• Title/Summary/Keyword: High Speed Schlieren Photography

Search Result 14, Processing Time 0.018 seconds

A Schlieren-photographic Visualization of the Methane/Air Premixed Flame Propagating inside a Rectangular Tube Locally-perturbed by an Ultrasonic Standing Wave (국소적 정상초음파장에 의해 교란되어 사각튜브형 연소실 내에서 전파하는 메탄/공기 예혼합화염의 슐리렌기법에 의한 가시화)

  • Kim, Min Sung;Kim, Jeong Soo;Hwang, Yeong Yeun
    • Journal of the Korean Society of Propulsion Engineers
    • /
    • v.18 no.4
    • /
    • pp.43-49
    • /
    • 2014
  • This experimental study has been conducted to scrutinize the effects of an ultrasonic standing wave (USW) on the propagating velocity and structure of methane/air premixed flame. Propagating flame was caught by high-speed Schlieren photography, and the variation of flame-behavior was analyzed in detail. It is revealed that horizontal splitting in burnt zone is resulted by the USW, and the flame propagation velocity is augmented due to the strengthened chemical reaction. Evolutionary feature of the flame perturbed by USW, maintaining a pseudo-symmetry of top and bottom flame-front about the propagation axis tends to be free from buoyancy effect.

Effects of Ultrasonic Standing Wave on the Ultrasonically-atomized Aerosol Flame Injected through a Slit-jet Nozzle (Slit-jet 노즐을 통과한 초음파 무화 에어로졸 화염에 정상초음파가 미치는 영향)

  • Ahn, Hyun Jong;Kang, Yun Hyeong;Kim, Jeong Soo
    • Journal of the Korean Society of Propulsion Engineers
    • /
    • v.24 no.6
    • /
    • pp.53-60
    • /
    • 2020
  • In liquid-fuel spray combustion, an experimental study was conducted to observe the effect of ultrasonic excitation on the ultrasonically-atomized liquid fuel flame by controlling pressure field through an ultrasonic standing wave. Flame of the ultrasonically-atomized kerosene aerosol was visualized by using a high speed camera, DSLR, and Schlieren photography. The amount of fuel consumed was obtained by a precise flow-rate measurement technique during combustion, through which the ratio of carrier gas (air) to fuel mass was able to be obtained, too. As a result, it could be found that the combustion reaction-rate of the liquid-fuel aerosol was increased by applying an ultrasonic standing wave to the secondary flame zone of the flame.

Behavioral Change of the Ultrasonic Standing Wave-affected Flame in the Reaction Zone of the Ultrasonically-atomized Kerosene Injected through a Slit-jet Nozzle (Slit-jet 노즐을 통해 분사되는 초음파 무화 케로신 화염의 정상초음파 가진에 의한 거동 변이)

  • Bae, Chang Han;Kang, Yun Hyeong;Ahn, Hyun Jong;Kim, Jeong Soo
    • Journal of the Korean Society of Propulsion Engineers
    • /
    • v.26 no.1
    • /
    • pp.60-67
    • /
    • 2022
  • A study was conducted to analyze the behavioral change of the kerosene flame ultrasonically-atomized under an ultrasonic standing-wave. Combustion region was visualized through DSLR, ICCD camera and the Schlieren photography with high-speed camera. The fuel consumption was measured by a precise scale. As a result, in the case of ultrasonic standing-wave excitation, it was observed that the intensity of OH radical(OH*) was enhanced and optimal combustion condition was formed around the upper edge of the standing-wave field.

Spray Characteristics of Swirl-coaxial Injector According to the Recess Length and Injection Pressure Variation (리세스 길이 및 분사압력 변이에 따른 스월 동축형 인젝터의 분무특성)

  • Bae, Seong Hun;Kwon, Oh Chae;Kim, Jeong Soo
    • Journal of the Korean Society of Propulsion Engineers
    • /
    • v.20 no.4
    • /
    • pp.68-76
    • /
    • 2016
  • This research is carried out for the performance evaluation of the injector that is one of the critical components of bipropellant-rocket-engine. Spray characteristics are investigated in detail according to the recess length and injection pressure on the swirl-coaxial-injector using gaseous methane and liquid oxygen as propellants. A visualization is conducted by the Schlieren photography that is composed of a light source, concave mirrors, knife, and high-speed-camera. A hollow-cone-shape is identified in the liquid spray that is spread only by inner injector and the spray angle is decreased due to the diminution of swirl strength in accordance with the increase of the length of injector orifice. When the injector sprays the liquid through the inner injector with the aid of gas through the outer injector, the spray angle in external mixing region tends to increase with rise of the recess length, while in internal mixing region, it is decreased. It is also confirmed that the same tendency of the spray angle with recess length appears irrespective of the injection pressure of liquid spray.