• 한국의학물리학회:학술대회논문집
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• 한국의학물리학회 2002년도 Proceedings
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• pp.121-122
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• 2002

The main principle of radiation therapy is to deliver optimum dose to tumor to increase tumor cure probability while minimizing dose to critical normal structure to reduce complications. RTP system is required for proper dose plan in radiation therapy treatment. The main goal of this research is to develop dose model for photon, electron, and brachytherapy, and to display dose distribution on patient images with optimum process. The main items developed in this research includes: (l) user requirements and quality control; analysis of user requirement in RTP, networking between RTP and relevant equipment, quality control using phantom for clinical application (2) dose model in RTP; photon, electron, brachytherapy, modifying dose model (3) image processing and 3D visualization; 2D image processing, auto contouring, image reconstruction, 3D visualization (4) object modeling and graphic user interface; development of total software structure, step-by-step planning procedure, window design and user-interface. Our final product show strong capability for routine and advance RTP planning.

• Journal of Radiation Protection and Research
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• 제20권4호
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• pp.227-236
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• 1995

선량데이타와 정확한 3차원 선량모델을 이용하여 여러 아크에 대한 선량분포를 조사하였다. 정확한 선량모델에 의해 계산된 선량 값은 판단한 실험식으로 표현이 가능했으며 이는 선량 최적화 과정에서 반복적으로 선량 값을 계산하는데 매우 유용하였다. 360도 아크와 부분 아크에 대한 선량 값을 빠른 속도로 계산하기 위하며 실험적으로 구해진 실린더형 선량모델을 개발하였다. 200개 위치의 정확한 선량 값을 비선형식으로 피팅하여 7개의 변수를 포함하는 실험식을 개발하였다. 결과적으로 이 모델을 이용하는 경우 한 아크에 대한 선량 계산시 400개의 위치를 계산하는데 PC-486으로 1초 이내에서 계산이 가능하였다. 결론적으로 개발된 고속선량모델은 정확한 선량모델에 의한 선량 값과 유사한 값을 제공함으로써 계간속도가 늦은 일반 3차원 선량모델을 대치할 수 있을 것으로 사려된다.

• Nuclear Engineering and Technology
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• 제51권5호
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• pp.1436-1443
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• 2019

A fast gamma-ray dose rate assessment method for complex geometries based on stylized model reconstruction and point-kernel method is proposed in this paper. The complex three-dimensional (3D) geometries are imported as a 3DS format file from 3dsMax software with material and radiometric attributes. Based on 3D stylized model reconstruction of solid mesh, the 3D-geometrical solids are automatically converted into stylized models. In point-kernel calculation, the stylized source models are divided into point kernels and the mean free paths (mfp) are calculated by the intersections between shield stylized models and tracing ray. Compared with MCNP, the proposed method can implement complex 3D geometries visually, and the dose rate calculation is accurate and fast.

• 한국의학물리학회지:의학물리
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• 제10권2호
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• pp.103-114
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• 1999

본 연구에서는 외부조사 광자선에 대한 3차원 선량계산 알고리즘 모델을 개발하기 위한 기초 연구로서 기존의 2D 선량 계산 알고리즘을 확장시켜 비동일 평면 조사가 가능한 2.5D 선량계산 모델을 개발하였다. 이를 위해 3차원 치료계획 및 선량계산에 적합하도록 환자 및 조사빔에 대한 3차원 좌표계 시스템을 정의하고, 이들 간의 좌표변환식을 유도하였다. 선량계산 알고리즘으로는 "Clarkson-Cunningham" 의 2D 광자선량 계산 알고리즘을 3차원으로 확장시켜 정형 조사면 및 비정형 조사면에 대한 선량계산과 wedge filter에 대한 선량계산이 가능하도록 하였고, Batho 방식을 적용하여 비 균질 보정을 구현하였다. 선량계산의 정확도를 평가하기 위해, AAPM TG #23 에 제시된 절차에 따라 자료에 제시된 4MV 광자선에 대한 실험 값과 본 연구에서 계산된 결과를 비교한 결과, 정형조 사면에 대한 PDD(percent depth dose)는 buildup 영역을 제외하면 $\pm$1% 이내, 비정형 조사면의 경우 $\pm$3% 이내에서 실험값과 일치하였다. 또한, wedge filter에 대한 PDD 및 profile은 $\pm$3% 이내, 45$^{\circ}$ oblique 입사빔에 대한 선량은 $\pm$4% 이내에서 실험값과 일치하였다. 비균질 보정의 경우 Lung/water 경계에서 7% 과소 평가되었고, Bone/water 경계에서 3% 과대 평가되는 것으로 나타났다. 이들 결과를 종합해 볼 때, 비균질 보정을 제외하고는 비교적 정확하게 선량을 계산하는 것으로 평가되었다. 추후 대부분의 상용 2.5D 치료계획시스템 (radiation treatment planning system; RTP)들이 비균질 보정 방법으로 사용하고 있는 Equivalent TAR(tissue-air ratio) 방식을 구현시키고자 하며, 본 연구에서 구현된 선량계산 모듈을 교육 및 연구용으로 활용할 수 있을 것으로 기대 한다.것으로 기대 한다.

