Primary Atomization (Near Nozzle Flows) Guidance on Experiments and Simulations to be Performed Sibendu Som: Argonne National Laboratory October 2 nd 2014.

Slides:



Advertisements
Similar presentations
A mathematical model of steady-state cavitation in Diesel injectors S. Martynov, D. Mason, M. Heikal, S. Sazhin Internal Engine Combustion Group School.
Advertisements

Topic 4: Panel Discussions 1 April 5, 2014 EFC Panelist-inspired Open Discussion 1.Assessment of 4.1Dave Reuss 2.Assessment of 4.2 Dan Haworth 3.Assessment.
Instituto Brasileiro de Petróleo e Gás UniversityofBrighton Airflow and Fuel Spray Interaction in a Gasoline DI Engine Professor Morgan Heikal Internal.
Status – Validation of Eulerian Spray Modelling University of Zagreb Faculty of Mechanical Engineering and Naval Architecture Department of Energy, Power.
ECN 2: Future Directions 1/4 September 2012 ECN2 Future Direction Continue – Spray A baseline – Soot New – Large, single-hole nozzle. – Spray B – GDI injector.
1 ECN Topic 1.1 Modeling Results Compiled by David P. Schmidt UMass Amherst *Hanabusa Itchō (1652–1724)
1  Introduction (10 min)  Experimental Activities (60 min) 3.1 Injector geometry assessment  Yongjin Jung* (KAIST/Sandi), Peter Hutchins (Infineum/ESRF)
ECN3 Introduction Lyle Pickett (Sandia), Gilles Bruneaux (IFPEN), Raúl Payri (CMT) 4-5 April 2014 University of Michigan.
Ultra-Fast X-Ray Radiography for the Study of Fuel Sprays U.S. Department of Energy, Energy Efficiency and Renewable Energy Vehicle Technologies Program.
This work and the use of the APS were supported by US Department of Energy, Office of Science/Basic Energy Science and Energy Efficiency and Renewable.
Droplets Size and Velocity Measurements in a Spray from a Common Rail System for DI Diesel Engines L. Allocca, S.Alfuso, M.Auriemma, G. Valentino Istituto.
Spray-Turbulence Interaction
FUEL INJECTION SYSTEMS WITH A FOCUS ON FUEL ATOMIZATION By: David Shamrell.
Educated Spray A Geometry Thomas Furlong Prof. Caroline Genzale August 2012.
Spray G Modeling ECN 3.0 April 5 th, ECN 3: Spray G - Spray Modeling 2 April 4-5, 2014 Participating InstitutionAbbreviationResearcher(s) Argonne.
© Fluent Inc. 5/10/2015N1 Fluids Review TRN Postprocessing and Visualization.
LES Combustion Modeling for Diesel Engine Simulations Bing Hu Professor Christopher J. Rutland Sponsors: DOE, Caterpillar.
High-Speed Microscopic Imaging of the Initial Stage of Diesel Spray Formation and Primary Breakup C. Crua, T. Shoba, M. Heikal, University of Brighton.
ECN4-Topic 10: Spray G in Engines Guidance Brian Peterson & Wei Zeng & Sandia National.
1 Gasoline Spray (Spray G) Topic 3.5Internal flow modeling Topic 3.5 Internal flow modeling Ron Grover (GM) Spray G – Internal Flow Modeling.
Gasoline Spray (Spray G)
ICHS 2007, San Sebastian, Spain 1 SAFETY OF LABORATORIES FOR NEW HYDROGEN TECHNIQUES Heitsch, M., Baraldi, D., Moretto, P., Wilkening, H. Institute for.
Analysis of In-Cylinder Process in Diesel Engines P M V Subbarao Professor Mechanical Engineering Department Sudden Creation of Young Flame & Gradual.
Design of Scintillator Die Fermi National Accelerator Laboratory Department of Mechanical Engineering Northern Illinois University.
DETAILED TURBULENCE CALCULATIONS FOR OPEN CHANNEL FLOW
Design of Port Injection Systems P M V Subbarao Professor Mechanical Engineering Department Collection of Models to Predict Multi-physics of Spray …...
Models for Design & Selection of Injection System P M V Subbarao Professor Mechanical Engineering Department Mathematical Tools for Sizing of Hard Ware.
Analysis of Fuel Injection & Related Processes in Diesel Engines
Some Ideas For Metrology to Extend Capability and Attract Investors and Users from Methods Development Communities Art Ruggles, UTNE.
N.P.Basse, M.Abrahamsson, M.Seeger and T.Votteler
Simulation of Droplet Drawback in Inkjet Printing
