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Monday, May 13th<br />
Tuesday, May 14th<br />
Wednesday, May 15th<br />
Thursday, May 16th<br />
optical line of sight diagnostics and hence the in-situ measurements<br />
of temperature and soot concentrations. Effects of diffusion<br />
and turbulence are minimised here and efforts are therefore<br />
paid on the modelling of combustion chemistry, radiation and<br />
soot formation. For improved computational runtime, a two-step<br />
chemical reaction scheme proposed by Westbrook and Dryer is<br />
used together with a steady-state solver. The steady-state solver is<br />
developed by modifying an existing solver, Local Time Stepping<br />
(LTS) ReactingParcelFoam. Akin to reactingFoam, which has been<br />
widely used in combustion simulations, LTSReactingParcelFoam is<br />
also applicable for laminar and turbulent reacting flow but it is a<br />
local time stepping solver for steady-state simulations. The modified<br />
version is henceforth addressed as radiationReactingLTSFoam<br />
(rareLTSFoam). In order to simulate the radiative heat loss, P1 radiation<br />
model is used. The model validation uses two test cases of<br />
laminar premixed flames with different equivalence ratios. In the<br />
first case, a stoichiometric flame is produced in which soot radiation<br />
process can be omitted; while in the second case, a rich flame<br />
with equivalence ratio of 2.15 is used. The results generated by the<br />
integrated CFD chemistry model are validated against temperature<br />
measurements at different heights along the axial direction. For<br />
the radiative heat transfer, a parametric study is conducted using<br />
P1 model. The absorption coefficients are modeled using RADCAL<br />
and WSGGM models. Implementation of the steady-state solver<br />
has been proved to simulate the stabilised, laminar premixed<br />
flame accurately with an expedited calculation. This serves as a<br />
useful platform when comprehensive radiation model such as inite<br />
Volume Discrete Ordinate Method (fvDOM) radiation model<br />
is implemented. Understanding and further improvements on the<br />
robustness of numerical models achieved at this phase are critical<br />
prior to computationally investigating the radiative heat transfer<br />
process in turbulent diffusion flame and diesel engine combustion<br />
that have higher levels of complexity.<br />
Flow and pressure simulation of cooling water,<br />
lubricating oil and fuel supply systems<br />
Andreas Hjort, Wärtsilä, Finland<br />
Juhani Ervasti, Wärtsilä, Finland<br />
Jaakko Koivula, Wärtsilä, Finland<br />
Lars Ola Liavag, Wärtsilä, Finland<br />
Alexandre Pereira, Wärtsilä, Finland<br />
Antonino Di Miceli, Wärtsilä, Finland<br />
When designing fluid systems for four-stroke medium-speed diesel<br />
engines, it is beneficial to use modern simulation tools to achieve<br />
an optimised design in an early phase. Today’s engines have become<br />
very compact and typically have a high degree of integration<br />
of fluid channels into castings. Therefore, changes to address flow<br />
problems after design is complete will require big re-design efforts<br />
and should be avoided. The heat balance of the engine determines<br />
the needed cooling water flow to achieve sufficient cooling without<br />
excessive temperature increase in the water. As the pumps used<br />
are of centrifugal type the flow in the system is determined by the<br />
system pressure drop. CFD simulation of complicated channelling<br />
as part of the design phase will ensure unnecessary pressure drop<br />
is avoided and thus the water flow through the system will be increased.<br />
A well-designed cooling system will have the majority of<br />
the pressure drop in coolers and as little as possible in the channels<br />
and piping. Oil pumps for four-stroke diesel engines must be<br />
dimensioned to ensure sufficient pressure is available in the critical<br />
components at all conditions. Over-dimensioning of the oil pump<br />
will lead to unnecessary oil flow wasted through the pressure control<br />
valve. To determine the exact oil flow through the engine in<br />
the design phase is difficult, as the oil system has many consumers<br />
with different characteristics. 1D flow simulation of a complete oil<br />
system gives a sufficiently accurate prediction of the needed flow<br />
to avoid over- or under-dimensioning of the oil pump and avoid<br />
excessive pressure drop in any part of the oil system. Pressure pulsation<br />
from mechanical fuel pumps to the fuel supply line can be<br />
a source for vibration both on the engine itself but also in the external<br />
fuel piping of the installation, e.g. ship. By 1D simulations<br />
of the fuel supply system, the pulsation can be predicted and the<br />
need for damping can be determined. This paper presents successful<br />
simulation projects of all the above mentioned systems.<br />
Turbulence during the compression stroke<br />
Eero Antila, VTT Technical Research Centre of Finland, Finland<br />
Mika Nuutinen, Aalto University, Finland<br />
Ossi Kaario, Aalto University, Finland<br />
Normally, diesel combustion simulations are started from bottom<br />
dead centre before combustion. Initial values of pressure and temperature<br />
are taken from experimental results or 1D-simulations.<br />
As initial turbulence values (k and ε), some correlation, intake<br />
flow simulation or just best practise values are used. All those values<br />
are initialised to be constant for whole simulation volume. In<br />
the previous study, intake channel simulations were done. Authors<br />
found that the level of turbulence values at TDC were different if<br />
the intake stroke was simulated or if average values were initialised<br />
at IVC. In this paper three different engines are simulated. For each<br />
engine intake and compression strokes are simulated to get the<br />
best possible knowledge about the real turbulence values. From<br />
those results the average values of p, T, k, ε and swirl number at<br />
IVC are captured and used as initial values of compression simulation.<br />
Finally, a better method to initialise turbulence values is<br />
described and tested.<br />
Wednesday May 15th / 13:30 – 15:00 Room B<br />
Environment, Fuel & Combustion<br />
Gas and Dual-Fuel Engines – Abnormal Combustion<br />
Understanding the influence of heat transfer and<br />
combustion behaviour on end gas knock in heavyduty<br />
lean burn engines<br />
Joel Hiltner, Hiltner Combustion Systems, USA<br />
The onset of end gas knock remains one of the primary factors<br />
limiting the thermal efficiency, fuel flexibility, specific power output,<br />
and transient capability of lean burn natural gas engines. In<br />
the past two decades, huge strides have been taken to improve the<br />
performance of these engines, based largely on a fundamental<br />
understanding of the impact of thermodynamic design and fuel<br />
properties on the resistance of a given combustion platform to engine<br />
knock. Simulation tools based on this knowledge have led to<br />
optimised designs as regards expansion ratio, Miller cycle utilisation,<br />
and other design approaches aimed at limiting end gas temperatures.<br />
Two basic engine phenomena whose impact on knock<br />
is less well understood are in-cylinder heat transfer and overall<br />
combustion rate, phasing, and stability. In-cylinder heat transfer<br />
has a profound impact on charge temperatures and can lead either<br />
to increased or decreased knock tolerance for a given design,<br />
depending on a number of factors. Combustion chamber surface<br />
temperatures are a function of detail design, engine load, and engine<br />
operating condition and have a direct impact on heat transfer<br />
rates during compression and the early part of combustion. Incylinder<br />
bulk flow and turbulence level induced, for example, by<br />
swirl and squish also impact the heat transfer rate and thus the unburned<br />
gas temperature. The influence of these heat transfer effects<br />
May 2013 | Schiff&Hafen | Ship&Offshore SPECIAL 55