• 제목/요약/키워드: Particle fluence

검색결과 29건 처리시간 0.026초

Characterization of saturation of CR-39 detector at high alpha-particle fluence

  • Ghazaly, M. El;Hassan, Nabil M.
    • Nuclear Engineering and Technology
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    • 제50권3호
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    • pp.432-438
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    • 2018
  • The occurrence of saturation in the CR-39 detector reduces and limits its detection dynamic range; nevertheless, this range could be extended using spectroscopic techniques and by measuring the net bulk rate of the saturated CR-39 detector surface. CR-39 detectors were irradiated by 1.5 MeV high alpha-particle fluence varying from $0.06{\times}10^8$ to $7.36{\times}10^8\;alphas/cm^2$ from Am-241 source; thereafter, they were etched in a 6.25N NaOH solution at a temperature of $70^{\circ}C$ for different durations. Net bulk etch rate measurement of the 1.5 MeV alpha-irradiated CR-39 detector surface revealed that rate increases with increasing etching time and reaches its maximum value at the end of the alpha-particle range. It is also correlated with the alpha-particle fluence. The measurements of UV-Visible (UV-Vis) absorbance at 500 and 600 nm reveal that the absorbance is linearly correlated with the fluence of alpha particles at the etching times of 2 and 4 hour. For extended etching times of 6, 10, and 14.5 hour, the absorbance is saturated for fluence values of $4.05{\times}10^8$, $5.30{\times}10^8$, and $7.36{\times}10^8\;alphas/cm^2$. These new methods pave the way to extend the dynamic range of polymer-based solid state nuclear track detectors (SSNTDs) in measurement of high fluence of heavy ions as well as in radiation dosimetry.

TIRE-LII 기법을 이용한 매연 입자 크기에 관한 수치적 연구 (Numerical Investigation on Soot Primary Particle Size Using Time Resolved Laser Induced Incandescence (TIRE-LII))

  • 김정용;이종호;정동수;전충환;장영준
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2004년도 추계학술대회
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    • pp.1152-1157
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    • 2004
  • Temporal behavior of the laser induced incandescence (LII) signal is often used for soot particle sizing, which is possible because the cooling behavior of a laser heated particle is dependent on the particle size. In present study, LII signals of soot particles are modeled using two non-linear coupled differential equations deduced from the energy- and mass-balance of the process. The objective of this study is to see the effects of particle size, laser fluence on soot temperature characteristics and cooling behavior. Together with this, we focus on validating our simulation code by comparing with other previous results. Results of normalized LII signals obtained from various laser fluence conditions showed a good agreement with that of Dalzell and Sarofim's. It could be found that small particles cool faster at a constant laser fluence. And it also could be observed that vaporization is dominant process of heat loss during first 100ns after laser pulse, then heat conduction played most important role while thermal radiation had little influence all the time.

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시분해 레이저 유도 백열법을 이용한 매연 입자 크기에 관한 수치적 연구 (Numerical Investigation on Soot Primary Particle Size Using Time Resolved Laser Induced Incandescence (TIRE-LII))

  • 이종호;김정용;정동수;장영준;전충환
    • 대한기계학회논문집B
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    • 제29권9호
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    • pp.1022-1031
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    • 2005
  • Temporal behavior of the laser induced incandescence (LII) signal is often used for soot particle sizing, which is possible because the cooling behavior of a laser heated particle is dependent on the particle size. In present study, LII signals of soot particles are modeled using two non-linear coupled differential equations deduced from the energy- and mass-balance of the process. The objective of this study is to obtain an appropriate calibration curve for determining primary particle size by comparing the gated signal ratio and double-exponential curve fitting methods. Not only the effects of laser fluence and gas temperature on the cooling behavior but also heat transfer mechanisms of heated soot particle have been investigated. The second-order exponential curve fitting showed better agreements with the LII signals than the gated signal ratio method which was based on the lust-order exponential curve fit. And the temporal decay rate of the LII signal and primary particle size showed nearly linear relationship, which was little dependent on the laser fluence. And it also could be reconfirmed that vaporization was dominant process of heat loss during first loons after laser pulse, then heat conduction played most important role while thermal radiation had little influence all the time.