• Radiation Oncology Journal
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• 제20권1호
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• pp.1-16
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• 2002

Purpose : Three dimensional conformal radiotherapy planning is being used widely for the treatment of patients with brain tumor. However, it takes much time to develop an optimal treatment plan, therefore, it is difficult to apply this technique to all patients. To increase the efficiency of this technique, we need to develop standard radiotherapy plant for each site of the brain. Therefore we developed several 3 dimensional conformal radiotherapy plans (3D plans) for tumors at each site of brain, compared them with each other, and with 2 dimensional radiotherapy plans. Finally model plans for each site of the brain were decide. Materials and Methods : Imaginary tumors, with sizes commonly observed in the clinic, were designed for each site of the brain and drawn on CT images. The planning target volumes (PTVs) were as follows; temporal $tumor-5.7\times8.2\times7.6\;cm$, suprasellar $tumor-3\times4\times4.1\;cm$, thalamic $tumor-3.1\times5.9\times3.7\;cm$, frontoparietal $tumor-5.5\times7\times5.5\;cm$, and occipitoparietal $tumor-5\times5.5\times5\;cm$. Plans using paralled opposed 2 portals and/or 3 portals including fronto-vertex and 2 lateral fields were developed manually as the conventional 2D plans, and 3D noncoplanar conformal plans were developed using beam's eye view and the automatic block drawing tool. Total tumor dose was 54 Gy for a suprasellar tumor, 59.4 Gy and 72 Gy for the other tumors. All dose plans (including 2D plans) were calculated using 3D plan software. Developed plans were compared with each other using dose-volume histograms (DVH), normal tissue complication probabilities (NTCP) and variable dose statistic values (minimum, maximum and mean dose, D5, V83, V85 and V95). Finally a best radiotherapy plan for each site of brain was selected. Results : 1) Temporal tumor; NTCPs and DVHs of the normal tissue of all 3D plans were superior to 2D plans and this trend was more definite when total dose was escalated to 72 Gy (NTCPs of normal brain 2D $plans:27\%,\;8\%\rightarrow\;3D\;plans:1\%,\;1\%$). Various dose statistic values did not show any consistent trend. A 3D plan using 3 noncoplanar portals was selected as a model radiotherapy plan. 2) Suprasellar tumor; NTCPs of all 3D plans and 2D plans did not show significant difference because the total dose of this tumor was only 54 Gy. DVHs of normal brain and brainstem were significantly different for different plans. D5, V85, V95 and mean values showed some consistent trend that was compatible with DVH. All 3D plans were superior to 2D plans even when 3 portals (fronto-vertex and 2 lateral fields) were used for 2D plans. A 3D plan using 7 portals was worse than plans using fewer portals. A 3D plan using 5 noncoplanar portals was selected as a model plan. 3) Thalamic tumor; NTCPs of all 3D plans were lower than the 2D plans when the total dose was elevated to 72 Gy. DVHs of normal tissues showed similar results. V83, V85, V95 showed some consistent differences between plans but not between 3D plans. 3D plans using 5 noncoplanar portals were selected as a model plan. 4) Parietal (fronto- and occipito-) tumors; all NTCPs of the normal brain in 3D plans were lower than in 2D plans. DVH also showed the same results. V83, V85, V95 showed consistent trends with NTCP and DVH. 3D plans using 5 portals for frontoparietal tumor and 6 portals for occipitoparietal tumor were selected as model plans. Conclusion : NTCP and DVH showed reasonable differences between plans and were through to be useful for comparing plans. All 3D plans were superior to 2D plans. Best 3D plans were selected for tumors in each site of brain using NTCP, DVH and finally by the planner's decision.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1991년도 하계학술대회 논문집
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• pp.753-756
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• 1991

