• 콘크리트학회논문집
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• 제12권2호
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• pp.31-42
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• 2000

This paper discusses the validity of models predicting the compressive strength of concrete subjected to various temperature histories and the shortcomings of existing rate constant model and apparent activation energy concept. Based on the discussion, a modified rate constant model is proposed. The modified rate constant model, in which apparent activation energy is a nonlinear function of curing temperature and age, accurately estimates the development of the experimental compressive strengths by a few researchers. Also, the apparent activation energy of concrete cured with high temperature decreases rapidly with age, but that of concrete cured with low temperature decreases gradually with age. Finally generalized models to predict apparent activation energy and compressive strength are proposed, which are based on the regression results.

• 동력기계공학회지
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• 제20권4호
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• pp.38-43
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• 2016

Safety-related equipments of Nuclear Power Plants(NPP) have to perform environmental qualification test in accordance with IEEE-323 standards. However, non-metallic materials replace new one regularly instead of the test because they are considered as consumable parts. In this study, the seven kinds of non-metallic materials are selected and their activation energy was experimentally evaluated with uncertainty analysis by using thermogravimetric analyzer(TGA). In order to obtain activation energy of non-metallic materials, mass difference, temperature raising rate and conversion rate on the specimen are analyzed. It is postulated that the three experiment conditions are important to get a reliable activation energy. This postulate was experimentally confirmed using Arrhenius equation and Flynn-Wall-Ozawa analysis.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1995년도 추계학술대회 논문집
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• pp.163-166
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• 1995

It was investigated the properties of TSC (Thermally Stimulated Current) to understand carriers behavior from long ago. Activation Energy of their properties is very important to verify electrical characteristics. So, for many years, many researchers were worked to get the activation energy, more compeletely. But, if boundary conditions were not satisfied, the values of activation energy contained several errors. In this work, to obtain the activation energy related to charged particles, the peak temperature Tp and the slope of tangential line on any coordinates of Arrhenius plot are applied. The calculation process can be denied with by computer, and the result of observation shows that the cures of calculation data and simulation data coincide very compeletely.

• 에너지공학
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• 제5권2호
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• pp.170-175
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• 1996

국내 석탄화력발전소에서 사용되고 있는 3종류의 유연탄 및 무연탄에 대해 입자 크기와 CaCO$_3$ 주입에 따른 TGA 분석을 수행하고 활성화에너지를 구하였다. 유연탄의 무게감량 시작온도는 360-38$0^{\circ}C$로 무연탄의 570~$600^{\circ}C$보다 20$0^{\circ}C$정도 낮았다. 유연탄의 활성화에너지는 입도 및 탄종에 따라 14~20kcal/mole 범위이고 무연탄은 37~55 kcal/mole로서 무연탄이 유연탄보다 활성화에너지가 매우 높았다. 석탄의 입도크기가 작아질수록 활성화에너지는 감소하였고 무게감량율과 활성화에너지값은 상관관계가 있었다. 유 무연탄의 유황분대 CaCO$_3$비율을 1:1로 주입시 유연탄은 활성화에너지 변화가 작았으나 무연탄의 경우 1~23 kcal/mole 정도로 활성화에너지가 감소하였다.

• 공업화학
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• 제23권3호
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• pp.352-357
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• 2012

1,3,5-trinitro-1,3,5-triazacylohexane (RDX)와 octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine (HMX)의 입자크기에 대한 열적 특성을 알아보기 위해서 DSC (Differential Scanning Calorimetry)와 TGA (Thermo-Gravimetric Analysis)를 사용하였다. 활성화 에너지와 빈도인자는 Kissinger 방법과 Vyazovkin 방법으로 계산하였다. DSC를 이용할 경우 RDX의 경우에는 고에너지 분자화약의 높은 분해열에 의하여 입자크기에 따른 활성화에너지의 경향성이 없었으나, TGA를 이용할 경우 입자크기가 클수록 활성화에너지가 커짐을 알 수 있었다. 그러나 HMX의 경우에는 DSC와 TGA의 방법 모두 입자 크기에 따라 활성화 에너지가 커지는 경향성을 보였다. 또한, Vyazovkin 방법을 이용하여 RDX와 HMX의 분해정도에 따른 활성화 에너지의 변화로 분해반응의 메커니즘을 이해할 수 있었다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 하계학술대회 논문집
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• pp.436-436
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• 2009