Cellulose Nitrate의 알파입자비적특성(粒子飛跡特性) (Characteristics of Alpha Particle Track on Cellulose Nitrate Film)

  • 도진열;전재식;황선태
    • Journal of Radiation Protection and Research
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    • 제9권2호
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    • pp.61-66
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    • 1984
  • Cellulose nitrate 의 ${\alpha}$입자비적특성(粒子飛跡特性), 특(特)히 화학부식조건(化學腐蝕條件)에 따른 ${\alpha}$입자(粒子)의 비적직경(飛跡直徑)을 중심(中心)으로 연구(硏究)하였다. Cellulose nitrate의 KOH 용액부식(溶液腐蝕)때에는 동일(同一)한 부식조건하에(腐蝕條件下)에서 NaOH 경우보다 ${\alpha}$비적직경(飛跡直徑)이 약(約) 3배(培) 크게 나타났다. 그밖에 부식시간(腐蝕時間) 및 ${\alpha}$입자(粒子)의 에너지에 따른 비적직경(飛跡直徑)의 데이타를 얻었고, ${\alpha}$입자(粒子)의 조사조건(照射條件)이 같을 때 흘루언스율(率)(fluence rate)이 부식시간(腐蝕時間)에 무관(無關)함을 알았다.

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인광입자(Sr,Mg)2SiO4:Eu2+를 이용한 액체의 온도장 측정에 관한 연구 (Study on Temperature Field Measurement of Fluid using Phophor Particle (Sr,Mg)2SiO4:Eu2+)

  • 송동진;이현창
    • 한국가시화정보학회지
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    • 제17권3호
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    • pp.59-65
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    • 2019
  • Phosphor particles ((Sr,Mg)2 SiO4:Eu2+ were suspended in deionized water in quartz cuvette and used for measuring liquid temperature field by using two-color-ratio method. In the temperature range of 23~77℃, it showed the relative error from 2.4% to 4% and the temperature sensitivity of 0.65 %/℃ at 30℃ and 0.95 %/℃ at 77 ℃. This performance is comparable to measurement techniques using thermographic liquid crystal or laser induced fluorescence or other thermographic phosphor particle. Among investigated potential error sources, the particle number density affected the intensity ratio and the temperature, but the effect of laser fluence was not evident.

압밀 금속 마이크로 입자의 펄스 레이저 ABLATION에 의한 나노입자 합성 (Nanoparticle Synthesis by Pulsed Laser Ablation of Consolidated Microparticles)

  • 장덕석;오부국;김동식
    • 한국레이저가공학회지
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    • 제5권2호
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    • pp.31-38
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    • 2002
  • This paper describes the process of nanoparticle synthesis by laser ablation of consolidated microparticles. We have generated nanoparticles by high-power pulsed laser ablation of Al, Cu and Ag microparticles using a Q-switched Nd:YAG laser (wavelength 355 nm, FWHM 5 ㎱, fluence 0.8∼2.0 J/㎠). Microparticles of mean diameter 18∼80 ㎛ are ablated in the ambient air The generated nanoparticles are collected on a glass substrate and the size distribution and morphology are examined using a scanning electron microscope and a transmission electron microscope. The effect of laser fluence and collector position on the distribution of particle size is investigated. The dynamics of ablation plume and shock wave is analyzed by monitoring the photoacoustic probe-beam deflection signal. Nanosecond time-resolved images of the ablation process are also obtained by laser flash shadowgraphy. Based on the experimental results, discussions are made on the dynamics of ablation plume.

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Laser와 PZT - Target간의 반응과 그에 따른 Plume 형성 및 입자 방출에 관한 연구 (Interaction of Laser Beam with PZT - Target and Observation of Laser - Induced Plume and Particle Ejection)

  • 이병우
    • Journal of Advanced Marine Engineering and Technology
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    • 제20권5호
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    • pp.93-102
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    • 1996
  • Laser-induced plume and laser-target interaction during pulsed laser deposition are demonstrated for a lead zirconate titanate (PZT). A KrF excimer laser (wavelength 248nm) was used and the laser was pulsed at 20Hz, with nominal pulse width of 20ns. The laser fluence was~$16J/cm^2,$ with 100mJ per pulse. The laser-induced plasma plume for nanosecond laser irradiation on PZT target has been investigated by optical emission spectra using an optical multichannel analyzer(OMA) and by direct observation of the plume using an ICCD high speed photography. OMA analysis showed two distinct ionic species with different expansion velocities of fast or slow according to their ionization states. The ion velocity of the front surface of the developing plume was about $10^7$cm/sec and corresponding kinetic energy was about 100eV. ICCD photograph showed another kind of even slower moving particles ejected from the target. These particles considered expelled molten parts of the target. SEM morphologies of the laser irradiated targets showed drastic melting and material removal by the laser pulse, and also showed the evidence of the molten particle ejection. The physics of the plasma(plume) formation and particle ejection has been discussed.

