• Title/Summary/Keyword: 화염 길이 스케일링

Search Result 3, Processing Time 0.015 seconds

Flame Length Scaling in a Non-premixed Turbulent Diluted Hydrogen Jet with Coaxial Air (희석된 동축공기 수소 난류확산화염의 화염 길이 스케일링)

  • Hwang, Jeong-Jae;Oh, Jeong-Seog;Yoon, Young-Bin
    • Proceedings of the Korean Society of Propulsion Engineers Conference
    • /
    • 2009.11a
    • /
    • pp.242-245
    • /
    • 2009
  • The effect of fuel composition on flame length was studied in a non-premixed turbulent diluted hydrogen jet with coaxial air. The observed flame length was expressed as a function of the ratio of coaxial air to fuel jet velocity and compared with a theoretical prediction based on the velocity ratio. Four cases of fuel mixed by volume were determined. In the present study, we derived a scaling correlation for predicting the flame length in a simple jet with coaxial air using the effective jet diameter in the near-field concept. The experimental results showed that visible flame length had a good relation with the theoretical prediction. The scaling analysis is also valid for diluted hydrogen jet flames with varied fuel composition.

  • PDF

Flame Length Scaling and Structure in Turbulent Hydrogen Non-Premixed Jet Flames with Coaxial Air (동축공기 수소 확산화염의 구조 및 화염길이 스케일링)

  • Yun, Sang-Wook;Oh, Jeong-Seog;Kim, Mun-Ki;Yoon, Young-Bin
    • 한국연소학회:학술대회논문집
    • /
    • 2006.04a
    • /
    • pp.105-110
    • /
    • 2006
  • Many previous works have been performed to provide correlations of flame length, theoretically and experimentally. Most of these results studied were conducted in vertical turbulent flame with no coaxial air condition. The present study analyzes the flame length scaling with coaxial air. In turbulent hydrogen non-premixed jet flames with coaxial air, flame length scaling theoretically proposed so far has been related with the concept of a far-field equivalent source. At high coaxial air to fuel velocity ratio, $U_A/U_F$, however, this scaling theory has some difference with experimental flame length data. This difference is understood to be due to the fact that the theory is based on far-field notion, while the effect of coaxial air on jet flame occurs in the region near the nozzle exit. Therefore, we define effective jet density $P_{eff}$ involving the concept of near-field so that effective jet diameter can be extended to the near-field region. In this condition, we modify the correlation and compare with experimental data.

  • PDF

Flame Length and EINOx Scaling of Syngas $H_2$/CO Turbulent Non-premixed Jet Flames ($H_2$/CO 합성가스의 비예혼합 난류 제트화염에서 화염 길이와 EINOx 스케일링)

  • Hwang, Jeongjae;Sohn, Kitae;Bouvet, Nicolas;Yoon, Youngbin
    • Journal of the Korean Society of Combustion
    • /
    • v.17 no.4
    • /
    • pp.30-37
    • /
    • 2012
  • The flame lengths and NOx emission characteristics of syngas $H_2$/CO turbulent non-premixed jet flames were investigated. The flame length which is the main parameter governs NOx emission was studied for various syngas compositions. The flame length was compared with previous correlation between Froude number and flame height and it shows that they have good agreements. It was confirmed that the turbulent jet flames herein investigated are in the region of buoyancy-momentum transition. NOx emission was reduced with increased Reynolds number and CO contents in syngas fuel and with decreased fuel nozzle diameter which is attributed by decreased flame residence time. Previous EINOx scaling based on flame residence time of $L_f^3/(d_f^2U_f)$ satisfies only the jet flame in momentum-dominated region, not buoyancy-momentum transition region. The simplified flame residence time ($L_f/U_f$) was adopted in modified EINOx scaling. The modified scaling satisfies the jet flames not only in momentum-dominated region but in buoyancy-momentum transition region. The scaling is also satisfied with $H_2$/CO syngas jet flames.