M.M. Alexeev, I.V. Smirnova Surgut state university 628412, Surgut, Russia CONDITIONS OF SPIN FLAME FRONT FORMATION PROPAGATING IN A NARROW SLOT.

Slides:



Advertisements
Similar presentations
Heat Transfer/Heat Exchanger
Advertisements

Indian Institute of Technology Bombay Why you should study a course on “Combustion” Introduction of the Combustion.
Wrinkled flame propagation in narrow channels: What Darrieus & Landau didn’t tell you M. Abid, J. A. Sharif, P. D. Ronney Dept.
MAE 5310: COMBUSTION FUNDAMENTALS
Laminar Flame Theory By Eng. Mohamad Okour UINVERSITY OF JORDAN MECHANICAL ENGINEERING DEPARTEMENT.
Laminar Premixed Flames and Diffusion Flames
Flame Stabilization.  In order to accomplish commercial combustion, the supply velocity of the reactant mixture is desired to be extremely high; it is.
Toshio Mogi, Woo-Kyung Kim, Ritsu Dobashi The University of Tokyo
DIFFUSION MODELS OF A FLUIDIZED BED REACTOR Chr. Bojadjiev Bulgarian Academy of Sciences, Institute of Chemical Engineering, “Acad. G.Bontchev” str.,
Boundary Layer Flow Describes the transport phenomena near the surface for the case of fluid flowing past a solid object.
On-Set of EHD Turbulence for Cylinder in Cross Flow Under Corona Discharges J.S. Chang, D. Brocilo, K. Urashima Dept. of Engineering Physics, McMaster.
Laminar Premixed Flames A flame represents an interface separating the unburned gas from the combustion products. A flame can propagate as in an engine.
Performance of Ignition Process P M V Subbarao Professor Mechanical Engineering Department Effectiveness of Ignition for Efficient Combustion …..
INTERNAL COMBUSTION ENGINES LECTURER PROF.Dr. DEMIR BAYKA.
Chapter 2: Overall Heat Transfer Coefficient
Jed Goodell Jesse Williams. Introduction Problem How much heat does a particular heat sink dissipate How many fins are needed to dissipate a specific.
Dr. Laila Guessous Suresh Putta, M.S. Student Numerical Investigations of Pulsatile Flows To develop a better understanding of the characteristics of pulsating.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Why Laminar Flow in Narrow Channels (Heat Transfer Analysis)
CHE/ME 109 Heat Transfer in Electronics
Knut Vaagsaether, Vegeir Knudsen and Dag Bjerketvedt
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
CHE/ME 109 Heat Transfer in Electronics
Chilton and Colburn J-factor analogy
Lecture #17 Boundary Layer Measurements  Boundary layer Thickness  * Displacement Thickness  Momentum Thickness.
Centre for Fire and Explosion Studies Numerical Study of Spontaneous Ignition of Pressurized Hydrogen Release through a length of tube with local contraction.
Improving Engine Performance and Efficiency by Minimisation of Knock Probability Project nº ENK6-CT Edgar C. Fernandes Ilídio Guerreiro Nuno.
1 CHAPTER 5 POROUS MEDIA Examples of Conduction in Porous Media component electronic micro channels coolant (d) coolant porous material (e) Fig.
Design & Thermo Chemistry of Turbo Combustor P M V Subbarao Professor Mechanical Engineering Department Design for performance, safety and Reliability…..
Molecular Transport Equations. Outline 1.Molecular Transport Equations 2.Viscosity of Fluids 3.Fluid Flow.
Principles of Fire Behavior
Pressure drop prediction models o Garimella et al. (2005) o Considered parameters o Single-phase pressure gradients o Martinelli parameter o Surface tension.
Faculty of Engineering, Kingston University London
Bryan S. Wang 3S103 Chew Hanson 3S109 Lim Han Xin 3S119.
ICHS, September 2007 On The Use Of Spray Systems: An Example Of R&D Work In Hydrogen Safety For Nuclear Applications C. Joseph-Auguste 1, H. Cheikhravat.
Outline Background Explosion Phenomena Experiments Correlation Conclusion/Summary Questions.
University of Illinois at Urbana-Champaign Computational Fluid Dynamics Lab Bin Zhao 1 LES Simulation of Transient Fluid Flow and Heat Transfer in Continuous.
