurement response; film response sensitivity to ambient factors; and stability of measured film response with time. EBT film was shown to have the following properties: near water equivalent atomic weight (Z_eff); dynamic dose range of (10<super>-1</super>-10<super>2</super>) Gy; 3% change in optical density (OD) response for a single exposure level when exposed to radiation energies from (75-18,000) kV; and best digitized using transmission densitometry. XRQA film was shown to have: a Zeff of ~25; a 12 fold increase in sensitivity at lower photon energies for a dynamic dose range of 10-3-100 Gy, a difference of 25% in OD response when comparing 120 kV to 320 kV, and best digitized using reflective densitometry. Both XRQA and EBT films were shown to have: a temporal stability (&#916;OD) of ~1% for t > 24 hr post film exposure for up to ~20 days; a change in dose response of ~0.03 mGy hr-1 when exposed to fluorescent room lighting at standard room temperature and humidity levels; a negligible dose rate and fractionation effect when operated within the optimal dose ranges; and a light wavelength dependence with dose for film readout.</p> <p>The flat bed scanner was chosen as the primary film digitizer due to its availability, cost, OD range, functionality (transmission and reflection scanning), and digitization speed. As a cost verses functionality comparison, the intrinsic and operational limitations were determined for two flat bed scanners. The EPSON V700 and 10000XL exhibited equal spatial and OD accuracy. The combined precision of both the scanner light sources and CCD sensors measured < 2% and < 7% deviation in pixel light intensities for 50 consecutive scans, respectively. Both scanner light sources were shown to be uniform in transmission and reflection scan modes along the center axis of light source translation. Additionally, RCFs demonstrated a larger dynamic range in pixel light intensities, and to be less sensitive to off axis light inhomogeneity, when scanned in landscape mode (long axis of film parallel with axis of light source translation). The EPSON 10000XL demonstrated slightly better light source/CCD temporal stability and provided a capacity to scan larger film formats at the center of the scanner in landscape mode. However, the EPSON V700 only measured an overall difference in accuracy and precision by 2%, and though smaller in size, at the time of this work, was one sixth the cost of the 10000XL. A scan protocol was developed to maximize RCF digitization accuracy and precision, and a calibration fitting function was developed for RCF absolute dosimetry. The fitting function demonstrated a superior goodness of fit for both RCF types over a large range of absorbed dose levels as compared to the currently accepted function found in literature.</p> <p>The RCF dosimetry system was applied to three novel areas from which a benefit could be derived for 2D or 3D dosimetric information. The first area was for a 3D dosimetry of a pendant breast in 3D-CT mammography. The novel method of developing a volumetric image of the breast from a CT acquisition technique was empirically measured for its dosimetry and compared to standard dual field digital mammography. The second area was dose reduction in CT for pediatric and adult scan protocols. In this application, novel methodologies were developed to measure 3D organ dosimetry and characterize a dose reduction scan protocol for pediatric and adult body habitus. The third area was in the field of small animal irradiation for radiobiology purposes and cancer patient treatment verification. Two methods for small animal irradiation were analyzed for their dosimetry. The first technique was within a gamma irradiator environment using a <super>137</super>Cs source (663 keV), and the second, a novel approach to mouse irradiation, was developed for fast neutron (10 MeV) irradiated by a Tandem Van de Graff accelerator in a <super>2</super>H(d,n)<super>3</super>He reaction. For the patient cancer treatment, RCF was used to verify a 3D radiochromic plastic, PRESAGETM, using multi-leaf collimation (MLC) on a medical linear accelerator (LINAC) with 6 MV x-rays. The RCF and PRESAGE<super>TM</super> dosimeters were employed to verify a simple respiratory-gated lung treatment for a small nodule; the film was considered the gold standard. In every case, the RCF dosimetry system was verified for accuracy using a traditional PDD as the golden standard. When considering all areas of radiation energy applications, the RCF dosimetry system agreed to better than 7% of the golden standard, and in some cases within better than 1%. In many instances, this work provided vital dosimetric information that otherwise was not captured using the PDD in similar geometry. This work demonstrates the need for RCF to more accurately measure volumetric dose.</p> / Dissertation

A dynamic mathematical model was developed to simulate the response of polyacrylamide gel (PAG) dosimeters to a single spherical radioactive brachytherapy seed. Simulations were conducted for a high dose-rate (HDR) seed using 192Ir and a low dose-rate (LDR) seed using 125I. The model is able to predict the amount of polymer formed, the crosslink density, and the volume fraction of aqueous phase as a function of radial distance and time. Results show that PAG dosimeters can provide accurate HDR brachytherapy dosimetry at distances larger than 4 mm from the centre of the seed but will give poor results for LDR due to monomer diffusion. Experiments were conducted to evaluate the potential for using pentacosa-10,12-diynoic acid (PCDA) as the reporter molecule in micelle gel dosimeters for optical computed tomography (CT) readout. Several gels containing PCDA that was solubilized using sodium dodecyl sulfate (SDS) responded to radiation by changing from colourless to blue. Unfortunately, all phantoms that showed colour changes were turbid, making them unsuitable for optical CT scanning. Several techniques were used to produce transparent gels containing PCDA but none of these gels responded noticeably to radiation. Only turbid gels with precipitated PCDA responded, indicating that the colour change was due to oligomerization within PCDA crystals and that PCDA molecules solubilized in micelles did not undergo oligomerization. As a result, PCDA is not suitable for use in radiochromic micelle gel dosimeters. A new recipe for a radiochromic leuco crystal violet (LCV) micelle gel dosimeters with enhanced dose sensitivity was developed for optical CT readout. The recipe contains LCV, trichloro acetic acid (TCAA), Cetyl Trimethyl Ammonium Bromide (CTAB), 2,2,2-Trichloroethanol (TCE), and gelatin. Experiments were conducted to improve understanding about interactions between the different components of LCV micelle gel, highlighting the importance of pH on dose sensitivity and transparency. Results also showed the effectiveness of chlorinated compounds in improving dose sensitivity. Statistical techniques were used to build empirical models that were used to optimize the gel recipe. Additional testing in larger phantoms will be required to assess the effectiveness of the proposed gel for clinical dosimetry. / Thesis (Ph.D, Chemical Engineering) -- Queen's University, 2014-03-27 11:11:47.655