• 제목/요약/키워드: Bragg scattering

검색결과 42건 처리시간 0.023초

Physico-mechanical, AC-conductivity and microstructural properties of FeCl3 doped HPMC polymer films

  • Prakash, Y.;Somashekarappa, H.;Manjunath, A.;Mahadevaiah, Mahadevaiah;Somashekar, R.
    • Advances in materials Research
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    • 제2권1호
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    • pp.37-49
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    • 2013
  • The transition metal salt doped solid polymer electrolyte [TSPE] were prepared with HPMC as a host polymer. The virgin and doped films were prepared by solution-casting method and investigated using wide angle X-ray scattering method. Micro structural parameters like lattice strain (g%), stacking/twin faults, the average number of unit cells counted in a direction perpendicular to the Bragg's plane (hkl) spacing of (hkl) planes dhkl, crystallite size Ds, distortion width, standard deviation were determined by whole pattern powder fitting (WPPF) method, which is an extension of single order method. It is found that the crystallite size decreases with the increase in the content of $FeCl_3$. This decrease is due to increase in localized breaking of polymer network which also accounts for the amorphous nature of the material. The filler inorganic salt $FeCl_3$ acts as plasticizer. FTIR study also confirms and justifies the interaction between the polymer and in-organic salt in the matrix. Physical properties like mechanical stability and Ac conductivity in these films are in conformity with the X-ray results.

Localisation of embedded water drop in glass composite using THz spectroscopy

  • Mieloszyk, Magdalena;Majewska, Katarzyna;Ostachowicz, Wieslaw
    • Smart Structures and Systems
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    • 제21권6호
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    • pp.751-759
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    • 2018
  • Glass fibre reinforced polymers (GFRP) are widely exploited in many industrial branches. Due to this Structural Health Monitoring systems containing embedded fibre optics sensors are applied. One of the problems that can influence on composite element durability is water contamination that can be introduced into material structure during manufacturing. Such inclusion can be a damage origin significantly decreasing mechanical properties of an element. A non-destructive method that can be applied for inspection of an internal structure of elements is THz spectroscopy. It can be used for identifications of material discontinuities that results in changes of absorption, refractive index or scattering of propagating THz waves. The limitations of THz propagation through water makes this technique a promising solution for detection of a water inclusion. The paper presents an application of THz spectroscopy for detection and localisation of a water drop inclusion embedded in a GFRP material between two fibre optics with fibre Bragg grating sensors. The proposed filtering method allowed to determine a 3D shape of the water drop.

Numerical Investigation of Scattering from a Surface Dielectric Barrier Discharge Actuator under Atmospheric Pressure

  • Kim, Yuna;Kim, Sangin;Kim, Doo-Soo;Oh, Il-Young;Yook, Jong-Gwan
    • Journal of electromagnetic engineering and science
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    • 제18권1호
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    • pp.52-57
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    • 2018
  • Surface dielectric barrier discharge (SDBD), which is widely used to control turbulence in aerodynamics, has a significant effect on the radar cross-section (RCS). A four-way linearly synthesized SDBD air plasma actuator is designed to bolster the plasma effects on electromagnetic waves. The diffraction angle is calculated to predict the RCS because of the periodic structure of staggered electrodes. The simplified plasma modeling is utilized to calculate the inhomogeneous surface plasma distribution. Monostatic RCS shows the diffraction in the plane perpendicular to the electrode array and the notable distortion by plasma. In comparison, the overall pattern is maintained in the parallel plane with minor plasma effects. The trends also appear in the bistatic RCS, which has a significant difference in the observation plane perpendicular to the electrodes. The peaks by Bragg's diffraction are shown, and the RCS is reduced by 10 dB in a certain range by the plasma effect. The diffraction caused by the actuator and the inhomogeneous air plasma should be considered in designing an SDBD actuator for a wide range of application.

PTRAN 코드를 이용한 양성자선에 대한 물 흡수선량의 해석 (Absorbed Dose Analysis in Water for Proton Beam using PTRAN Code System)

  • 김진영;정동혁
    • 한국의학물리학회지:의학물리
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    • 제15권3호
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    • pp.140-148
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    • 2004
  • 본 연구에서는 PTRAN 전산코드를 사용하여 양성자에 대한 물 흡수선량의 분포를 계산하였다. 먼저 양성자와 물과의 상호작용에 대하여 정리하고 흡수선량의 계산과정에 대하여 기술하였다. 또한 PTRAN의 수송 알고리즘, 파일구조, 그리고 실행방법을 제시하였다. 본 결과에서는 양성자 에너지 60, 100, 150, 200, 250 WeV에 대하여 양성자에 의한 물 흡수선량의 분포가 쿨롱 상호작용과 핵반응의 합으로 주어지며, 브레그 봉우리의 형태가 에너지손실의 통계적 성질과 다중산란에 의존함을 보였다. 본 연구를 통하여 양성자에 대한 물 흡수선량의 구조 해석에 PTRAN 코드가 유용함을 알 수 있었다.