Lesson 13 CONVECTION HEAT TRANSFER Given the formula for heat transfer and the operating conditions of the system, CALCULATE the rate of heat transfer.
Funded by FCH JU (Grant agreement No ) 1 © HyFacts Project 2012/13 CONFIDENTIAL – NOT FOR PUBLIC USE 1.
Chapter 7 External Convection
Kakutkina N.A., Korzhavin A.A., Rychkov A.D. Ignition of the waves of filtration gas combustion with open flame Institute of chemical kinetics and combustion.
External Flow: Mass Transfer Chapter 7 Sections , 7.7, 7.8.
AE 412 THERMODYNAMIC CYCLE SIMULATION II Prof.Dr. Demir Bayka.
Analogies among Mass, Heat, and Momentum Transfer
이 동 현 상 (Transport phenomena) 2009 년 숭실대학교 환경화학공학과.
Multimedia files Nos. 9.1 – 9.10 Chapter 9. Combustion features of the propane round and plane jet at the low Reynolds number The results of researches.
Combustion Calculations Calculate the theoretical flame temperature of combustion of hydrogen with theoretical amount of air assuming (a)No dissociation.
Application of Plasma Assisted Vertical Jet Flame to the Ignition of Horizontal Methane-Air Mixture 吴文伟 等离子体所
The Chemistry of Fuel Combustion in SI Engines P M V Subbarao Professor Mechanical Engineering Department Exploit the Chemical Characteristics of Combustion?!?!
External Flow: The Flat Plate in Parallel Flow Chapter 7 Section 7.1 through 7.3.
CONVECTION : An Activity at Solid Boundary P M V Subbarao Associate Professor Mechanical Engineering Department IIT Delhi Identify and Compute Gradients.
Dynamics of Front Propagation in Narrow Channels Mohammed Abid, Jamal A. Sharif, Paul D. Ronney Department of Aerospace & Mechanical Engineering University.
Design of Ignition System for SI Engines P M V Subbarao Professor Mechanical Engineering Department A Successful Ignition leads to Efficient Combustion…
University of Wisconsin -- Engine Research Center slide 1 Counter-flow diffusion flame ME Project Chi-wei Tsang Longxiang Liu Krishna P.
CHAPTER 6 Introduction to convection
Date of download: 10/10/2017 Copyright © ASME. All rights reserved.
Evolution of Spark into Flame Kernel
ME 475/675 Introduction to Combustion
Study of Hydrogen/Syngas Combustion and NO Emissions
Intro to Chromatography CHM 480 Suroviec
Fundamentals of Convection
Convection.
Heat Transfer Coefficient
Step change in the boundary condition of conduction problems
Heat Transfer from Extended Surfaces (Fins)
Solving Equations 3x+7 –7 13 –7 =.
COMBUSTION TA : Bonchan Gu PROF. SEUNG WOOK BAEK
COMBUSTION TA : Donggi Lee PROF. SEUNG WOOK BAEK
Chemical Engineering Department
The Scale Relevant to Life
Presentation transcript:

M.M. Alexeev, I.V. Smirnova Surgut state university , Surgut, Russia CONDITIONS OF SPIN FLAME FRONT FORMATION PROPAGATING IN A NARROW SLOT

The purpose of this work The experimental study of the formation regularities of and propagation of the spin flame front in propane-air mixture in the narrow slot.

The experimental setup

Development of disturbances on the surface of the cylindrical flame front

Rupture of the flame front in the initial period after the ignition mixture

Formation of two separate spin nuclei

D - diffusion coefficient of lacking component a - thermal conductance coefficient of the propane-air mixture u f - visible front propagation velocity l - distance between plates of slot Existence range of gas spin flame front in the coordinates of Lewis and Peclet numbers:

Behavior of laminar flame in a narrow boundless slot I – region of laminar flame instability to small-scale perturbations II – region of the spin centers (spin nuclei) formation. III – region of formation of «tails» from the spin nuclei. IV – region of oscillatory instability and turbulence in flame.

The resulting patterns of fluid flow and heat and mass transfer in the spin flame front can identify a range of problems to solve urgent problems of increasing the efficiency of internal combustion engines.