• Title/Summary/Keyword: temperature pulse

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Ultrasonic pulse velocity analysis for high- temperature mechanical properties of high strength concrete replacing non-sintered hwangto (비소성 황토를 치환한 고강도 콘크리트의 고온 역학적 특성 평가를 위한 초음파 속도 분석)

  • Hong, Kil-Dong;Lim, Gguk-Jeong;Jang, Kil-San
    • Proceedings of the Korean Institute of Building Construction Conference
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    • 2023.11a
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    • pp.273-274
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    • 2023
  • In this study, ultrasonic pulse velocity was analyzed to evaluate the high-temperature mechanical properties of concrete mixed with non-sintered hwangto. The W/B of the specimens was set at 0.41, the percentage of non-sintered hwangto admixture was set at two levels of 15,30%. The target temperature of the specimen is set to 6 levels of 20, 100, 200, 300, 500, 700 ℃, and the heating rate is set to 1℃/min. The result showed that the amount of non-sintered hwangto incorporated into the concrete tends to results in lower compressive strength. Ultrasonic pulse velocity showed similar trends, but differed in some areas.

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Enthalpy Flow Loss by Steady Mass Streaming in Pulse Tube Refrigerators (맥동관냉동기의 정상상태 질량흐름에 의한 엔탈피손실)

  • 백상호;정은수
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.12 no.7
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    • pp.623-631
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    • 2000
  • Effects of the taper angle and the angular velocity of a pulse tube on the enthalpy flow loss associated with the steady mass streaming were analysis by two-dimensional analysis of a pulse tube with variable cross-section. It was shown that the steady mass flux can lead to a large steady second-order temperature. The enthalpy flow loss associated with the steady mass streaming increases as the angular velocity increases. For a pulse tube where the viscous penetration depth is far thinner than the inner radius, the enthalpy flow loss can be significantly reduced by tapering the pulse tube since both the steady mass flux and the steady second-order temperature decrease as the taper angle increase.

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Second-order velocity and temperature in pulse tube refrigerators (맥동관냉동기의 2차속도와 온도)

  • Lee, H.J.;Chae, W.B.;Jeong, E.S.
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.9 no.2
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    • pp.239-248
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    • 1997
  • Steady components and unsteady components of second-order velocity and temperature within pulse tube refrigerators were obtained. Second-order solutions were obtained from the first-order solutions of continuity, momentum and energy equations, assuming that the amplitude of the piston motion is small. The axial temperature gradient was considered in the analysis. The flow direction of the streaming was consistent with previous experimental observations. Effects of axial temperature gradient on secondary flow and second-order temperature were shown.

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The Effects of Pulse Current on the Surface Appearance of Chromium Plating (크롬 전착층의 표면광택에 미치는 펄스도금의 영향)

  • 한성호;권식철;여운관
    • Journal of the Korean institute of surface engineering
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    • v.14 no.4
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    • pp.215-220
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    • 1981
  • The surface appearance of chromium electrodeposit was studied by employing a pulse curr-ent plating in self-regulating high speed (SRHS) bath containing 20 g/$\ell$, K2SiF6 7.5 g/$\ell$ SrSO4 and 250 g/$\ell$ CrO3. As the pulse frequency increased, the surface appearance changed suddenly from bright a-ppearance in a direct current plating condition to gray one in the range of pulse frequency less than about 20KHz. However the bright appearance is recovered as the pulse frequen-cy exceeded 20 KHz. This phenomena seemed to be related with the preferred orientation of electrodeposits, considering the relationship between the preferred orientation of elect-rodeposits and surface appearance in a SRHS bath. Direct current plating was also applied to both Sargent and SRHS bath and investigat-ion on surface appearance was extended to the high current density of 400 A/dm2. In a Sa-rgent bath, the increase in bath temperature was necessary for bright appearance as the current density was increased within 150 A/dm2, but bright region was shown in the cons-tant temperature of 70-75$^{\circ}C$ above the current density of 150A/dm2. On the other hand, two regions of surface brightness was found in a SRHS bath. One is region in the low temperature less than 25$^{\circ}C$ and the other in the moderate temperature range from 55$^{\circ}C$ to 65$^{\circ}C$.

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Improvement of Color Temperature using Auxiliary Address Pulse Driving Scheme in 42-in. WVGA Plasma Display Panel

  • Park, Ki-Hyung;Lee, Eun-Cheol;Cho, Ki-Duck;Tae, Heung-Sik;Chien, Sung-Il
    • Journal of Information Display
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    • v.6 no.1
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    • pp.22-27
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    • 2005
  • Auxiliary address pulse driving scheme is proposed for controlling and improving the color temperature of the 42-inch WVGA ac-plasma display panel (ac-PDP) without sacrificing total luminance. Under a white-background, the color temperature of 42-inch ac-PDP is improved by about 1,700 K, whereas under a black-background, the color temperature of 42-inch ac-PDP is improved by about 3,200 K. In addition, by properly controlling the luminance in the R, G, and B cells, the color temperature of 42-inch ac-PDP can be raised from 5,827K to 10,705K.