현재 상용화되어 있는 결정질 태양전지의 경우 높은 실리콘 가격으로 인해 저가화에 어려움을 격고 있다. 따라서 태양전지 저가화의 한 방법으로 박막태양전지가 주목을 받고 있다. P-I-N 구조의 박막태양전지에서 각 층의 thickness, activation energy, energy bandgap은 고효율 달성을 위한 중요한 요소이다. 본 논문에서는 박막태양전지 P-I-N layer의 가변을 통하여 고효율을 달성하기 위한 simulation을 수행하였다. 가변 조건으로는 p-layer의 thickness, activation energy 그리고 energy bandgap을 단계별로 변화시켰고 i-layer는 thickness를 n-layer는 thickness와 activation energy를 가변하여 최적의 조건을 찾아 분석하였다. 최종 simulation 결과 p-layer의 thickness 5nm, activation energy 0.3eV 그리고 energy bandgap 1.8eV에서, i-layer thickness 400nm, n-layer thickness 30nm, activation energy 0.2eV에서 최고 효율 11.08%를 달성하였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 하계학술대회 논문집
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• pp.437-437
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• 2009

현재 상용화되어 있는 결정질 태양전지의 경우 높은 실리콘 가격으로 인해 저가화에 어려움을 격고 있다. 따라서 태양전지 저가화의 한 방법으로 박막태양전지가 주목을 받고 있다. P-I-N 구조의 박막태양전지에서 I-layer 각 층의 thickness, activation energy, energy bandgap은 고효율 달성을 위한 중요한 요소이다. 본 논문에서는 박막태양전지 P-I-N layer의 가변을 통하여 고효율을 달성하기 위한 simulation을 수행하였다. 가변 조건으로는 p-layer의 thickness, activation energy 그리고 energy bandgap을 단계별로 변화시켰고 i-layer는 thickness를 n-layer는 thickness와 activation energy를 가변하여 최적의 조건을 찾아 분석하였다. 최종 simulation 결과 p-layer의 thickness 5nm, activation energy 0.3eV 그리고 energy bandgap 1.8eV에서, i-layer thickness 400nm, n-layer thickness 30nm, activation energy 0.2eV에서 최고 효율 11.08%를 달성하였다.

• KIEE International Transactions on Electrophysics and Applications
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• 제2C권6호
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• pp.281-286
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• 2002

The temperature accelerated dielectric breakdown strength of on-wafer low-k dielectric polymer films with thicknesses ranging from 94 nm to 1141 nm is investigated by using the current-voltage characteristic measurements with MIS structures. The temperature dependence of dielectric strength is demonstrated to be Arrhenious for all thicknesses. However, the activation energy is found to be strongly thickness dependent. It follows an exponential relationship rather than being a single value, i.e., the activation energy increase significantly as film thickness increases for the thickness below 500 nm, but it is almost constant for the thickness above 500 nm. This relationship suggests that the change of the activation energy corresponding to different film thickness is closely related to the temperature dependence of the electron trapping/detrapping process in polymer thin films, and is determined by both the trapping rate and the detrapping rate. Thinner films need less energy to form a conduction path compared to thicker films. Hence, it leads to smaller activation energy in thinner films, and the activation energy increases with the increase in film thickness. However, a nearly constant value of the activation energy is achieved above a certain range of film thickness, indicating that the trapping rate and detrapping rate is almost equal and eventually the activation energy approaches the value of bulk material.

• Current Applied Physics
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• 제18권12호
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• pp.1528-1533
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• 2018

The trajectories of adsorption and dissociation process of $O_2$ on the Al (111) surface were studied by the spinpolarized ab initio molecular dynamics method, and the adsorption activation energy was clarified by the NEB method with hybrid functionals. Three typical dissociation trajectories were found through simulation of $O_2$ molecule at different initial positions. When vertically approaches to the Al surface, the $O_2$ molecule tends to rotate, and the activation energy is 0.66eV. If $O_2$ molecule does not rotate, the activation energy will increase to 1.43 eV, and it makes the O atom enter the Al sublayer eventually. When the $O_2$ molecules parallel approach to the Al surface, there is no activation energy, due to the huge energy released during the adsorption process.

• 한국환경과학회지
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• 제25권2호
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• pp.281-288
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• 2016

After analyzing of heating value of four kinds of RDF, the RDF-D has the highest heating value, was chosen to be mixed with carbonized sludge by different ratio. The 85%:15% ratio, which has the highest efficiency, was analyzed with thermogravimetric and pyrolysis kinetics. Applying of Kissinger method, activation energy was obtained from slope which is calculated from relation of ln(${\beta}/T^2{_m}$) and $1/T_m$. The kinetic parameters obtained from Kissinger method were 46.06 kJ/mol of RDF, 55.99 kJ/mol of carbonized sludge and 40.68 kJ/mol of mixture of RDF and carbonized sludge. The mixture of RDF and carbonized sludge has the lowest activation energy and frequency factor, during thermal decomposition reaction it has the slowest reaction rate and needs the lowest energy. Although activation energy with pyrolysis of RDF was irregularly scattered, it showed that activation energy was stabilized by co-pyrolysis of RDF and additives(Carbonized Sludge).