Department of Mechanical Engineering, IUPUI Christina Koehly Michael Schneider Internship Students from Germany Indiana University - Purdue University.

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

Finite Element Radiative and Conductive Module for use with PHOENICS Department of Materials Engineering, University of Swansea, Swansea, SA2 8PP, UK DERA.
1 Application of for Predicting Indoor Airflow and Thermal Comfort.
SolidWorks Flow Simulation
Outline Overview of Pipe Flow CFD Process ANSYS Workbench
Mid Term Meeting, Sept. 21st-22nd, 2004, Karlsruhe Presentation by: F.Pittaluga - UNIGE-DIMSET Dept. of Fluid Machinery, Energy Systems and Transportation.
CIMNE Fluid-Structure Interaction for Combustion Systems 36-Months Progress Meeting Queen's University of Belfast Belfast UK Jan 24.
Svetlana Marmutova Laminar flow simulation around circular cylinder 11 of March 2013, Espoo Faculty of Technology.
University of Western Ontario
The Flame Deflector and Five Segment Booster By: Geoffrey Husk.
Computer Simulation of Vehicle Aerodynamic Forces and Moments Using Fluent 6.2 MSC VisualNastran 4D WorkingModel 2D Zerguy Maazouddin California State.
Youngwook Kang, Cornell University Andrei Simion, The Cooper Union
Interactive System for Pulverized Coal Combustion Visualization with Fluid Simulator Marek Gayer, Pavel Slavík and František Hrdlička Department of Computer.
1 “CFD Analysis of Inlet and Outlet Regions of Coolant Channels in an Advanced Hydrocarbon Engine Nozzle” Dr. Kevin R. Anderson Associate Professor California.
NNMREC Arshiya Hoseyni Chime Advisor: Professor Phil Malte UW –NNMREC 04 November 2012.
C OMPUTATIONAL F LUID D YNAMIC M ODEL OF A RTERIOVENOUS F ISTULA A NASTOMOSIS TO S TUDY THE E FFECTS OF V ESSEL S IZE AND P RESSURE G RADIENT ON THE P.
2L 2aL s h T Introduction Zach Frye, University of Wisconsin-Eau Claire Faculty Advisors: Mohamed Elgindi, and John Drost, Department of Mathematics Funded.
Aerodynamic Study of Go-kart Nose Cones ME450 Introduction to Computer Aided Engineering Becker, Joe Professor H. U. Akay May 1, 2000.
Analyses of Triangular Die with a Hole ToNICADD-FNALBy Praveen Reddy and Meung Kim ME, NIU.
Nelson Research, Inc – N. 88 th St. Seattle, WA USA aol.com Craig E. Nelson – Consultant Engineer Toothbrush Bristle.
Computer Simulations of Wind Tunnel Experiments
Experimental and Numerical Study of the Effect of Geometric Parameters on Liquid Single-Phase Pressure Drop in Micro- Scale Pin-Fin Arrays Valerie Pezzullo,
ANTEC EXTRUSION SIMULATION AND EXPERIMENTAL VALIDATION TO OPTIMIZE PRECISION DIE DESIGN by Srinivasa Rao Vaddiraju, M.
Triangular Die Analyses ToNICADD-FNALBy Praveen Reddy and Meung Kim ME, NIU.
Preliminary Assessment of Porous Gas-Cooled and Thin- Liquid-Protected Divertors S. I. Abdel-Khalik, S. Shin, and M. Yoda ARIES Meeting, UCSD (March 2004)
Gambit Overview Ahmadi/Nazridoust ME 437/537/637.
Image courtesy of National Optical Astronomy Observatory, operated by the Association of Universities for Research in Astronomy, under cooperative agreement.
ABSTRACT Many new devices and applications are being created that involve transporting droplets from one place to another. A common method of achieving.
Reynolds Method to Diagnosize Symptoms of Infected Flows.... P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Reynolds Averaged.
OPTIMIZATION OF A PROFILE- EXTRUSION DIE DESIGN USING INVERSE CFD SIMULATION June Department of Mechanical Engineering,
Introduction to Fluid Mechanics
1 Short Summary of the Mechanics of Wind Turbine Korn Saran-Yasoontorn Department of Civil Engineering University of Texas at Austin 8/7/02.
Computational Modelling of Unsteady Rotor Effects Duncan McNae – PhD candidate Professor J Michael R Graham.
