• Title/Summary/Keyword: 연소속도증가

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Flmae Visualization of the sector combustor (분할연소기의 화염 가시화 연구)

  • Kim, Bo-Ra-Mi;Choi, Chea-Hong;Kim, Chun-Taek;Choi, Seong-Man
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2009.11a
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    • pp.213-216
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    • 2009
  • In order to see the flame behavior in the gas turbine combustor, combustion test was performed by using sector combustor. Ignition test with torch ignition system was carried out at the various combustor inlet velocity and air fuel ratio. Also, flame blow out limit was measured by changing fuel flow rate with fixed air mass flow rate. In the test results, stable ignition is possible at air excess ratio of 6 and this limit is gradually increased with combustor inlet air velocity. The minimum blow out limit is about 4 at 40 m/s of combustor inlet velocity. This blow out limit is also increased up to about 10 with increasing combustor inlet velocity.

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Combustion Instability and Active Control in a Dump Combustor (덤프 연소기에서의 연소불안정과 능동제어에 대한 연구)

  • Ahn Kyu-Bok;Yu Kenneth;Yoon Young-Bin
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2005.11a
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    • pp.445-449
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    • 2005
  • The mixed acoustic-convective mode combustion instability and the possibility of combustion control using a loudspeaker to these instabilities were studied. By changing inlet velocity, combustor length and equivalence ratio, the dynamic pressure signals and the flame structures were simultaneously taken. The results showed that as the combustor length increased and the inlet velocity decreased, the instability frequency decreased and the maximum power spectral densities of the dynamic pressures generally decreased. The instability frequency could be affected by an equivalence ratio over the operating conditions. From the data of close-loop control, as the loudspeaker may work out-of-phase with the natural instability, the optimum time-delay controller was confirmed to be able to reduce the vortex shedding from the mixed acoustic-convective mode combustion instability.

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A Study of Flame Visualization of the APU Gas Turbine Engine Sector Combustor (APU용 가스터빈 엔진 분할연소기의 화염가시화 연구)

  • Kim, Bo-Ra-Mi;Choi, Chea-Hong;Choi, Seong-Man
    • Journal of the Korean Society of Propulsion Engineers
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    • v.15 no.4
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    • pp.11-17
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    • 2011
  • In order to see flame behavior in the annular reverse gas turbine combustor, sector combustion test was performed. Ignition test by using torch ignition system was carried out at various combustor inlet velocity and air fuel ratio. Also, flame blow out limit was measured by changing fuel flow rate with constant air mass flow rate. In test results, stable ignition is possible at air excess ratio of 6 and this limit is gradually increased with combustor inlet velocity. The minimum blow out limit is about 4 at 40 m/s of combustor inlet velocity. This blow out limit is also increased up to about 10 with increasing combustor inlet velocity. Test result shows that lean blow out limits are increased with air velocity. The highest blow out limit was found at the combustor inlet velocity of 65 m/s.

A Study of Flame Visualization of the APU Gas Turbine Engine Sector Combustor (APU용 가스터빈 엔진 분할연소기의 화염가시화 연구)

  • Kim, Bo-Ra-Mi;Choi, Chea-Hong;Choi, Seong-Man
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2010.11a
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    • pp.153-159
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    • 2010
  • In order to see the flame behavior in the annular reverse gas turbine combustor, sector combustion test was performed. Ignition test by using torch ignition system was carried out at the various combustor inlet velocity and air fuel ratio. Also, flame blow out limit was measured by changing fuel flow rate with constant air mass flow rate. In the test results, stable ignition is possible at air excess ratio of 6 and this limit is gradually increased with combustor inlet velocity. The minimum blow out limit is about 4 at 40 m/s of combustor inlet velocity. This blow out limit is also increased up to about 10 with increasing combustor inlet velocity. Test result shows that lean blow out limits are increased with air velocity. The highest blow out limit was found at the combustor inlet velocity of 65m/s.

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Study on the Enhancement of Burning Rate of HTPB/AP Solid Propellants (HTPB/AP계 고체 추진제의 연소속도 증진 방안 연구)

  • Lee, Sunyoung;Ryu, Taeha;Hong, Myungpyo;Lee, Hyoungjin
    • Journal of the Korean Society of Propulsion Engineers
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    • v.21 no.4
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    • pp.21-27
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    • 2017
  • In this paper, in order to control the burning rate and pressure exponent of HTPB/AP/Al based propellant for the improvement of performance, the effect of the size ratio of AP particles and various contents of Butacene as burning catalyst on combustion properties was investigated. In the propellant formulation with both $28{\mu}m$ Al of 23% and Butacene of 3%, the burning rate and pressure exponent were increased with increasing the contents of $9{\mu}m$ AP particles. And the burning rate was increased with increasing the contents of Butacene with showing the relatively low pressure exponent in the propellant containing Butacene. However, the significant variations of pressure exponent by contents of Butacene were not observed.