This paper aimed to analyse dose sensitivity to the controllable parameters of in-door radon $(^{222}Rn)$ and its decay products(Rn-D) by applying the input-output linear system theory. Physical behaviors of $^{222}Rn$ & Rn-D were analyzed in terms of $^{222}Rn$ gas generation, -migation and - infiltration to indoor environments, and the performance output-function(i.e. mean dose equivalent to Tracho-Bronchial(TB) lung region was assessed to the following ranges of the controllable parameters; a) the ventilation rate constant $({\lambda}_v)$ : $0{\sun}500[h^{-1}]$. b) the attachment rate constant$({\lambda}_a)$ : 0-500 $[h^{-1}]$. c) deposition rate constant $({\lambda}{_{d}^{u}})$: 0-50$[h^{-1}]$. A linear input-output model was reconstructed from the original models in literatures, as follows, which was modified into the matrices consisting of 111 nodal equations. a) indoor ${222}Rn$ & Rn-D Behaviour: jacobi- Porstendorfer- Bruno model. b) lung dosimerty : Jacobi-Eisfeld model. Some of the major findings, which identify the effectiveness of this model, were as follows. a) ${\lambda}_v$ is most effective, dominant controllable parameters in dose reduction, if mechanical ventilation is applied. b) ${\lambda}_v$, depending on the air particle-concentration, reduces the dose somewhat within ${\lambda}_v$<1 $h^{-1}R range. However, the dose increases conversely, ${\lambda}_v$>1 $h^{-1}R range range. c) ${\lambda}{_{d}^{4}}$ reduces the dose linearly as ${\lambda}_v$ dose. Such dose(z-axis) sentivities are shown with three-dimensional plots whoes x,y-axes are combined 2out the 3 parameter${\lambda}_v{\lambda}_s,\;{\lambda}_d^s$.

• 대한방사선기술학회지:방사선기술과학
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• 제41권6호
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• pp.561-566
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• 2018

Field-in-Field Technique is applied to the radiation therapy of breast cancer patients, and it is possible to compensate the difference in breast thickness and deliver uniform dose in the breast. However, there are several fields in the treatment field that result in a more complex dose delivery than a single field dose delivery. If the patient's respiration is irregular during the delivery of the dose by several fields and the change of respiration occurs, the dose distribution in the breast changes. Therefore, based on the computed tomography images of breast cancer patients, a human model was created by using a 3D printer (Builder Extreme 1000) to describe the volume in the same manner. A computerized tomography (CT) of the human body model was performed and a treatment plan of 260 cGy / fx was established using a 6-MV field-in-field technique using a computerized treatment planning system (Eclipse 13.6, Varian, USA). The distribution of the dose in the breast according to the change of the respiration was measured using a moving phantom at 0.1 cm, 0.3 cm, 0.5 cm amplitude, using a MOSOXIDE Silicon Field Effect Transistor (MOSFET, Best Medical, Canada) Were measured and compared. The distribution of dose in the breast according to the change of respiration showed similar value within ${\pm}2%$ in the movement up to 0.3 cm compared to the treatment plan. In this experiment, we found that the dose distribution in the breast due to the change of respiration when the change of respiration was increased was not much different from the treatment plan.

• 한국기계가공학회지
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• 제17권2호
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• pp.47-53
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• 2018

Nowadays, additive manufacturing (AM) technology is a promising process to fabricate complex shaped devices applied in medical and dental services. Among the AM processes, a DLP (digital light processing) type 3D printing process has some advantages, such as high precision, relatively low cost, etc. In this work, we propose a simple method to fabricate precise dental models using a DLP 3D printer. After 3D printing, a part is commonly post-cured using secondary UV-curing equipment for complete polymerization. However, some shrinkage occurs during the post-curing process, so we adaptively control the UV-exposure time on each layer for over- or under-curing to change the local shape-size of a part in the DLP process. From the results, the shrinkage amounts in the post-curing process vary due to the UV-dose in 3D printing. We believe that the proposed method can be utilized to fabricate dental models precisely, even with a change of the 3D CAD model.