© Ram Ramanan 8/27/2015 CFD 1 ME 5337/7337 Notes Introduction to Computational Fluid Dynamics Lecture 2: CFD Introduction.
Fluids Fluids in Motion. In steady flow the velocity of the fluid particles at any point is constant as time passes. Unsteady flow exists whenever the.
Introduction to COMSOL Travis Campbell Developed for CHE 331 – Fall 2012 Oregon State University School of Chemical, Biological and Environmental Engineering.
Thermal Model of MEMS Thruster Apurva Varia Propulsion Branch Code 597.
CFD Pre-Lab 2 Simulation of Turbulent Flow around an Airfoil Seong Mo Yeon, and Timur Dogan 11/12/2013.
1 Department: Material science and engineering Discipline: Finite element method By: Anelia Ivanova To: Prof. V. Iliev Subject : Hydrodynamics Simulation.
Page 1 SIMULATIONS OF HYDROGEN RELEASES FROM STORAGE TANKS: DISPERSION AND CONSEQUENCES OF IGNITION By Benjamin Angers 1, Ahmed Hourri 1 and Pierre Bénard.
Numerical investigation on the upstream flow condition of the air flow meter in the air intake assembly of a passenger car Zoltán Kórik Supervisor: Dr.
ANSYS for MEMS by Manjula1 FEM of MEMS on ANSYS MEMS Summer 2007 Why FEM for MEMS? Features in ANSYS Basic Procedures Examples.
Department Of Material Science And Engineering FINITE ELEMENT METHOD UNIVERSITY OF CHEMICAL TECHNOLOGY AND METALLURGY Sofia Nina Velikova, June 2010.
CFX-10 Introduction Lecture 1.
Computational Fluid Dynamics Applied to the Analysis of 10-mm Hydrocyclone Solids Separation Performance S. A. Grady, M. M. Abdullah, and G. D. Wesson.
Compressor Cascade Pressure Rise Prediction
Flowing Matter – COST Action MP1305, , Sofia NUMERICAL ANALYSIS OF THE STENOSIS EFFECTS ON THE BLOOD FLOW IN THE COMMON CAROTID ARTERY BIFURCATION.
ME 101: Fluids Engineering Chapter 6 ME Two Areas for Mechanical Engineers Fluid Statics –Deals with stationary objects Ships, Tanks, Dams –Common.
CFD Study of the Development of Vortices on a Ring Wing
V. Fundamentals of Fluid Dynamics. Contents 1. State of Stress in Moving Fluid 2. Equations of Motion 3. Bernoulli Equation.
Comparison of 5 MW fires in UXC with different geometries Michael Plagge Physics Department Compact Muon Solenoid Experiment Group European Organization.
Appendix A.
한국수자원공사 연구소 배관내부 전산해석 : CFX-5.7 김 범 석 한국해양대학교 유동정보연구실.
Potential Flow and Computational Fluid Dynamics Numerical Analysis C8.3 Saleh David Ramezani BIEN 301 February 14, 2007.
CFD Simulation Investigation of Natural Gas Components through a Drilling Pipe RASEL A SULTAN HOUSSEMEDDINE LEULMI.
ANSYS. Overview of ANSYS It is an engineering simulation software developed in 1970 by Dr. John A. Swanson It was developed to use finite element analysis.
AERODYNAMIC OPTIMIZATION OF REAR AND FRONT FLAPS ON A CAR UNIVERSITY OF GENOVA – POLYTECHNIC SCHOOL ADVANCED FLUID DYNAMICS COURSE 2015/2016 Student: Giannoni.
FOILING MOTH CENTERBOAD ON O PEN FOAM COURSE: ADVANCED FLUID DYNAMICS PROFESSOR: JAN PRALITS STUDENT: ALESSANDRO CHIAPPALONE.
Presenter: Nicholus Tayari Akankwasa
4th Global Engineering, Science and Technology Conference
Workshop 5 Centrifugal Pump
Blade Design for Modern Wind Turbines
Multi-physics Simulation of a Wind Piezoelectric Energy Harvester Validated by Experimental Results Giuseppe Acciani, Filomena Di Modugno, Ernesto Mininno,
11th International Conference on Mechanical Engineering (ICME2015)
MAE 5130: VISCOUS FLOWS Examples Utilizing The Navier-Stokes Equations
Identification of Fundamental Design Parameter for A Wind Turbine
Comparison between Serrated & Notched Serrated Heat Exchanger Fin Performance Presented by NABILA RUBAIYA.
Conservation of Energy/Bernoulli’s Equation
Thermal behavior of the LHCb PS VFE Board
Investigation of Flow Turning in a Natural Blockage
Presentation transcript:

Department of Mechanical Engineering, IUPUI Christina Koehly Michael Schneider Internship Students from Germany Indiana University - Purdue University Indianapolis, USA Berufsakademie (University of Cooperative Education) Karlsruhe, Mannheim, Germany Faculty Advisor: Professor H. U. Akay Aerodynamic study of Jeff Gordon’s NASCAR 2000 March 2001

Jeff Gordon’s NASCAR (BRICKYARD 400, AUGUST 5 th 2000)

Indianapolis Motor Speedway Home of Brickyard 400

Project Objective Use Finite Element code ANSYS/FLOTRAN and Finite Volume code StarCD –Examination of aerodynamic behavior –Comparison of Velocity Magnitude and Static Pressure Decision of which program give better results

THE PROJECT TEAM AT WORK!

Theory: Assumptions Incompressible Fluid Adiabatic Conditions Steady State Newtonian Fluid Turbulent Model PropertyValueUnitsReynolds Number Density1.205kg/m 3 Dynamic Viscosity1.81E-5Ns/m 2 Car Length m 1. Free Stream Velocity35m/s12.17E Free Stream Velocity70m/s24.21E Free Stream Velocity100m/s34.59E+06

ANSYS/FLOTRAN and StarCD Procedure Define the problem Define Keypoints Make Areas from Keypoints Create the Finite Element Mesh Set Boundary Conditions Set Solver Parameters Get the results

Areas

Meshes

Boundary Conditions All Boundary Conditions were applied to lines Velocity applied to surface of the car Velocity of 35 m/s, 70 m/s and 100 m/s applied in x-direction to “inlet” and lower free stream surface Relative Pressure of 0 Pa applied to “outlet”

Parameters Steady-state with turbulent solver Fluid properties set to air in standard SI Solver set to perform more than 500 iterations

RESULTS

Velocity Magnitude 35 m/s StarCD: Velocity by 35 m/s ANSYS: Velocity by 35 m/s

Velocity Magnitude 70 m/s StarCD: Velocity by 70 m/s ANSYS: Velocity by 70 m/s

Velocity Magnitude 100 m/s StarCD: Velocity by 100 m/s ANSYS: Velocity by 100 m/s

Static Pressure 35 m/s StarCD: Pressure by 35 m/s ANSYS: Pressure by 35 m/s

Static Pressure 70 m/s StarCD: Pressure by 70 m/s ANSYS: Pressure by 70 m/s

Static Pressure 100 m/s StarCD: Pressure by 100 m/s ANSYS: Pressure by 100 m/s

Conclusion Both programs are good to solve these problems For easy geometries ANSYS/FLOTRAN should be used to get fast results For complex geometries StarCD gives more reasonable results, but it takes more time to define the boundary conditions

THE END!