Combustion Characteristics of Methane-Air Pre-mixture in a Closed Vessel(II) (밀폐용기내 메탄-공기 예혼합기의 연소특성(II))

  • 김봉석;이영재;고창조;권철홍
    • Journal of Energy Engineering
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    • v.4 no.1
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    • pp.85-94
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    • 1995
  • 본 연구에서는 최근 차량용 대체연료로서 주목받고 있는 천연가스의 연소특성을 규명하기 위해 밀폐된 정적연소실을 이용, 당량비, 초기압력 및 점화위치 변화에 따른 연소실험을 행하였으며, 그 결과 다음과 같은 결론을 얻었다. 메탄-공기 예혼합기의 화염전파과정은 이론혼합기 부근에서 구면형으로 진행되는데 반해, 과농 또는 과박 혼합기 그리고 점화위치가 연소실 벽면에 가까울수록 타원형으로 진행되며, 초기압력이 증가함에 따라 화염전파는 느려진다. 화염전파속도와 연소 속도는 초기압력이 낮고 점화위치가 연소실 중심에 가까울수록 빠르며, 당량비 1.0∼1.1 사이에서 최대치를 보인다.

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A Combustion Analysis of Surface Fuel Burning Experiment According to Density Variation (밀도에 따른 지표 연료의 연소실험 분석)

  • Kim, Eung-Sik;Kim, Jang-Hwan;Kim, Dong-Hyun;Park, Hyung-Ju;Kim, Jeong-Hun
    • Fire Science and Engineering
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    • v.24 no.1
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    • pp.1-7
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    • 2010
  • This paper shows combustion characteristics of fallen leaves of Quercus variabilis and Pinus densiflora according to variation of mass densities. Combustion temperature, mass loss rate, flame height, duration of combustion and velocity of hot gas are measured and analyzed. For the experiment 10cm heighted baskets with varying diameters of 20, 30, 40 and 50cm are used for the combustion and the pilot ignition is carried on the top of the fuel. In case of Pinus densiflora mass loss rate, duration of flame, flame height and combustion time become larger as the mass density and diameter of basket increase, on the other hand Quercus variabilis shows saturation characteristics in mass loss rate and flame height. Velocity of hot gas is proportional to flame height.

A Numerical Analysis on Combustion Characteristics of the Gasoline Engine using Methanol Reformulated Fuels under WOT Condition (전부하 운전조건에서 메탄올 개질연료를 사용한 가솔린 엔진의 연소특성에 대한 수치해석)

  • Lee, Suk-Young;Jeon, Chung-Hwan
    • Journal of Energy Engineering
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    • v.20 no.2
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    • pp.163-169
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    • 2011
  • This research is to decide the possibility of using RM50(reformulated methanol fuel) without any modification of engine by the method of numerical analysis. Comparing the heat release rate, the difference among each fuel was decreased according to the increase of the engine speed, and the maximum heat release rate was higher in the order of RM50 and gasoline fuel. Also, this order corresponds to the order of burning speed. RM50 had the higher turbulent burning speed, and the curve of turbulent intensity was showed similar tendency to the curve of turbulent burning speed. RM50 had relatively high burning speed, short quenching length, high temperature in cylinder, so that it might increase NO emission, but owing to chemical reaction dynamics, it was decreased NO emission. Therefore, in order to predict the possibility of using RM50, it is needed to consider not only the temperature in cylinder by low heating value, but also combustion characteristics including burning speed.

Burning Rate Testing of Double Base Solid Propellants using Ultrasound (초음파를 이용한 Double Base형 고체추진제의 연소속도 측정)

  • Song, Sung-Jin;Ko, Sun-Feel;Kim, Hak-Joon;Oh, Hyun-Taek;Kim, In-Chul;Yoo, Ji-Chang;Jung, Jung-Yong
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2006.11a
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    • pp.247-250
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    • 2006
  • In the previous study, we have developed an ultrasonic measurement system and analysis technique for borning rate testing of solid propellants using ultrasound. And then, using the developed system, burning rate of composite propellants were measured. So, in this study, we performed measurement of double base solid propellant, which has non-linear homing rate as pressure increasing, using the developed system in order to evaluate capability of ultrasonic method. Furthermore, accuracy of measured homing rates using ultrasound was verified by comparison to homing rate measured by the strand burner method.

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Effect of Chamber Configuration on Combustion Characteristic Velocity of Full-scale Combustion Chamber (실물형 연소기의 형상에 따른 연소특성속도 비교)

  • Kim, Jong-Gyu;Han, Yeoung-Min;Ahn, Kyu-Bok;Kim, Mun-Ki;Seo, Seong-Hyeon;Choi, Hwan-Seok
    • Proceedings of the Korean Society of Propulsion Engineers Conference
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    • 2008.05a
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    • pp.149-152
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    • 2008
  • Effects of chamber configuration on combustion characteristic velocity of full-scale combustion chamber for 30-tonf-class liquid rocket engine were studied. The configurations of combustion chamber are ablative and channel cooling chamber (${\varepsilon}$=3.2) which have detachable mixing head, and single body regenerative cooling chamber which has nozzle expansion ratio of 3.5 and 12, respectively. The combustion chambers have chamber pressure of 53${\sim}$60 bar and propellant mass flow rate of 89 kg/s, and the injectors of all combustion chamber have recess number 1.0 and double-swirl characteristics. The hot firing test results at design point show that the combustion characteristic velocity of the regenerative cooling chamber which has nozzle expansion ratio of 12 is higher than that of other combustion chambers. The reasons for the above result are the increases of combustion pressure and enthalpy of kerosene which is heated due to cooling of the chamber wall before injection into the combustion field.

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