Title: Spray dynamics as a multirate process
1Spray dynamics as a multi-rate process
- Sergei SAZHIN, Sergey MARTYNOV,
- Felix KAPLANSKI, Steven BEGG
- Sir Harry Ricardo Laboratories, Internal
Combustion Engines Group, School of Environment
and Technology, Faculty of Science and
Engineering, University of Brighton, Brighton,
BN2 4GJ, UK - Department of Mechanical Engineering,
University College London, Torrington Place,
London, WC1E 7JE, UK -
- Laboratory of Multiphase Physics, Tallinn
University of Technology, Tallinn 19086, Estonia
2 Presentation overview
- INTRODUCTION
- SPRAY BREAK-UP MODELS
- VORTEX RING MODELS
- OTHER RECENT RESULTS
-
3 INTRODUCTION Processes in Direct Injection
Internal Combustion Engines (Diesel and Gasoline)
- Formation of a liquid fuel spray
- Fuel spray penetration
- Droplet break-up
- Vortex ring formation (gasoline engines)
- Heating of fuel droplets
- Evaporation of fuel droplets
- Ignition of fuel vapour / air mixture
4Ignition (experiment)
160 MPa injection into 10 MPa gas
140 MPa injection into 10 MPa gas
100 MPa injection into 10 MPa gas
5A typical spray in Diesel engines
6Typical vortex ring-like structure in a gasoline
fuel spray
7Typical Scales (lengths)
- Spray Length 0.03-0.1 m
- Diameter of the Nozzle 10-4 m
- Droplet Diameter 10-5 m
8Typical Scales (times)
- Spray Penetration 3 10-3 s
- Injection Duration 10-3 s
- Droplet Break-up Time 10-5 s
9SPRAY BREAK-UP MODELS
- WAVE model
- TAB (Taylor Analogy Breakup) model
- Stochastic model
,
10WAVE model
where
and
11TAB (Taylor Analogy Breakup) model
where
and
12Stochastic model
where
The break-up of parent particles into secondary
particles does not depend on the instantaneous
sizes of the parent particles (Kolmogorov, 1941).
and
is the normalised droplet distribution function
by radii
is the frequency of production of new droplets
is the break-up operator
13Stochastic model
where
is the probable number of new droplets in the
interval
and
?0 is the number of break-ups per unit time
14Stochastic model
where
The previous equation cannot be solved but we
can use the expansion
and
the third and higher logarithmic moments are set
to be zero for large times
is the number distribution function
15Stochastic model
where
and
16Comparison of the results
where
and
Gas pressure is 2 MPa, injection pressure is 60
MPa, B1v31.73
17Modified WAVE model
where
and
18Comparison of the results
where
and
Gas pressure is 2 MPa, injection pressure is 60
MPa
19Comparison of the results
where
and
Gas pressure is 2 MPa, injection pressure is 60
MPa (b) Modified WAVE c,d) conventional WAVE
B110 B160
20SPRAY BREAK-UP MODELS (Conclusions)
- The modified WAVE model can explain the main
properties of sprays at the initial stage of
penetration - The development of more rigorous physical and
mathematical versions of this model is essential - (Martynov, S.B., Sazhin, S.S., Gorokhovski, M.A.,
Chtab, A., Karimi, K, - Crua, C, Heikal, M.R. (2008) A modified
wave model for transient liquid sprays,
Atomization and Sprays, (submitted). - Sazhin, S.S., Martynov, S.B., Kristyadi, T.,
Crua, C., Heikal, M.R. (2008) Diesel fuel spray
penetration, heating, evaporation and ignition
modelling versus experimentation, International J
of Engineering Systems Modelling and Simulation,
1(1) (in press)).