• Asian Pacific Journal of Cancer Prevention
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• 제15권13호
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• pp.5259-5264
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• 2014

Background: CT based brachytherapy allows 3-dimensional (3D) assessment of organs at risk (OAR) doses with dose volume histograms (DVHs). The purpose of this study was to compare computed tomography (CT) based volumetric calculations and International Commission on Radiation Units and Measurements (ICRU) reference-point estimates of radiation doses to the bladder and rectum in patients with carcinoma of the cervix treated with high-dose-rate (HDR) intracavitary brachytherapy (ICBT). Materials and Methods: Between March 2011 and May 2012, 20 patients were treated with 55 fractions of brachytherapy using tandem and ovoids and underwent post-implant CT scans. The external beam radiotherapy (EBRT) dose was 48.6Gy in 27 fractions. HDR brachytherapy was delivered to a dose of 21 Gy in three fractions. The ICRU bladder and rectum point doses along with 4 additional rectal points were recorded. The maximum dose ($D_{Max}$) to rectum was the highest recorded dose at one of these five points. Using the HDRplus 2.6 brachyhtherapy treatment planning system, the bladder and rectum were retrospectively contoured on the 55 CT datasets. The DVHs for rectum and bladder were calculated and the minimum doses to the highest irradiated 2cc area of rectum and bladder were recorded ($D_{2cc}$) for all individual fractions. The mean $D_{2cc}$ of rectum was compared to the means of ICRU rectal point and rectal $D_{Max}$ using the Student's t-test. The mean $D_{2cc}$ of bladder was compared with the mean ICRU bladder point using the same statistical test. The total dose, combining EBRT and HDR brachytherapy, were biologically normalized to the conventional 2 Gy/fraction using the linear-quadratic model. (${\alpha}/{\beta}$ value of 10 Gy for target, 3 Gy for organs at risk). Results: The total prescribed dose was $77.5Gy{\alpha}/{\beta}10$. The mean dose to the rectum was $4.58{\pm}1.22Gy$ for $D_{2cc}$, $3.76{\pm}0.65Gy$ at $D_{ICRU}$ and $4.75{\pm}1.01Gy$ at $D_{Max}$. The mean rectal $D_{2cc}$ dose differed significantly from the mean dose calculated at the ICRU reference point (p<0.005); the mean difference was 0.82 Gy (0.48-1.19Gy). The mean EQD2 was $68.52{\pm}7.24Gy_{{\alpha}/{\beta}3}$ for $D_{2cc}$, $61.71{\pm}2.77Gy_{{\alpha}/{\beta}3}$ at $D_{ICRU}$ and $69.24{\pm}6.02Gy_{{\alpha}/{\beta}3}$ at $D_{Max}$. The mean ratio of $D_{2cc}$ rectum to $D_{ICRU}$ rectum was 1.25 and the mean ratio of $D_{2cc}$ rectum to $D_{Max}$ rectum was 0.98 for all individual fractions. The mean dose to the bladder was $6.00{\pm}1.90Gy$ for $D_{2cc}$ and $5.10{\pm}2.03Gy$ at $D_{ICRU}$. However, the mean $D_{2cc}$ dose did not differ significantly from the mean dose calculated at the ICRU reference point (p=0.307); the mean difference was 0.90 Gy (0.49-1.25Gy). The mean EQD2 was $81.85{\pm}13.03Gy_{{\alpha}/{\beta}3}$ for $D_{2cc}$ and $74.11{\pm}19.39Gy_{{\alpha}/{\beta}3}$ at $D_{ICRU}$. The mean ratio of $D_{2cc}$ bladder to $D_{ICRU}$ bladder was 1.24. In the majority of applications, the maximum dose point was not the ICRU point. On average, the rectum received 77% and bladder received 92% of the prescribed dose. Conclusions: OARs doses assessed by DVH criteria were higher than ICRU point doses. Our data suggest that the estimated dose to the ICRU bladder point may be a reasonable surrogate for the $D_{2cc}$ and rectal $D_{Max}$ for $D_{2cc}$. However, the dose to the ICRU rectal point does not appear to be a reasonable surrogate for the $D_{2cc}$.

