摘要(英) |
This thesis quantitatively measures laminar and turbulent burning velocities (SL and ST) of the premixed PRF95 (primary reference fuel with 95% volume of iso-octane and 5% volume of n-heptane) at high temperature and high pressure conditions. There are two objectives in this thesis: (1) To measure values of SL and ST of spherical premixed flames of PRF95 and investigate the pressure effect on SL and ST by keeping the r.m.s. turbulent fluctuation velocity (u′) constant. (2) To investigate the effect of pressure and turbulent flow Reynolds number (ReT,flow = u′LI/) on ST under constant ReT,flow condition, where LI and are the integral length scale of turbulence and the kinematic viscosity of reactants respectively. Experiments are conducted in a large dual-chamber, high-pressure, high-temperature, fan-stirred cruciform premixed turbulent explosion facility capable of generating isotropic turbulence for ST measurements of expanding spherical PRF95/air flames. While controlling the product of u′LI in proportion to the decreasing at elevated pressure to obtain the constant ReT,flow value, and we measure SL and ST of PRF95 at the equivalence ratio ( = 1.0, Le ≈ 1.44), T = 358K, and 373K, p = 1-5 atm, u′= 1.0-5.4 m/s, and at three constant ReT,flow = 6,700; 9,100; 11,600 in order to further investigate the ReT,flow effect on ST. Under high pressure condition, SL decreases with increasing pressure, where cellular structures all over the flame surface can be observed. For laminar flames, SL decreases with increasing pressure because SL is effected by a pressure chain reaction mechanism during flame propagating. Take H-O2 reaction for example, key reaction (H1): H + O2 → OH + O is a two-body branching reaction, while reaction (H9): H + O2 + M → HO2 + M is a three-body inhibiting reaction. While by increasing pressure, (H9) is enhanced relative to (H1) because three-body reactions are favored over two-body reactions as pressure increases. Therefore, in the overall reaction at high pressure conditions, the inhibition reaction is enhanced to cause a decrease in SL. For turbulence flames, when under constant u′ condition, ST increases with increasing pressure. In the past, this is because the flame thickness decreases with increasing pressure, making the flame surface interfered with Hydrodynamic Instability (i.e., Darrieus-Landau Instability). Flame surface results in the cellular structures which causes an increase in the area of the turbulent flame and increases the ST. However, previous studies have not considered the fact that pressure increases with the ReT,flow increasing.
Results show that when under the condition of constant u′, the values of ST increase with increasing p, which is mainly due to increase of ReT,flow with increasing p. On the contrary, when under the condition of constant ReT,flow, we find that the values of ST actually decrease with increasing p. Both ST and SL have an exponential decrease in pressure effect which indicates that the ReT,flow may be a key factor affecting the increase of ST.
This thesis also includes previous iso-octane ST at T=358K, 373K, and 423K obtained from data our laboratory using the same methodology, so that the normalization of these data by using five general correlations can be made for comparison as describe below (1) ST,c=0.5/u′ = A(Da)B, where the subscript c is the mean progress variable, Damköhler number Da = (LI/u′)(SL/L), L is laminar flame thickness. (2) ST,c=0.5/SL = A(ReT,flame)0.5, where the turbulent flame Reynolds number ReT,flame= (u′/SL)(<R>/L). (3)ST,c=0.5/SL = A[(u′/SL)(p/p0)]B, where p0 is the atmospheric pressure. (4)ST/u′=AK-0.3, where Karlovitz number K = 0.157(u′/SL)2(ReT,flow)-0.5. (5)ST,c=0.5/SL= A(ReT,flame/Le2)B and A and B are experimental constants of different general correlations. As a result, it is found that the previously dispersed normalized ST/SL data can be converged into a single curve after being substituted into a function that considers the Le number as a correction. The five modified general correlations all show good fitting goodness. Among them, the general correlation (3) has better fitting goodness (R2 = 0.90). The results show that the flame propagation still has self-propagation similarity even though for different fuel and equivalence ratios. The results of this thesis are useful for high temperature and high pressure premixed turbulent combustion applications, such as combustion studies for vehicles engines. |
參考文獻 |
參考文獻
[1]https://www.taipower.com.tw/tc/page.aspx?mid=202&cid=129&cchk=675cea43-9c45-4ae1-80c6-4f18b3b38d8e.
