• Title/Summary/Keyword: quenching temperature

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The Effect of Temperature on the Photoluminescence Properties of the InZnP/ZnSe/ZnS (Core/Multishell) Quantum Dots (온도에 따른 InZnP/ZnSe/ZnS (핵/다중껍질) 양자점의 형광 특성 변화)

  • Son, Min Ji;Jung, Hyunsung;Lee, Younki;Koo, Eunhae;Bang, Jiwon
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.31 no.7
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    • pp.443-449
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    • 2018
  • We investigated the temperature-dependent photoluminescence spectroscopy of colloidal InZnP/ZnSe/ZnS (core/shell/shell) quantum dots with varying ZnSe and ZnS shell thickness in the 278~363 K temperature range. Temperature-dependent photoluminescence of the InZnP-based quantum dot samples reveal red-shifting of the photoluminescence peaks, thermal quenching of photoluminescence, and broadening of bandwidth with increasing temperature. The degree of band-gap shifting and line broadening as a function of temperature is affected little by shell composition and thickness. However, the thermal quenching of the photoluminescence is strongly dependent on the shell components. The irreversible photoluminescence quenching behavior is dominant for thin-shell-deposited InZnP quantum dots, whereas thick-shelled InZnP quantum dots exhibit superior thermal stability of the photoluminescence intensity.

The Latent Heat of Phase Transformation of the Carbon Steel and the Calculation of Cooling Curves Including the Latent Heat in Quenching (탄소강 담금질시의 상변태열과 이를 포함한 냉각곡선의 계산)

  • 윤석훈;김경근
    • Journal of Advanced Marine Engineering and Technology
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    • v.18 no.3
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    • pp.10-16
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    • 1994
  • This study aimed at measuring the latent heat of phase transformation of S45C carbon steel in quenching and at conducting the analytical researches into the calculation of cooling curves including the latent heat. The temperature of phase transformation of steel and its latent heat are dependant upon the cooling rates at the temperature of A1 phase transformation point. The effect of the latent heat of phase transformation is especially manifest at the cooling curve of center of specimens. The higher the cooling rates became, the lower fell the temperature region of phase transformation. In the figures of cooling rates, the phenomena of cooling rate dropping into zero was caused by the latent heat of phase transformation.

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The Effects of Heat-treating Conditions on Wear Characteristics of High Speed Steel by Powder Metallurgy (분말고속도공구강의 미끄럼 마모특성에 미치는 열처리조건의 영향)

  • Lee, H.Y.;Bae, J.S.;Kim, Y.J.
    • Journal of the Korean Society for Heat Treatment
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    • v.13 no.6
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    • pp.405-411
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    • 2000
  • The effects of added elements, such as Co or Nb, on wear properties of high speed steel by powder metaliurgy(PM-HSS) had been eluminated in auther's previous paper. In addition, it is generally known that the wear properties of materials have been influenced by heat-treating conditions as well. Therefore, a study has been done to clarify the effects of heat-treating conditions on wear properties of PM-HSS. The wear tests have been performed under the same conditions as the previous paper using heat-treated PM-HSS(5%Co-1%Nb) with different quenching and tempering temperatures. The result of this paper shows that wear resistance of PM-HSS is improved with relatively high quenching temperature. However, tempering temperature is not sensitive to the wear resistance in the range of high quenching temperature. It may be deduced by the fact that the shear strength of matrix by strengthening mechanisms due to not only the quenching aging but also dispersion-hardening is improved.

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Effect of Quenching Heat-treatment on Mechanical Properties and Microstructure of Modified C95600 Bronze (개량형 C95600 청동의 기계적 성질과 미세조직에 미치는 퀜칭 열처리의 영향)