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원자짝 분포 함수를 이용한 칼슘 실리케이트 경화체의 나노 구조 변형 거동 해석 (Nanostructural Deformation Analysis of Tricalcium Silicate Paste by Atomic Pair Distribution Function)

  • 배성철;장유현;지현석
    • 한국건축시공학회:학술대회논문집
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    • 한국건축시공학회 2016년도 추계 학술논문 발표대회
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    • pp.94-95
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    • 2016
  • Calcium Silicate Hydrate (C-S-H), which takes up most of the hydration products of Portland Cement (PC), has the greatest impact on the mechanical behavior and strength development of concrete. The exact mechanism of its deformation, however, has not yet been elucidated. The present study aims to demonstrate the mechanism of nano-deformation behavior of C-S-H in tricalcium silicate paste under compressive loading, unloading and reloading by interpreting atomic pair distribution function (PDF) based on synchrotron X-ray scattering. The strain of the tricalcium silicate paste for a short-range of 0 ~ 20 Å under compressive load exhibited two stages, I) nano-packing of interlayer of C-S-H and II) micro-packing of C-S-H globules, whereas the deformation for a long-range order of 20 ~ 40 Å was similar to that of a calcium hydroxide phase measured by Bragg peak shift. Moreover, the residual strains due to the plastic deformation of C-S-H was clearly observed.

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레이저 유도 격자 분광장치 제작 및 $C_3H_8$화염에서 열 격자 측정 (Construction of laser induced grating spectrometer and measurement of thermal grating in $C_3H_8$ flame)

  • 박철웅;한재원;이중재;이영우;고동섭
    • 한국광학회지
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    • 제12권6호
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    • pp.446-451
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    • 2001
  • 레이저 유도 격자 분광장치를 제작하여, $C_3$ $H_{8}$ 층류 확산화염에서 생성된 열 격자 신호를 측정하였다. 열 격자를 생성시키기 위한 여기광은 파장이 532nm인 Nd:YAG 레이저를 사용하였고, 검침광은 488nm의 CW A $r^{+}$레이저를 이용하였다. 검침 광의 세기를 변화시켜 장치의 회절효율과 신호 특성을 측정하였다. 측정된 열 격자 신호의 세기를 분석하여 화염내의 매연의 농도 분포를 정성적으로 측정하였고, 신호의 주파수 변화를 측정하여 온도 분포를 구하였다.

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비고용 V-Cu계 MA합금의 중성자 및 X선 회절에 의한 상분석 (Phase Analysis of Immiscible V-Cu MA Powders by Neutron and X-ray Diffraction)

  • 이충효;조재문;이상진;김지순
    • 한국재료학회지
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    • 제14권5호
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    • pp.348-352
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    • 2004
  • The mechanical alloying (MA) effect in immiscible V-Cu system with positive heat of mixing was studied by not only the neutron and X-ray diffraction but also the analysis of DSC spectra. The total energy, ΔHt accumulated during MA for the mixture of $V_{50}$ $Cu_{50}$ / powders increased with milling time and approached the saturation value of 14 kJ/mol after 120 h of milling. It can be seen that the free energy difference between the amorphous phase and the pure V and Cu powders with an atomic ratio 5:5 is estimated to be 11 kJ/mol by Miedema et al. This is thermodynamically taken as one of the evidences for the amorphization. The structural changes of V-Cu MA powders were characterized by the X-ray diffraction and neutron diffraction. We take a full advantage of a negligibly small scattering length of the V atom in the neutron diffraction measurement. The neutron diffraction data definitely indicate that the amorphization proceeds gradually but incompletely even after 120 h of MA and bcc-Cu Bragg peaks appears after 60 h of MA.