• 한국의학물리학회지:의학물리
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• 제25권2호
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• pp.100-109
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• 2014

정위신체방사선치료(SBRT)에서 환자의 호흡에 대한 정확한 치료위치의 확보는 필수적으로 고려되어야 하며 그 정확성에 관련하여 많은 연구들이 진행되어왔다. 본 연구에서는 실제 호흡에 의한 움직임과 실제 환자 폐의 형태를 고려한 팬텀실험으로 실제 치료에서 일어나는 임상적 상황을 모사함으로 호흡 동조 부피적조절회전 방사선치료(Volumeric Modulated Arc Therapy, VMAT) 기법을 이용한 폐부 SBRT의 정확성을 분석하는 방법을 제시하고자 하였다. SBRT을 받은 폐암 환자의 CT 영상을 기반으로 3D 프린터를 이용하여 치료부위와 유사하게 폐 팬텀을 제작하였고 환자 호흡과 동일하게 움직임을 재현할 수 있도록 $QUASAR^{TM}$ 호흡 동조 구동 팬텀(Modus Medical Devices, London, Canada)에 장착하여 호흡동조 VMAT에서의 2차원 선량 분포를 평가할 수 있는 시스템을 구축하였다. 폐 팬텀은 종양부위를 중심으로 2등분하여 EBT3 필름을 삽입하고 선량분포를 측정할 수 있도록 제작되었다. 비균질 조건에서의 선량계산의 정확성을 확인하기 위하여 균질한 플라스틱 팬텀과 제작된 비균질 폐 팬텀에서 Analytical Anisotropic Algorithm (AAA)와 AcurosXB (AXB) 두가지 알고리즘으로 선량계산을 하여 비교, 분석하였다. 움직임에 대한 치료의 정확성을 평가하기 위하여 호흡동조와 비 호흡동조의 경우, 그리고 움직임이 없는 조건에서 선량분포를 취득하여 치료계획 선량에 대한 감마지표를 분석하였다. 치료부위 GTV에서의 CT number는 실제 환자의 경우 78 HU를 나타내었고 모사된 폐 팬텀의 경우 92 HU를 나타내었다. 팬텀 내 폐 조직부분은 3D프린터로 적층하는 과정에서 격자구조의 형태를 이용하여 구현하였다. 측정된 필름선량은 AAA 알고리즘을 이용한 치료계획 선량에 대하여 움직이는 팬텀에서 호흡동조의 유무에 따라 3%/3 mm 감마지표 조건하에서 각각 88%와 78%의 감마합격률을 나타내었으며, 움직임이 없는 경우 95% 이상의 감마합격률을 보였다. AXB 알고리즘을 적용하였을 경우에는 모든 경우에서 98% 이상의 합격률을 나타내었다. 균질한 플라스틱 팬텀에 대하여 측정하였을 때 두가지 선량계산 알고리즘을 포함한 모든 조건에서 99% 이상의 감마합격률을 나타내었다. 선택된 환자의 호흡 진폭이 비교적 작고 inhale보다는 exhale에 더 오래 머무르는 호흡패턴 때문에 3%/3 mm 감마 기준에서는 호흡에 따른 차이가 거의 나타나지 않은 것으로 이해되었다. 선량계산의 정확성에서는 AAA 알고리즘을 적용하였을 때보다 AXB 알고리즘을 적용하였을 때가 균질과 비균질 환경에서의 선량 분포에 따른 감마 합격률의 차이가 적게 나타남을 확인 할 수 있었다. 본 논문에서는 환자와 유사하게 제작된 폐 팬텀에 실제 환자 호흡 패턴을 연동함으로 새로운 4D 치료선량 분포 검증 방법을 제시하였고 보다 사실적인 선량분포를 반영한 개별 환자 치료의 정확성 검증이 가능할 것으로 평가되었다.