  • Lee, Sung-Yul;Moon, Kyung-Man;Oh, Jae-Hwan;Shin, Dong-Il
    • Journal of Ocean Engineering and Technology
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    • v.25 no.6
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    • pp.97-104
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    • 2011
  • Modified C95600 bronze contains Fe component of 0.7 weight percentage besides Cu-7Al-2.5Si composition. The shape of centrifugal cast is a circular pipe with thick wall. Specimens machined from the centrifugal cast were quenched in oil after isothermal holding at a given heat treatment temperature in the range of $700{\sim}900^{\circ}C$. Mechanical properties and structural morphology are depended on the quenching heat treatment temperature regardless of isothermal holding time. Tensile strength or Brinell hardness is increased with increasing heat treatment temperature. The microstructure caused by quenching contains mixing phases of ${\alpha}+{\beta}'+FeSi+{\kappa}$ which martensite of ${\beta}'$ phase has been transformed from ${\beta}$ phase. Effect of isothermal holding temperature on mechanical properties in case of quenching heat treatment attributes to the change of volume fraction of ${\beta}'$ on the structural morphology. Mechanical characteristics of specimen, initially quenched from $850^{\circ}C$, and then tempered at $500^{\circ}C$, does not show an obvious softening indication, because disappearance of ${\beta}'$ during tempering process can be compensated by precipitation of brittle phase ${\gamma}$.

Fluorescence Quenching of Bis-msb by Carbon Tetrachloride in Different Solvents

  • Thipperudrappa, J.;Biradar, D.S.;Lagare, M.T.;Hanagodimath, S.M.;Inamdar, S.R.;Kadadevaramath, J.S.
    • Journal of Photoscience
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    • v.11 no.1
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    • pp.11-17
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    • 2004
  • Fluorescence quenching of l,4-bis [2-(2-methylphenyl) ethenyl]-benzene (Bis-MSB) by carbon tetrachloride in five different solvents namely hexane, cyclohexane, toluene, benzene and dioxane has been carried out at room temperature with a view to understand the quenching mechanisms. The Stern-Volmer plot has been found to be non-linear with a positive deviation for all the solvents studied. In order to interpret these results we have invoked the Ground state complex and Sphere of action static quenching models. Using these models various rate parameters have been determined. The magnitudes of these parameters imply that sphere of action static quenching model agrees well with the experimental results. Hence the positive deviation in the Stem-Volmer plots is attributed to the static and dynamic quenching. Further, with the use of Finite Sink approximation model, it was possible to check whether these bimolecular reactions as diffusion limited and to estimate independently distance parameter R' and mutual diffusion coefficient D. Finally an effort has been made to correlate the values of R'and D with the values of the encounter distance R and the mutual diffusion coefficient D determined using the Edwardis empirical relation and Stokes-Einstein relation.

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Effects of Heat Treatment on the Micro-structures and the Mechanical Properties of 0.002% Boron-added Low Carbon Steel (0.002% 보론첨가 저탄소강의 미세조직 및 기계적 성질에 미치는 열처리의 영향)

  • Lim, Jong-Ho;Kim, Jong-Sik;Park, Byung-Ho;Lee, Jin-Hyeon;Choi, Jeong-Mook
    • Korean Journal of Materials Research
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    • v.21 no.6
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    • pp.303-308
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    • 2011
  • The effect of heat treatment on the micro-structures and the mechanical properties of 0.002% boron added low carbon steel was investigated. The tensile strength reached the peak at about $880-890^{\circ}C$ with the rising quenching temperature and then the hardness decreased sharply, but the tensile strength hardly decreased. The tensile and yield strength decreased and the total elongation increased with a rising tempering temperature, but the tensile and yield strength sharply fell and the total elongation prominently increased from above a $400-450^{\circ}C$ tempering temperature. Tempered martensite embrittlement (TME) was observed at tempering condition of $350-400^{\circ}C$. In the condition of quenching at $890^{\circ}C$ and tempering at $350^{\circ}C$, the boron precipitates were observed as Fe-C-B and BN together. The hardness decreased in proportion to the tempering temperature untill $350^{\circ}C$ and dropped sharply above $400^{\circ}C$ regardless of the quenching temperature.