[2] https://www.youtube.com/watch?v=cWHq-Qr903g.
[3] O. Mannaa, M.S. Mansour, W.L. Roberts, S.H. Chung, “Laminar burning velocities at elevated pressures for gasoline and gasoline surrogates associated with RON”, Combustion and Flame, Vol. 162, pp. 2311-2321, 2015.
[4] R. Yang, D. Hariharan, S. Zilg, B. Lawler, S. Mamalis, “Efficiency and Emissions Characteristics of an HCCI Engine Fueled by Primary Reference Fuels”, SAE Technical Paper 2018-01-1255, 2018.
[5] V. S. B. Shankar, M. Sajid, K. Al-Qurashi, N. Atef, I. Alkhesho, A. Ahmed, S. Chung, W. Roberts, " Primary Reference Fuels (PRFs) as Surrogates for Low Sensitivity Gasoline Fuels ", SAE Technical Paper 2016-01-0748, 2016.
[6] M. Chaos, A. Kazakov, Z. Zhao, F. L. Dryer, “A high-temperature chemical kinetic model for primary reference fuels”, International Journal of Chemical Kinetics, Vol. 39, pp. 399-414, 2007.
[7] Y. Huang, C.J. Sung, J.A. Eng, “Laminar flame speeds of primary reference fuels and reformer gas mixtures”, Combustion and Flame, Vol. 139, pp. 239-251, 2004.
[8] Y.H. Liao, W.L. Roberts, “Laminar Flame Speeds of Gasoline Surrogates Measured with the Flat Flame Method”, Energy Fuels, Vol. 30, pp. 1317-1324, 2016.
[9] H. Wei, D. Gao, L. Zhou, S. Petrakides, R. Chen, D. Feng, J. Pan, “Experimental study on laminar flame characteristics of methane-PRF95 dual fuel under lean burn conditions”, Fuel, Vol. 185, pp. 254-262, 2016.
[10] S. Jerzembeck, N. Peters, P. Pepiot-Desjardins, H. Pitsch, “Laminar burning velocities at high pressure for primary reference fuels and gasoline: Experimental and numerical investigation”, Combustion and Flame, Vol. 156, pp. 292-301, 2009.
[11] Z. Zhao, J. P. Conley, A. Kazakov, F. L. Dryer, "Burning velocities of real gasoline fuel at 353 K and 500 K", SAE Technical Paper 2003-01-3265, 2003.
[12] M. Lawes, M. P. Ormsby, C. G. W. Sheppard, R. Woolley, “The turbulent burning velocity of iso-octane/air mixtures”, Combustion and Flame, Vol. 159, pp. 1949-1959, 2012.
[13] 于德維,“高溫高壓預混異辛烷火焰之層流與紊流燃燒速度量測與正規化分析”,國立中央大學機械工程研究所,碩士論文,2017年。
[14] O. Mannaa, P. Brequigny, C. Mounaim-Rousselle, F. Foucher, S. H. Chung, W. L. Roberts, “Turbulent burning characteristics of FACE-C gasoline and TPRF blend associated with the same RON at elevated pressures”, Experimental Thermal and Fluid Science, Vol. 95, pp. 104-114, 2018.
[15] D. Bradley, J. Hynes, M. Lawes, C. G. W. Sheppard, “Limitations to turbulence-enhanced burning rates in lean burn engines”, International Conference on Combustion in Engines. Institution of Mechanical Engineers, London, pp. 17, 1988.
[16] D. Bradley, Z. Chen, J. R. Swithenbank, “Burning rates in turbulent fine Dust-Air explosions”, Twenty-Second Symposium (International) on Combustion, The Combustion Institute, 1988.
[17] R. G. Abdel-Gayed, K. J. Al-Khishali, D. Bradley, “Turbulent burning velocities and flame straining in explosions”, Proc. R. Soc. Lond. A, Vol. 391, pp. 393-414, 1984.
[18] H. Kobayashi, Y. Kawabata, K. Maruta, “Experimental study on general correlation of turbulent burning velocity at high pressure”, Twenty-Seventh Symposium (International) on Combustion, The Combustion Institute, Vol. 27, pp. 941-948, 1998.