Carbon-ion radiotherapy in osteosarcoma of the mandible: a case report

  • Ha, Tae-Wook;Park, Slmaro;Youn, Min Yeong;Kim, Dong Wook;Kim, Hyung Jun
    • Journal of the Korean Association of Oral and Maxillofacial Surgeons
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    • 제47권4호
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    • pp.315-320
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    • 2021
  • Carbon-ion radiotherapy (CIRT) is on the rise as a treatment choice for malignant tumor. Compared to conventional radiotherapy, particle beams have different physical and biological properties. Particle beam provides a low entry dose, deposits most of the energy at the endpoint of the flight path, and forms an asymptotic dose peak (the "Bragg peak"). Compared to protons, carbon with its larger mass decreases beam scattering, resulting in a sharper dose distribution border. We report a 50-year-old male who underwent CIRT without surgical resection on osteosarcoma of the mandible. After CIRT, the patient's pain was gone, and the malignant mass remained stable with accompanying necrosis. Nine months later, however, magnetic resonance imaging demonstrated progression of the left mandibular osteosarcoma with pulmonary metastases. After multidisciplinary discussion, concurrent chemoradiotherapy was conducted. While necrotic bone segments came out of the mandible during subsequent periodic outpatient visits, the tumor itself was stable. Thirty months after his first visit and diagnosis, the patient is waiting for chemotherapy. Although CIRT is superior in treating radioresistant hypoxic disease, CIRT is in its infancy, so care must be taken for its indications and complications.

Therapeutic Proton Beam Range Measurement with EBT3 Film and Comparison with Tool for Particle Simulation

  • Lee, Nuri;Kim, Chankyu;Song, Mi Hee;Lee, Se Byeong
    • 한국의학물리학회지:의학물리
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    • 제30권4호
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    • pp.112-119
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    • 2019
  • Purpose: The advantages of ocular proton therapy are that it spares the optic nerve and delivers the minimal dose to normal surrounding tissues. In this study, it developed a solid eye phantom that enabled us to perform quality assurance (QA) to verify the dose and beam range for passive single scattering proton therapy using a single phantom. For this purpose, a new solid eye phantom with a polymethyl-methacrylate (PMMA) wedge was developed using film dosimetry and an ionization chamber. Methods: The typical beam shape used for eye treatment is approximately 3 cm in diameter and the beam range is below 5 cm. Since proton therapy has a problem with beam range uncertainty due to differences in the stopping power of normal tissue, bone, air, etc, the beam range should be confirmed before treatment. A film can be placed on the slope of the phantom to evaluate the Spread-out Bragg Peak based on the water equivalent thickness value of PMMA on the film. In addition, an ionization chamber (Pin-point, PTW 31014) can be inserted into a hole in the phantom to measure the absolute dose. Results: The eye phantom was used for independent patient-specific QA. The differences in the output and beam range between the measurement and the planned treatment were less than 1.5% and 0.1 cm, respectively. Conclusions: An eye phantom was developed and the performance was successfully validated. The phantom can be employed to verify the output and beam range for ocular proton therapy.

Measurement of Proton Beam Dose-Averaged Linear Energy Transfer Using a Radiochromic Film

  • Seohyeon An;Sang-il Pak;Seonghoon Jeong;Soonki Min;Tae Jeong Kim;Dongho Shin;Youngkyung Lim;Jong Hwi Jeong;Haksoo Kim;Se Byeong Lee
    • 한국의학물리학회지:의학물리
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    • 제33권4호
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    • pp.80-87
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    • 2022
  • Purpose: Proton therapy has different relative biological effectiveness (RBE) compared with X-ray treatment, which is the standard in radiation therapy, and the fixed RBE value of 1.1 is widely used. However, RBE depends on a charged particle's linear energy transfer (LET); therefore, measuring LET is important. We have developed a LET measurement method using the inefficiency characteristic of an EBT3 film on a proton beam's Bragg peak (BP) region. Methods: A Gafchromic EBT3 film was used to measure the proton beam LET. It measured the dose at a 10-cm pristine BP proton beam in water to determine the quenching factor of the EBT3 film as a reference beam condition. Monte Carlo (MC) calculations of dose-averaged LET (LETd) were used to determine the quenching factor and validation. The dose-averaged LETs at the 12-, 16-, and 20-cm pristine BP proton beam in water were calculated with the quenching factor. Results: Using the passive scattering proton beam nozzle of the National Cancer Center in Korea, the LETd was measured for each beam range. The quenching factor was determined to be 26.15 with 0.3% uncertainty under the reference beam condition. The dose-averaged LETs were measured for each test beam condition. Conclusions: We developed a method for measuring the proton beam LET using an EBT3 film. This study showed that the magnitude of the quenching effect can be estimated using only one beam range, and the quenching factor determined under the reference condition can be applied to any therapeutic proton beam range.