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Simulation of the Determination of NaCl Concentration in Concrete samples by the Neutron induced Prompt Gamma-ray Method

  • Kim, Hyeon-Soo
    • 한국환경과학회지
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    • 제13권2호
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    • pp.175-180
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    • 2004
  • A prompt gamma-ray neutron activation (PGNA) system was simulated by the Monte Carlo N-Particle transport code (MCNP-4A) to estimate the level at which the scattered photon fluence rate, the absolute efficiency of the HPGe-detector, the volume of the concrete sample and the $^{35}$ /Cl(n, ${\gamma}$) reaction rate in this sample contribute to the count rate in the NaCl concentration measurement. The n- ${\gamma}$ fluence rates at the ST-2 beam tube exit of the HANARO reactor were used as input data, and the GAMMA-X type HPGe detector was modeled to tally 1.1649 MeV ${\gamma}$ -rays emitted from the $^{35}$ Cl(n, ${\gamma}$) reaction in the concrete sample. For three cylindrical concrete samples of 13.8, 46.8 and 157.1 ㎤ volumes, respectively, the relations between the NaCl weight fractions of 0.1, 1, 2 and 5 % in each of the concrete samples and the 1.1 649 MeV pulses created in the HPGe detector model were studied. As a result, it was found that the count rate at the same NaCl concentration nearly depends on the volume of the samples in a simulated condition of the same NaCl concentration samples, and that the linearities of the NaCl concentration calibration curves were reasonable in the narrow range of the NaCl weight fraction.

금속 마이크로입자 및 압밀 시편의 펄스레이저 어블레이션에 의한 나노입자 합성 (Nanoparticle Synthesis by Pulsed Laser Ablation of Metal Microparticle and Consolidated Sample)

  • 김동식;장덕석
    • 대한기계학회논문집B
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    • 제27권9호
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    • pp.1335-1341
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    • 2003
  • This paper describes the process of nanoparticle synthesis by laser ablation of microparticles and consolidated sample. We have generated nanoparticles by high-power pulsed laser ablation of AI, Cu and Ag microparticles using a Q-switched Nd:YAG laser (wavelength 355nm, FWHM 6ns, fluence $0.8{\sim}2.0J/cm^2$). Microparticles of mean diameter $18{\sim}80{\mu}m$ are ablated in the ambient air. The generated nanoparticles are collected on a glass substrate and the size distribution and morphology are examined using a scanning electron microscope and a transmission electron microscope. The effect of laser fluence, collector position and compacting pressure on the distribution of particle size is investigated. To better understand the process of laser ablation of microparticle(LAM), we investigated the Nd: YAG laser-induced breakdown of Cu microparticle using time-resolved optical shadow images. Nanosecond time-resolved images of the ablation process are also obtained by laser flash shadowgraphy. Based on the experimental results, discussions are made on the dynamics of ablation plume.

수계공정에 의한 알루미나 테이프로 제조한 세라믹 인공치관용 알루미나 유리 복합체의 기계적 물성 (Mechanical Properties of Alumina-Glass Dental Composites Prepared from Aqueous-Based Tape Casting)

  • 이명현;김대준;이득용;이정훈;김창은
    • 한국세라믹학회지
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    • 제36권10호
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    • pp.1123-1131
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    • 1999
  • Alumina-glass composites which are considered as the material of the choice for all dental crown was prepared by aqeous-based tape casting and sintering for 2h at 1120$^{\circ}C$ followed by glass infiltration for 2h at 1100$^{\circ}C$ Biaxial strength and fracture toughness of the composites were evaluated to determine the optimum composition of the tape as a function of the amount of constituent such as alumina binder and plasticizer. The strength and the fracture toughness of the alumina tape increased with increasing the contents of alumina and binder. These observations are consistent with in fluence of the constituents on mean alumuna particle distance in tapes suggesting that high strength of the glass infiltrated alumina composites is related to toughening by crack bowing. The biaxial strength and the fracture toughness of the composite containing the optimum constituent composition were 523 MPa and 3.3 MPa$.$1/2 respectively.

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