ICHS4, San Francisco, September E. Papanikolaou, D. Baraldi Joint Research Centre - Institute for Energy and Transport
1 Distribution A. Approved for public release; distribution is unlimited. Integrity  Service  Excellence Aerospace Vehicles Division April 2015.
4 th ICHS San Francisco, September 2011 Numerical Investigation of Subsonic Hydrogen Jet Release Boris Chernyavsky 1, Pierre Benard 1, Peter Oshkai.
Neutrino Factory / Muon Collider Target Meeting Numerical Simulations for Jet-Proton Interaction Wurigen Bo, Roman Samulyak Department of Applied Mathematics.
University of Illinois at Urbana-Champaign Computational Fluid Dynamics Lab Bin Zhao 1 LES Simulation of Transient Fluid Flow and Heat Transfer in Continuous.
Wet Stack Fine Particulate Method/CEMS Development Measurement Technology Workshop January 29, 2013.
Auto Ignition, Premixed & Diffusive Combustion in CI Engines
Dr. R. Nagarajan Professor Dept of Chemical Engineering IIT Madras
INTRODUCTION Many heat and mass transfer processes in column apparatuses may be described by the convection – diffusion equation with a volume reaction.
Compression Ignition Engines
Topic 1 – Internal flow Presenter: Marco Arienti, Sandia National Laboratories Support by Sandia National Laboratories’ LDRD (Laboratory Directed Research.
T HE E VAPORATIVE C OOLING E FFECTS OF V ARYING W ATER D ROPLET C HARACTERISTICS ON A M ETAL S URFACE I N A S TEADY S TATE, H IGH T EMPERATURE A IR F LOW.
ECN4 Introduction Lyle Pickett (Sandia), Gilles Bruneaux (IFPEN), Raúl Payri (CMT) 5-6 Sept 2015 Kyoto University.
ECN 4 Topic 8: Internal & Near Nozzle Flow Modeling Spray G Organizer: Chris Powell Argonne National Laboratory Ronald Grover, Presenter.
CFD Lab 1 Simulation of Turbulent Pipe Flow Seong Mo Yeon, Timur Dogan, and Michael Conger 10/07/2015.
Spray G - Program 9:30 Introduction
ON THE DESIGN OF HYPERSONIC INLETS 3rd Symposium on Integrating CFD & Experiments in Aerodynamics USAFA, CO June, 2007 Capt Barry Croker Executive.
1 13:00 Introduction Experimental Activities 13:153.1 Injector geometry assessment  Yongjin Jung* (KAIST), Peter Hutchins (Infineum/ESRF) 13:203.2 Rate-of-injection.
GMUWCollaborative Research Lab Near-Nozzle Diesel Spray Imaging Using Visible Light T.E. Briggs & P. V. Farrell Diesel combustion systems must continue.
Post Injection Process in Port Injection Systems P M V Subbarao Professor Mechanical Engineering Department Models Based Predictions of Multi-physics.
Date of download: 6/3/2016 Copyright © ASME. All rights reserved. From: Enhanced Splash Models for High Pressure Diesel Spray J. Eng. Gas Turbines Power.
Mixing Length of Hydrogen in an Air Intake Greg Lilik EGEE 520.
Date of download: 6/21/2016 Copyright © ASME. All rights reserved. From: RANS and Large Eddy Simulation of Internal Combustion Engine Flows—A Comparative.
Date of download: 9/18/2016 Copyright © ASME. All rights reserved. From: Grid-Convergent Spray Models for Internal Combustion Engine Computational Fluid.
CFD ANALYSIS OF MULTIPHASE TRANSIENT FLOW IN A CFB RISER
SIMULATION ANALYSIS ON THE RISK OF HYDROGEN
Tsinghua University, Beijing, China
The Tilted Rocket Rig: A Rayleigh–Taylor Test Case for RANS Models1
Design of Port Injection Systems for SI Engines
2D Free Jet Simulations (FLUENT)
Date of download: 10/16/2017 Copyright © ASME. All rights reserved.
Integrating Modeling and Physical Testing for Assessing Filtered Exhaust Stack Sampling Probe Location Xiao-Ying Yu, Kurtis P. Recknagle, John A. Glissmeyer,
Date of download: 10/27/2017 Copyright © ASME. All rights reserved.
Date of download: 10/27/2017 Copyright © ASME. All rights reserved.
CI-DI I C Engines for Automobiles
Simulation of turbulent airfoil Flow Using FlowLab 1.1 (CFD PreLab 2)
Development of Design Knowledge for GDI Internal Combustion Engines
E. Papanikolaou, D. Baraldi
Post Injection Processes in Diesel Engines
Presentation transcript:

Primary Atomization (Near Nozzle Flows) Guidance on Experiments and Simulations to be Performed Sibendu Som: Argonne National Laboratory October 2 nd 2014

Experimental Objectives Focus on the near nozzle region within first 10 mm Concentrate on non-vaporizing experiments Provide boundary conditions for initializing the simulations for both Spray A and Spray B – Nozzle geometry – Rate of injection – Needle lift & off-axis motion – Injection pressure vs. time Provide data for validation for both Spray A and Spray B – Liquid mass distribution at nozzle exit and in the spray region – Droplet sizes – Qualitative physics to understand the spray processes – liquid penetration Assess the uncertainties for all of these parameters

Modeling Objectives Focus on the near nozzle region within first 10 mm Encourage high-fidelity simulations of fuel sprays to understand the primary atomization physics Capture the SOI and EOI physics for single and multi-hole injectors Capture the spray physics during the main injection process for both single and multi-hole injectors Study the capability of the different modeling approaches (Lagrangian-Eulerian, Eulerian-Eulerian) and CFD frameworks (RANS, LES, DNS) for the simulation of the primary atomization Assess which physical phenomena are important for including in models: Turbulence, Compressibility, …?

Target Injectors Spray A – Diesel nozzle, single hole, n-dodecane, non-cavitating – High resolution (1 mm) X-ray tomography of Nozzle 675 – Ultra High resolution (0.6 mm) tomography for 678, & 679 – Lift and wobble measured for all nozzles – The target injector will be Spray B – Diesel nozzle, 3-hole, n-dodecane –.stl files available for 196, 198, 199, 201 – Lift and wobble measured for all the injectors – The target injector will be 201 – Ultra High resolution (0.6  m) tomography completed and a CFD ready mesh is available

Conditions of Interest: Experiments Spray A and B operating conditions from Argonne: ( – Spray A: 675; Spray B: 201 – Priority 1: Pinj = 150 MPa; Priority 2: 100 MPa – Fuel temperature: Spray A K; Spray B – 338 K Spray A and Spray B conditions at Sandia and Univ. of Brighton: – Spray A: 675; Spray B: 201 – ?? Spray A and Spray B conditions at Chalmers??: – Spray A: 675; Spray B: 201 – ??

