2D Jet Simulation Updates Jan.23 rd 2014 Yan Zhan SUNY Stony Brook 1.

Slides:



Advertisements
Similar presentations
Vortex instability and the onset of superfluid turbulence
Advertisements

FLOW IN POROUS BEDS Industrial application Porous bed:  porous material (felt, ceramics, paper)  granular bed (sand, filter cake)  packing (spheres,
Motion of particles trough fluids part 1
University of Western Ontario
Results of 2D Hg Jet Simulation and Experimental Data Yan April 10 th
Nozzle Study Yan Zhan, Foluso Ladeinde April, 2011.
MUTAC Review April 6-7, 2009, FNAL, Batavia, IL Mercury Jet Target Simulations Roman Samulyak, Wurigen Bo Applied Mathematics Department, Stony Brook University.
National Aeronautics and Space Administration Numerical Simulation of a fully turbulent flow in a pipe at low Reynolds numbers Click to edit.
Continuity Equation Tutorial
UNICAMP THE HEIGHT OF LIQUID METHOD FOR FREE SURFACE FLOWS Flow simulations of real processes often involve fluids that are separated by a sharp interface.
PHYS16 – Lecture 35 Sound December 3, 2010 “Since light travels faster than sound, is that why some people appear bright until you hear them speak?”
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2005, LBNL Target Simulation Roman Samulyak, in collaboration with.
CE1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
PHYS16 – Lecture 40 Ch. 17 Sound.
CE 230-Engineering Fluid Mechanics Lecture # 18 CONTINUITY EQUATION Section 5.3 (p.154) in text.
Many people will expect the rain drop size should be as follows:
CE 230-Engineering Fluid Mechanics Lecture # 2&3 Fluid properties (1)
Kelvin Effect: Physical Cartoon Equilibrium vapor pressure is higher over a curved surface than a flat one. Important for nucleation of new particles,
Drag The trajectory of an ink droplet stream ejecting horizontally out of an inkjet printer is photographed as shown below. It is counterintuitive that.
CEE 262A H YDRODYNAMICS Lecture 1* Introduction and properties of fluids *Adapted from notes by Prof. Stephen Monismith 1.
Fixed and Fluidized Beds
Valves In Industry (Part 3).
Simulation of Droplet Drawback in Inkjet Printing
Falling Liquid Film Flow along Cascade- type First Wall of Laser-Fusion Reactor T. Kunugi, T. Nakai, Z. Kawara Department of Nuclear Engineering Kyoto.
1 Institute for Fluid Mechanics and Heat Transfer Conex mid-term meeting, Oct 28th 2004, Warsaw 1 Numerical simulation of the flow in an experimental device.
Brookhaven Science Associates U.S. Department of Energy MUTAC Review April , 2004, LBNL Target Simulation Roman Samulyak, in collaboration with.
1 Modeling and validation of coal combustion in a circulating fluidized bed using Eulerian-Lagrangian approach U.S. Department of Energy, National Energy.
CE 230-Engineering Fluid Mechanics Week 1 Introduction.
Design Analysis of Furnace Of A Steam Generator P M V Subbarao Professor Mechanical Engineering Department Perfection of Primary Cause for All that Continues…..
Neutrino Factory / Muon Collider Target Meeting Numerical Simulations for Jet-Proton Interaction Wurigen Bo, Roman Samulyak Department of Applied Mathematics.
1 MICRO FLOWS: AN INTRODUCTION Michael Shusser. 2 SIZE RANGES OF MACRO, MICRO, AND NANO DEVICES.
Aerodynamic Forces Lift and Drag.
J.-Ph. Braeunig CEA DAM Ile-de-FrancePage 1 Jean-Philippe Braeunig CEA DAM Île-de-France, Bruyères-le-Châtel, LRC CEA-ENS Cachan
Lecture Objectives Unsteady State Simulation Example Modeling of PM.
ACOUSTIC THEORY  WAVE VELOCITY  ACOUSTIC IMPEDANCE  REFLECTION AND TRANSMISSION  REFRACTION  RADIATION  ATTENUATION.
Simulation Of 2D Hg Jet Using Implicit LES Method Yan March. 20 th
Numerical simulation of droplet motion and two-phase flow field in an oscillating container Tadashi Watanabe Center for Computational Science and e-Systems.
Governing Equations Conservation of Mass Conservation of Momentum Velocity Stress tensor Force Pressure Surface normal Computation Flowsheet Grid values.
TransAT Tutorial Separation of Oil, Gas & Water July 2015 ASCOMP
Brookhaven Science Associates U.S. Department of Energy Muon Collider/Neutrino Factory Collaboration Meeting LBL, February , 2005 Target Simulation.
CFD Study of the Development of Vortices on a Ring Wing
1 NUMERICAL AND EXPERIMENTAL STUDIES OF THIN-LIQUID-FILM WALL PROTECTION SCHEMES S.I. ABDEL-KHALIK AND M. YODA G. W. Woodruff School of Mechanical Engineering.
Targetry Simulation with Front Tracking And Embedded Boundary Method Jian Du SUNY at Stony Brook Neutrino Factory and Muon Collider Collaboration UCLA.
Modelling Spray Impingement
Direct Numercal Simulation of two-phase turbulent boundary layer over waved water surface O. A. Druzhinin, Yu.I. Тroitskaya Institute of Applied Physics.
CFX Slide serial no 1 © 2003 ANSYS CFX CFX-5.6 Multiphase Course Free Surface Lecture 5 Free Surface Flow.
TransAT Tutorial Dam Break June 2015 ASCOMP
TransAT Tutorial Flow over a Cylinder (Re=150) June 2015 ASCOMP
Boundary Layer Correction Air enters a two-dimensional wind tunnel as shown. Because of the presence of the boundary layer, fluid will be displaced away.
Fluids – Special Topics
Indian Institute of Space Science and Technology STUDY OF EFFECT OF GAS INJECTION OVER A TORPEDO ON FLOW-FIELD USING CFD.
CFD Simulation Investigation of Natural Gas Components through a Drilling Pipe RASEL A SULTAN HOUSSEMEDDINE LEULMI.
Droplet Dynamics Multi-phase flow modelling Background D d = 0.001m,  d = 1000 kg/m 3,  d = kg/ms,  ad = N/m,  a = 1 kg/m 3,  a = 1 ×
CFD ANALYSIS OF MULTIPHASE TRANSIENT FLOW IN A CFB RISER
From: Hydraulic Loss of Finite Length Dividing Junctions
Workshop 7 Tank Flushing
2D Free Jet Simulations (FLUENT)
2D Jet Simulation Testing
The inner flow analysis of the model
Model Validation Drop Collisions: Exp. vs. Sim.
Isothermal Two-Phase Pipe Flow Sim
Flow Through a Pipe Elbow (Comsol)
Date of download: 12/16/2017 Copyright © ASME. All rights reserved.
Lecture Objectives Unsteady State Ventilation Modeling of PM.
Sunny Ri Li, Nasser Ashgriz
Secondary Atomisation in Disturbed Flow Fields
Effect of Flow over a Cylinder MAE 5130 Viscous Flow Final Project
Fixed and Fluidized Beds
Boundary Layer Correction
Presentation transcript:

2D Jet Simulation Updates Jan.23 rd 2014 Yan Zhan SUNY Stony Brook 1

Problem 1: Water-Air Jet An axis-symmetric water jet into still air with a mean bulk velocity of m/s (D = 0.01m, and Re = 50,000). 2

Boundary Conditions Outflow 3

Jet Characteristics Physical Characteristics Numerical Characteristics – Determination of the mesh size: Assume only primary breakup, the critical liquid Weber number is 10, then Δx_critical = 34.4μm 4 Diameter (D)VelocityTurbulent Intensity m m/su‘/U = 0.05 PhaseDensityViscositySurface Tension Air1.225 kg/m ×10 -5 m 2 /s N/m Water998 kg/m 3 0.9×10 -6 m 2 /s

Mesh Halved (axis-symmetric) model with grid# of 822,000 5

Results (t = s) 6

Problem 2: Menard’s Test [1] 7 [1] T. Menard, etc., Coupling level set/VOF/ghost fluid methods: Validation and application to 3D simulation of the primary break-up of a liquid jet, International Journal of Multiphase Flow 33 (2007) 510–524 50D 20D An axis-symmetric liquid jet into still gas with a mean bulk velocity of 100 m/s (D = 100 μm, and Re = 5,800).

Menard’s Results [1] 8 Jet development and penetration (dt = 2.5 μm)

Boundary Condition 9 50D 20D Outflow

Jet Characteristics Physical Characteristics Numerical Characteristics – Determination of the mesh size: Assume only primary breakup, the critical liquid Weber number is 10, then Δx_critical = 2.36 μm 10 Diameter (D)VelocityTurbulent Intensity 100 μm100 m/su‘/U = 0.05 PhaseDensityViscositySurface Tension Gas25 kg/m 3 4x10 -7 m 2 /s 0.06 N/m Liquid696 kg/m ×10 -6 m 2 /s

Mesh 11 Halved (axis-symmetric) model with grid# of 1,146,880

Results 12 Set Up 1 (t = 0 s):

Results 13 Set Up 1 (t = 10 μs):

Results 14 Set Up 1 (t = 30 μs):

Results 15 Set Up 2 (iteration = 0 ):

Results 16 Set Up 2 (iteration = 1500 ): :

Results 17 Set Up 2 (iteration = 3500) :

Results 18 Set Up 2 (iteration = 4500) : Next: Turn to Unsteady Simulation

More Information 19 [2] P-K Wu and G M Faeth, Onset and end of drop formation along the surface of turbulent liquid jets in still gases, Phys. Fluids, Vol. 7, No. 11, November 1995 Surface breakup regime map for turbulent liquid jets in still gases when aerodynamic effects are small (liquid/gas density ratios are larger than 500) [2]

More Information 20 Problem # Problem 12,90450, d10.387d Problem 211,6005, d106.4d