An Experimental Study on the Quenching Phenomena of Hemispherical Downward Facing Convex Surfaces with Narrow Gaps (반구형 소형 간극 내에서의 냉각과정에 관한 실험적 연구)

  • Ha, Kwang-Soon;Park, Rae-Joon;Kim, Sang-Baik;Cho, Young-Ro;Kim, Hee-Dong
    • Proceedings of the KSME Conference
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    • 2001.06d
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    • pp.447-452
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    • 2001
  • Quenching phenomena of hemispherical downward facing convex surfaces with narrow gaps have been investigated experimentally. Experiments employed test sections having 1 and 2 mm in gap thickness and 1 atm in system pressure. From interpretations of the temperature and the heat flux history, it was found that the flooding inside the gap was restricted by CCFL phenomena and quenching process was propagated from lower to upper region of the internal copper shell. The ratio of the maximum heat fluxes at 1 mm to 2mm in gap thickness was the almost same that obtained by steady state experiments. The quenching scenario of the hemispherical downward facing surface with narrow gap has been suggested.

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EFFECT OF SOLVENT POLARITY ON THE FLUORESCENCE QUENCHING OF ORGANIC LIQUID SCINTILLATORS BY ANILINE

  • Shailaja, M.K.;Hanagodimath, S.M.;Kadadevarmath, J.S.;Chikkur, G.C.
    • Journal of Photoscience
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    • v.6 no.4
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    • pp.159-163
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    • 1999
  • The fluorescence quenching of 2-phenyl-5-(4-biphenylyl)-1,3,4-oxadiazole (PBD) and 1,4-di-[2-(5-phenyloxazolyl)]-benzene (POPOP) by aniline has been carried out in different solvent mixtures of dioxane and acetonitrile at room temperature. The quenching is found to be appreciable and a positive deviation from linearity was observed in the Stern-Volmer plot in all the solvent mixtures. Various rate constants for the quenching processes have been determined using a modified Stern-Volmer equation. From the positive deviations of linear Stern-Volmer plots and the dependence of rate constants on the polarity of the solvents, it has been concluded that both static and dynamic quenching processes are responsible for the observed positive deviation in the Stern-Volmer plot.

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Quenching rate controlled Laser Annealing (QLA) for poly-Si TFT fabrication

  • Han, Gyoo-W.;Alexander, Voronov;Ryu, S.G.;Kim, H.S.;Roh, C.L.
    • 한국정보디스플레이학회:학술대회논문집
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    • 2005.07b
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    • pp.897-897
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    • 2005
  • We report QLA (Quenching-rate controlled Laser Annealing) system as new concept using pulsed DPSSL and CW lasers. This process can control temperature quenching-rate of poly-Si crystallization by additional CW laser and fabricate high quality poly-Si with faster scanning speed than conventional processes. In this paper, QLA system, the experimental results and theoretical discussion will be introduced.

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Effect of Quenching Temperature and Cooling Rate on the Mechanical Properties of Direct Quenched Micro-Alloyed Steel for Hot Forging (직접Quenching 열간 단조용 비조질강의 기계적 성질에 미치는 Quenching온도 및 냉각속도의 영향)

  • Shin, Jung-Ho;Ryu, Young-Joo;Kim, Byung-Ok;Ko, In-Yong;Lee, Oh-Yeon
    • Korean Journal of Materials Research
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    • v.22 no.10
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    • pp.513-518
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    • 2012
  • Recently, automobile parts have been required to have high strength and toughness to allow for weight lightening or improved stability. But, traditional micro-alloyed steel cannot be applied in automobile parts. In this study, we considered the influence of quenching temperature and cooling rate for specimens fabricated by vacuum induction furnace. Directly quenched micro-alloyed steel for hot forging can be controlled according to its micro structure and the heat-treatment process. Low carbon steel, as well as alloying elements for improvement of strength and toughness, was used to obtain optimized conditions. After hot forging at $1,200^{\circ}C$, the ideal mechanical properties (tensile strength ${\geq}$ 1,000 MPa, Charpy impact value ${\geq}\;100\;J/cm^2$) can be achieved by using optimized conditions (quenching temperature : 925 to $1,050^{\circ}C$, cooling rate : ${\geq}\;5^{\circ}C/sec$). The difference of impact value according to cooling rate can be influenced by the microstructure. A fine lath martensite micro structure is formed at a cooling rate of over $5^{\circ}C/sec$. On the other hand, the second phase of the M-A constituent microstructure is the cause of crack initiation under the cooling rate of $5^{\circ}C/sec$.