21
IESVi 1 QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS Arash Ash Supervisors: Dr. Djilali Dr. Oshkai Institute for Integrated Energy Systems University of Victoria ICHS2011 – September 12 th 2011

QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

  • Upload
    etenia

  • View
    46

  • Download
    1

Embed Size (px)

DESCRIPTION

QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS. Arash Ash Supervisors: Dr. Djilali Dr. Oshkai Institute for Integrated Energy Systems University of Victoria ICHS2011 – September 12 th 2011. Safety Standards. - PowerPoint PPT Presentation

Citation preview

Page 1: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 1

QUANTITATIVE IMAGING OF MULTI-COMPONENT

TURBULENT JETSArash AshSupervisors:Dr. DjilaliDr. OshkaiInstitute for Integrated Energy SystemsUniversity of VictoriaICHS2011 – September 12th 2011

Page 2: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 2

Safety Standards The integration of a hydrogen gas

storage has not been without its challenges.

Flammable characteristics of Hydrogen results in the requirement of more robust, high pressure storage systems that can meet modern safety standards.

Prior to the development of a hydrogen infrastructure, well-researched safety standards must be implemented to reduce the risk of uncontrolled leaks related to hydrogen storage.

Page 3: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 3

H2 – Fuel Cell Application

Page 4: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 4

Project Motivation and Objectives

• Perform series of well-defined experiments to generate data to guide development of engineering turbulence model suitable for rapid discharge simulations

• Objectives– experimentally characterize the effects of

buoyancy and cross-flow in a complex flow structure

– provide a quantitative database that can be used for future concentration measurements and also to validate CFD models

Page 5: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 5

Introduction• the momentum and buoyancy effects

related to the rapid, uncontrolled release of hydrogen must be studied in detail to accurately determine the resultant dispersion.

• In this study, dispersion of a buoyant, turbulent, round jet in a quiescent and moving ambient at a wide range of Froude numbers was investigated.

• This study focuses on slow leaks which might take place in small-scaled hydrogen based systems.

Page 6: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 6

Experimental Setup• Jet Apparatus:

– honeycomb settling chamber

– Sharp-edged orifice– Nozzle Diameter =

2mm• Cross-flow assembly:

– 11m/s ± 4%• Laser: Nd YAG 532 nm• CCD camera: 1376 ×

1040 pixels

Page 7: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 7

Flow ConditionsCase Q (lpm –

H2)Uoc (m/s) Fr Re r

1 64.4 318.33 ~1000 5263 11.22 43.4 248.98 ~750 4196 6.93 35.7 185.23 ~500 3121 6.14 21 94.56 ~250 1593 3.25 12 18.86 ~50 317 0.6

Helium density and viscosity are 0.166 kg/m3 and 1.97E-05 kg/ms, respectively

21jjetoc gDU=Fr

Where Fr – Froude number, Dimensionless; Uoc – Jet centerline exit velocity, m/s; g – acceleration due to gravity, m2/s; D – Jet diameter, mm; , ρ – Ambient air density, kg/m3 and ρj – Jet exit density of helium, kg/m3

Page 8: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 8

PIV - Cross Correlation

Search Area

Original IA

Particles In image B

Page 9: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 9

Results and Discussions

Page 10: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 10

Velocity Fields• Free Jet• Jet in Cross - Flow

Page 11: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 11

Jet Centerline• New coordinate

system• Jet Centerline

Page 12: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 12

Jet Centerline (Continue)

Free Jet Jet in Cross-flow

Page 13: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 13

Scaling FactorsFree JetJet in Cross-flow

Where 2/1

4/3

BMLM

first effects of buoyancy in case of Fr = 250 and 50, happens at approximately x/LM = 0.16 and 0.61 which corresponds to x/D = 43 and 32 respectively.

rD scaling

scalingDr 22

2

UU

r ocj

Page 14: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 14

Velocity DecaysFree Jet Jet in Cross-flow

Where:Uoc is mean nozzle exit velocity

Page 15: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 15

Velocity Decay (Continue)

NCF = Free jetWCF = Jet in cross-flow

1. Decay rates are faster in cross- flowing jets2. In jet far-field region decay rates drop for jets in cross-flow3. Decay rate drops in Buoyancy dominated regions

Page 16: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 16

Turbulence QuantitiesFree jet Jet in cross-flow

Where, Uc is the time-averaged velocity magnitude along the jet centerline

Page 17: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 17

Conclusion• Effects of buoyancy and cross-flow were

investigated in subsonic release of Helium,• Mean and fluctuation velocity components

were quantified using PIV,• lowering the Froude number led to slower

velocity decays due to the buoyancy-driven acceleration components in buoyancy dominated regions,

• Increasing effects of buoyancy were observed by reducing the Froude number,

• The present data can serve to validate computational models derived for investigating hydrogen safety scenarios.

Page 18: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 18

Thank you

Questions?

Page 19: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 19

Appendix• Initial Condition – Sharp-edged

Orifice

Page 20: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 20

Velocity ProfilesFree Jet Jet in cross-flow

Page 21: QUANTITATIVE IMAGING OF MULTI-COMPONENT TURBULENT JETS

IESVic 21

Seeding - Stokes number• Seeding particles must:

1. Match fluid properties2. Neutrally buoyant3. Short response time to flow motion4. ReflectivityParticle Flow is dominated by Stokes drag:

For St>>1, particles will continue in a straight line regardless of fluid streamline but for St<<1, particles will follow the fluid streamlines closely.

2

18U d CUStL L