,
21VORTEX RING MODELS
,
22Schematic view of vortex ring generator (Gharib
et al.,1998 )
23Formation stage (Gharib et al.,1998 )
L/Dlt4
optimal ring
L/D4
L/Dgt4
24Gasoline engine injectors
Injector A B Fuel injector type Port
(PFI) Direct (G-DI) Nominal fuel pressure 3.5
bar 100 bar Fuel temperature 22 C 22
C Fuel type Iso-octane (2,2,4 TMP) Iso-octane
(2,2,4 TMP) Injection frequency 1 Hz 1
Hz Injection duration 5 ms 2 ms Air
pressure 1 bar 1 bar Air temperature 20
C 20 C Orifice size 200 µm
250 µm
25VORTEX RING-LIKE STRUCTURE IS GASOLINE ENGINE
(injector A)
,
26VORTEX RING-LIKE STRUCTURE IS GASOLINE ENGINE
(injector B)
,
27Schematic view of a vortex ring
28Schematic view of a vortex ring
29VORTEX RING MODELS
,
30Formulation of the problem
,
ring-to-core radius
31Approximate solution
32Velocity of the centroid at r0
,
33 Velocity of the centroid at r0
,
34 Velocity of the centroid at r0 (short times)
,
? 0.57721566 is the Euler constant, ?(x) is the
di-gamma function
35 Velocity of the centroid at r0 (long times)
,
36 The region of maximal vorticity
,
37 Velocity of the region of maximal vorticity
,
38 Velocity of the region of maximal vorticity at
long times
,
T 3 t-3b
39 Velocity of the region of maximal vorticity
,
40 Velocity of the region of maximal vorticity
,
41VORTEX RING MODELS (Conclusions)
- A generalised vortex ring model is based on the
assumption that the time dependence of the vortex
ring thickness l is given by the relation atb,
where a is an arbitrary positive number, and 1/4
b 1/2. In the case when av2?, where ? is the
laminar kinematic viscosity, and b1/2, the
predictions of the generalised model are
identical with the predictions of the
conventional model. - The predictions of the model are compared with
the results of experimental studies of vortex
rings in gasoline engine-like conditions with a
high pressure (100 bar) G-DI injector and a
low-pressure (3.5 bar) port fuel injector (PFI).
The G-DI results has shown good agreement with
the model. In contrast, the agreement of the PFI
results with the model has been poor.
42Other Recent Results
43Transient heating of a semitransparent spherical
body
- Sazhin, S.S., Krutitskii, P.A., Martynov, S.B.,
Mason, D., Heikal, M.R., - Sazhina, E.M. (2007) Transient heating of
a semitransparent spherical body, Int J Thermal
Science, 46(5), 444-457.
when RdltRltRg
44Evaporation of droplets into a background gas
kinetic modelling
- Sazhin, S.S., Shishkova, I.N., Kryukov, A.P.,
Levashov, V.Yu., Heikal, M.R. (2007) Evaporation
of droplets into a background gas kinetic
modelling, Int J Heat Mass Transfer, 50,
2675-2691.
45Approximate analysis of thermal radiation
absorption in fuel droplets
when RdltRltRg
46Approximate analysis of thermal radiation
absorption in fuel droplets
- Sazhin, S.S., Kristyadi T., Abdelghaffar, W.A.,
Begg, S., Heikal, M.R., Mikhalovsky, S.V., Meikle
S.T., Al-Hanbali, O. (2007) Approximate analysis
of thermal radiation absorption in fuel droplets,
ASME J Heat Transfer, 129, 1246-1255.
47Particle grouping in oscillating flows
- .
- Sazhin S.S., Shakked, T., Sobolev, V.,
Katoshevski, D. (2008) Particle grouping in
oscillating flows, European J of Mechanics
B/Fluids, 27, 131-149.
Velocities are normalised by ?/k, the distance by
1/k and the time by 1/?
48Monodisperse droplet heating and evaporation
experimental study and modelling
- Maqua, C., Castanet, G., Grisch, F., Lemoine, F.,
Kristyadi, T., Sazhin, S.S. (2008) Monodisperse
droplet heating and evaporation experimental
study and modelling, International J of Heat and
Mass Transfer (in press).
Plots of ethanol droplet temperature Td, measured
experimentally (solid triangles) and predicted by
the model (Tds droplet temperatures at the
surface of the droplet, Tdav average droplet
temperature, and Tdc droplet temperature at the
centre of the droplet) and gas temperature Tg for
the initial conditions Rdo 118.65 µm, Tdo294 K,
C3.97
49Acknowledgements
- The authors are grateful to the European Regional
Development Fund Franco-British INTERREG IIIa
(Project Ref 162/025/247) and EPSRC (Project
EP/E047912/1) for financial support.
50Thank you for your attentionAny comments or
suggestionswould be highly appreciated
51Spray dynamics as a multi-rate process
- Sergei SAZHIN, Sergey MARTYNOV,
- Felix KAPLANSKI, Steven BEGG
- Sir Harry Ricardo Laboratories, Internal
Combustion Engines Group, School of Environment
and Technology, Faculty of Science and
Engineering, University of Brighton, Brighton,
BN2 4GJ, UK - Department of Mechanical Engineering,
University College London, Torrington Place,
London, WC1E 7JE, UK -
- Laboratory of Multiphase Physics, Tallinn
University of Technology, Tallinn 19086, Estonia
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