Study on the Correlation between the Change in SAR and Temperature of the Human Head by use Dental Implant on 3.0T Brain MRI : Using the XFDTD program (3.0T Brain MRI 검사 시 치아임플란트 시술 유무와 인체의 SAR, 체온 변화와의 상관관계에 관한 연구 : XFDTD 프로그램을 이용)

  • Choe, Dea-yeon;Kim, Dong-Hyun
    • Journal of the Korean Society of Radiology
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    • v.11 no.3
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    • pp.139-146
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    • 2017
  • At the Brain MRI examination, RF Pulse are irradiated on the human head in order to acquire MR images. At this time, a considerable part of the irradiated RF Pulse energy is absorbed in our body and the temperature of the human head will rise depending on the degree of exposure, so it will affect the human head. Even if the same RF Pulse energy is given, if the metal is inserted in the human head, the conductivity of the human head is greatly increased by the metal, so the SAR value increases and the temperature also rises. Therefore, we started this research with the question as to whether there is difference between the change in SAR value and temperature displayed on the head of the human according to use or not of the dental implant. Experiments were using the XFDTD program on a 128 MHz RF Pulse frequency by a 3.0 tesla MRI. We can see that both are increasing that the average value of SAR and temperature that absorbed by the human head model used the dental implant. In addition, the average maximum SAR value and the maximum temperature rise in the brain part are shown below the international safety standard value but the influence can not be ignored because of the result may change according to the increase in the number of dental implant. And as future tasks. we need to the simulation of temperature rise and SAR due to an increase in the number of implants and volumes of teeth, dental implant material.

Influence of extreme curing conditions on compressive strength and pulse velocity of lightweight pumice concrete

  • Anwar Hossain, Khandaker M.
    • Computers and Concrete
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    • v.6 no.6
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    • pp.437-450
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    • 2009
  • The effect of six different curing conditions on compressive strength and ultrasonic pulse velocity (UPV) of volcanic pumice concrete (VPC) and normal concrete (NC) has been studied. The curing conditions include water, air, low temperature ($4^{\circ}C$) and different elevated temperatures of up to $110^{\circ}C$. The curing age varies from 3 days to 91 days. The development in the pulse velocity and the compressive strength is found to be higher in full water curing than the other curing conditions. The reduction of pulse velocity and compressive strength is more in high temperature curing conditions and also more in VPC compared to NC. Curing conditions affect the relationship between pulse velocity and compressive strength of both VPC and NC.

Plasma Assisted Nitriding of Stainless Steel Type 304L (304L 스테인리스 강의 플라즈마 질화처리)

  • Park, J.R.
    • Journal of the Korean Society for Heat Treatment
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    • v.8 no.4
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    • pp.255-265
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    • 1995
  • Stainless steel type 304L has been nitrided in the low pressure (600Pa) and high nitrogen (80% $N_2$+20% $H_2$) environment for 5 hours by the square-wave-pulsed-d.c. plasma as a function of temperature $400{\sim}550^{\circ}C$ and pulsation. At the lower temperature range of $400{\sim}500^{\circ}C$ and at the relatively high ratio of pulse duration to pulse period. "S-phase" has been developed in the form of thin nitrided surface layer which has many cracks, leading to be nearly impossible for the industrial anti-wear and anti-corrosion applications. At the higher temperature up to $550^{\circ}C$ with the increasing ratio of the pulse duration to pulse period up to $50{\mu}s/100{\mu}s$, the nitrided layer, whose growth rate has increased also, has been composed mainly of CrN and $Fe_4N$ phases and has become thick, uniform and nearly crack-free.

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Plasma Characteristics and Substrate Temperature Change in Al:ZnO Pulse Sputter Deposition: Effects of Frequency (Al:ZnO의 펄스 스퍼터 증착에서 주파수에 따른 플라즈마의 특성과 기판 온도 변화)

  • Yang, Won-Kyun;Joo, Jung-Hoon
    • Journal of the Korean institute of surface engineering
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    • v.40 no.5
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    • pp.209-213
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    • 2007
  • Change of the plasma volume by pulse frequency in a bipolar pulsed DC unbalanced magnetron sputtering was investigated. As increasing the frequency at off duty 10% and at a constant power, the plasma volume was lengthened in vertical direction from the AZO target. When there is an electrically floated substrate, the vertical length of the plasma area was not affected by the pulse frequency. Instead, the diameter of the plasma volume was increased. We found that the temperature rise of a substrate was affected by the pulse frequency, too. As increasing it, the maximum temperature rise of a glass substrate was decreased from $132^{\circ}C\;to\;108^{\circ}C$.

Measurement of properties of laser-produced plasmas (레이저플라즈마의 제특성의 계측)

  • 강형부
    • 전기의세계
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    • v.29 no.2
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    • pp.118-128
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    • 1980
  • The properties of plasmas produced by high power glass laser were investigated with various methods of diagnostics. Electron temperature was estimated by measurement of soft X-ray, and ion temperature was estimated by measurement of the time-of-flight of ion. The measurement of incident and reflected laser light, and Schlieren and shadowgragh methods were also used. No influence of laser pulse duration on the temperature was observed in the case of durations 2, 4 and 10 nsecs. The effective heating of plasma occurred in about 2 nsec of beginning of incident laser pulse. The experimental results for fast rising laser pulse were discussed and the influence of resetime of laser pulse on the heating of plasma was described. Neutrons produced by irradiating laser beam to solid deuterium target were detected.

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