Conditions of Interest: Simulations Spray A and B operating conditions from Argonne: ( – Spray A: 675; Spray B: 201 – Priority 1: P inj = 150 MPa; Priority 2: P inj = 100 MPa – Fuel temperature: Spray A K; Spray B – 338 K Ambient gas temperature303 (K) Ambient gas pressure2.0 (MPa) Ambient gas density22.8 (kg/m3) Ambient gas N 2 (by volume)100%

Anticipated Experimental Results Microscopic measurements of the initial penetration and spreading angle as the needle opens Break up and mixing of the sprays at the end of injection at the microscopic level, possible dribble? USAXS droplet sizing and perhaps optically measured droplet size as well X-ray radiography of Spray A and Spray B nozzles and plumes of interest Ballistic imaging of near-nozzle region

For both Spray A and Spray B injectors: Mass flow rate at the nozzle exit from virtual ROI tool from CMT and measured nozzle coefficients (already available from ECN3) Fuel spray penetration vs. time from long-distance microscopy and diffused back-illumination Contour plots of projected liquid density at 0.1 ms and 0.5 ms from Argonne Transverse mass distribution (projected density across the spray) profiles averaged between 0.5 – 1.0 ms: o x = 0.1, 0.6, 2, 6, and 10 mm downstream to nozzle exit o Projection plane is 0°plane (i.e., plane containing fuel inlet, or projection along the z-axis with the injector in the theta = 0 position) Liquid volume fraction (LVF) across cross-section at x = 0.1, 0.6, 2, 6, 10 mm o the y-axis cut plane Transverse integrated mass (TIM) vs. axial 0.5 ms Mean droplet size (SMD) at x = 1, 4, 8 mm at 0.5 ms after SOI o Mean SMD at the above axial positions vs. axial position Data Needed from Experiments

Mass flow rate at the nozzle exit Fuel spray penetration vs. time (0.1% liquid mass fraction) Contour plots of projected density in the 0°plane at 0.1 and 0.5 ms after actual SOI Transverse mass distribution (projected density across the spray) in ug/mm x = 0.1, 0.6, 2, 6, and 10 mm downstream to nozzle exit: o between 0.5 – 1.0 ms after SOI, at intervals of 0.1 ms o Averaged profiles between ms at the above locations 2D contours of LVF at x = 0.1, 0.6, 2, 6, 10 mm at 0.5, 0.75, and 1.0 ms Transverse integrated mass profiles at 0.5 ms after SOI: o x = 0.1 mm, 0.6 mm, 2 mm, 6 mm, and 10 mm Mean droplet size (SMD) at x = 1, 4, 8 mm at 0.5 ms after SOI o Mean SMD at the above axial positions vs. axial position o Distributions of SMD vs. radial position at the above axial positions Dynamics: peak projected density and Full Width Half Maximum (FWHM) of distribution at x = 0.1, 2, 6 mm from nozzle for entire duration of the injection event (in intervals of 20 μs) Data Needed from Spray A Simulations Set-up conditions from Argonne

Spray B target injector (201): Compare results between different plumes for condition # 1 o Penetration vs. time o Transverse mass distribution at 0.1 mm, 2 mm, and 6 mm o Mean SMD at 1, 4 mm at 0.5 ms after SOI vs. axial position Data Needed from Spray B Simulations For plume # 3 which is measured at Argonne Contour plots of projected density in the 0°plane at 0.1 and 0.5 ms Transverse mass distribution (projected density across the spray) in ug/mm x = 0.1, 0.6, 2, 6, and 10 mm downstream to nozzle exit: o between 0.5 – 1.0 ms after SOI, at intervals of 0.1 ms o Averaged profiles between ms at the above locations 2D contours of LVF at x = 0.1, 0.6, 2, 6, 10 mm at 0.5, 0.75, 1.0 ms Transverse integrated mass profiles at 0.5 ms after SOI: o x = 0.1 mm, 0.6 mm, 2 mm, 6 mm, and 10 mm Mean droplet size (SMD) at x = 1, 4, 8 mm at 0.5 ms after SOI o Mean SMD at the above axial positions vs. axial position o Distributions of SMD vs. radial position at the above axial positions Set-up conditions from Argonne

Confirmed Participants and Volunteers Experiments Argonne, Sandia, Univ. of Brighton Confirm participation: Chalmers Simulations Argonne + Univ. of Perugia, ASU, Aachen, Sandia, CMT, GATECH Confirm participation: UMass, IFPEN, Coria Possible volunteers Experiments: ?? Simulations: ??