[19] S. Chaudhuri, V. Akkerman, C. K. Law, “Spectral formulation of turbulent flame speed with consideration of hydrodynamic instability”, Physical Review Letters, Vol. 84, 2011.
[20] S. S. Shy, C. C. Liu, W. T. Shih, “Ignition transition in turbulent premixed combustion”, Combustion and Flame, Vol. 157, pp. 341-350, 2010.
[21] S. S. Shy, W. J. Lin, J. C. Wei, “An experimental correlation of turbulent burning velocities for premixed turbulent methane-air combustion”, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences, Vol. 456, pp. 1997-2019, 2000.
[22] T. S. Yang, S. S. Shy, “Two-way interaction between solid particles and homogeneous air turbulence: particle settling rate and turbulence modification measurements”, Journal of Fluid Mechanics, Vol. 526, pp. 171-216, 2005.
[23] C. C. Liu, S. S. Shy, H. C. Chen, M. W. Peng, “On interaction of centrally-ignited, outwardly-propagating premixed flames with fully-developed isotropic turbulence at elevated pressure”, Proceedings of the Combustion Institute, Vol. 33, pp. 1293-1299, 2011.
[24] L. J. Jiang, S. S. Shy, W. Y. Li, H. M. Huang, M. T. Nguyen, “High-temperature, high-pressure burning velocities of expanding turbulent premixed flames and their comparison with Bunsen-type flames”, Combustion and Flame, Vol. 172, pp. 173-182, 2016.
[25] C. K. Law, C. J. Sung, H. Wang, T. F. Lu, “Development of Comprehensive Detailed and Reduced Reaction Mechanisms for Combustion Modeling” AIAA J., Vol. 41, pp. 1629-1646, 2003.
[26] S. Dooley, S. H. Won, M. Chaos, J. Heyne, Y. Ju, F. L. Dryer, K. Kumar, C. J. Sung, H. Wang, M. A. Oehlschlaeger, R. J. Santoro, T. A. Litzinger, “A jet fuel surrogate formulated by real fuel properties”, Combustion and Flame, Vol. 157, pp. 2333-2339, 2010.
[27] Z. Chen, M. P. Burke, Y. Ju, “Effects of Lewis number and ignition energy on the determination of laminar flame speed using propagating spherical flames”, Proceedings of the Combustion Institute, Vol. 32, pp. 1253-1260, 2009.
[28] Z. Chen, “On the accuracy of laminar flame speeds measured from outwardly propagating spherical flames: Methane/air at normal temperature and pressure”, Combustion and Flame, Vol. 162, pp. 2442-2453, 2015.
[29] M. T. Nguyen, D. W. Yu, S. S. Shy, “General Correlations of High Pressure Turbulent Burning Velocities with the Consideration of Lewis Number Effect”, Proceedings of the Combustion Institute, Vol.37, pp. 2391-2398, 2019.
[30] G. H. Markstein, Nonsteady Flame Propagation, Pergamon, 1964.
[31] D. Bradley, P. H. Gaskell, X. J. Gu, “Burning Velocities, Markstein Lengths, and Flame Quenching for Spherical Methane-Air Flames: A Computational Study”, Combustion and Flame, Vol. 104, pp. 176-198, 1996.
[32] S. Chaudhuri, F. Wu, D. Zhu, C. K. Law, “Flame speed and self-similar propagation of expanding turbulent premixed flames”, Physical Review Letters, Vol. 108, 2012.
[33] D. Bradley, M. Lawes, M. S. Mansour, “Correlation of turbulent burning velocities of ethanol–air, measured in a fan-stirred bomb up to 1.2 MPa”, Combustion and Flame, Vol. 158, pp. 123-138, 2011.
[34] H. Kobayashi, “Experimental study of high-pressure turbulent premixed flames”, Experimental Thermal and Fluid Science, Vol 26, pp. 375-387, 2002.
[35] M. T. Nguyen, D. W. Yu, C. Y. Chen, S. S. Shy, “General Correlations of Iso-octane Turbulent Burning Velocities Relevant to Spark Ignition Engines”, Energies, Vol.12, pp. 1848-1860, 2019. |