1
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 Energy/Vehicle Technology 0% 25% 50% 75% 100% 0 5 10 15 20 25 30 35 40 45 50 55 60 65 70 Probability Feature size [μm ] 2M Pa 7M Pa Ultrafast X-ray Study of Swirling Hollow-Cone Sprays in the Near-Field Advanced Photon Source, Argonne National Laboratory, US Objectives Interpretation of near-field flow development of swirling hollow-cone sprays Physical insight on various types of breakups and atomization process P inj = 2 MPa, Ambient Gas = N 2 , Fuel = Gasoline Calibration Fluid (Viscor 16BR) Ultrafast X-ray Phase-Enhanced Imaging Temporal Resolution : 150ps High Energy X-ray : 9.62keV Spatial Resolution < 1mm Temporal Spray Development Outward-Opening Swirl Injector Opening -‘Skirts’ Closing – ‘Streaks from Weakened Swirl’ X-ray Tomography from APS, ANL Opening -‘Instability Waves’ Steady – ‘Turbulent Flow from High Swirl’ Nozzle Structure (taken using x-ray phase-enhanced imaging) 1mm P inj = 2 MPa Steady-state White-Light 11 ns Exposure W. Cai et al., Appl. Phys. Lett. 83, 1671 (2003) 1m m 1-5% Transmission at 1 mm location Visible Light Image * Setup in XOR 7ID-B in APS, ANL A B C D A. Opening – ‘Skirts’ 500 m P inj = 5 MPa, 80 s ASOI P inj = 2 MPa Droplet Sizes : 41 ~ 67 m Low velocity laminar-like flow before swirl motion Dictated by transient pressure and velocity during needle opening Skirt Ligaments Droplets High injection pressures form thin and long ligaments, and smaller droplets P inj = 7 MPa Droplet Sizes : 35 ~ 50 m B. Opening – ‘Instability Waves’ P inj = 2 MPa 150 s ASOI P inj = 7 MPa 120 s ASOI Instability waves, an indicator of laminar to turbulence transition, appear on the sheet. The wavelengths are dependent to Re. Wavelength : 40 m Wavelength : 26 m C. Steady – ‘Turbulent Flow from Strong Swirl’ D. Closing – ‘Streaks from Weakened Swirl’ 0 10 20 30 40 50 0 2000 4000 6000 W avelength [ m] Re Re Dependency Analyzed from non-swirl hollow spray Concluding Remarks Hollow-cone swirl spray showed four representative stages of flow development with time: (1) skirts and (2) instability waves during opening, (3) turbulent flow from strong-swirl at steady-state and (4) streaks from weakened swirl during closing. Instability wavelengths, ligament and droplet sizes decrease and number of streaks increases with increase in injection pressure. P inj = 2 MPa 500 m 500 m 1 mm P inj = 2 MPa, 1.0 ms P inj = 5 MPa, 1.19 ms P inj = 7 MPa, 1.19 ms 2 MPa 5 MPa 7 MPa 0 10 20 30 40 N um berofStreaks Number of Streaks at Dotted Boxes P inj = 7 MPa Probability of Feature Size Turbulent flow from nozzle exit from strong swirl flow Ligaments, droplets and bubbles at downstream Decrease in feature size at higher injection pressure Increase in feature density at higher injection pressure Streaks with less turbulent flow from weakened swirl Increase in number of streaks at higher injection pre Streaks are from hydrodynamic instability 500 m

Ultrafast X-ray Study of Swirling Hollow-Cone Sprays in the Near-Field

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Ultrafast X-ray Study of Swirling Hollow-Cone Sprays in the Near-Field. Advanced Photon Source, Argonne National Laboratory, US. Objectives. Ultrafast X-ray Phase-Enhanced Imaging. High Energy X-ray : 9.62keV. - PowerPoint PPT Presentation

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Page 1: Ultrafast X-ray Study of Swirling Hollow-Cone Sprays in the Near-Field

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 Energy/Vehicle Technology

0%

25%

50%

75%

100%

0 5 10 15 20 25 30 35 40 45 50 55 60 65 70

Prob

abili

ty

Feature size [μm]

2MPa

7MPa

Ultrafast X-ray Study of Swirling Hollow-Cone Spraysin the Near-Field

Advanced Photon Source, Argonne National Laboratory, US

Objectives Interpretation of near-field flow development of swirling hollow-cone sprays Physical insight on various types of breakups and atomization process

Pinj = 2 MPa, Ambient Gas = N2,Fuel = Gasoline Calibration Fluid (Viscor 16BR)

Ultrafast X-ray Phase-Enhanced Imaging

Temporal Resolution : 150psHigh Energy X-ray : 9.62keV

Spatial Resolution < 1mm

Temporal Spray Development

Outward-Opening Swirl Injector

Opening -‘Skirts’

Closing – ‘Streaks from Weakened Swirl’

X-ray Tomography from APS, ANLOpening -‘Instability Waves’ Steady – ‘Turbulent Flow from High Swirl’

Nozzle Structure(taken using x-ray phase-enhanced imaging)

1mm

Pinj = 2 MPaSteady-stateWhite-Light

11 ns Exposure

W. Cai et al., Appl. Phys. Lett. 83, 1671 (2003)

1mm 1-5% Transmissionat 1 mm location

Visible Light Image

* Setup in XOR 7ID-B in APS, ANL

A B C

D

A. Opening – ‘Skirts’

500 m Pinj = 5 MPa, 80 s ASOI

Pinj = 2 MPa

Droplet Sizes: 41 ~ 67 m

Low velocity laminar-like flow before swirl motion Dictated by transient pressure and velocity during needle opening

Skirt Ligaments Droplets High injection pressures form thin and long ligaments, and smaller droplets

Pinj = 7 MPa

Droplet Sizes: 35 ~ 50 m

B. Opening – ‘Instability Waves’

Pinj = 2 MPa150 s ASOI

Pinj = 7 MPa120 s ASOI

Instability waves, an indicator of laminar to turbulence transition, appear on the sheet. The wavelengths are dependent to Re.

Wavelength: 40 m

Wavelength : 26 m

C. Steady – ‘Turbulent Flow from Strong Swirl’ D. Closing – ‘Streaks from Weakened Swirl’

0

10

20

30

40

50

0 2000 4000 6000

Wav

elen

gth

[m

]

Re

Re DependencyAnalyzed from

non-swirl hollow spray

Concluding Remarks Hollow-cone swirl spray showed four representative stages of flow development with time: (1) skirts and (2) instability waves during opening, (3) turbulent flow

from strong-swirl at steady-state and (4) streaks from weakened swirl during closing. Instability wavelengths, ligament and droplet sizes decrease and number of streaks increases with increase in injection pressure.

Pinj = 2 MPa

500 m 500 m

1 mm

Pinj = 2 MPa, 1.0 ms

Pinj = 5 MPa, 1.19 ms

Pinj = 7 MPa, 1.19 ms 2 MPa 5 MPa 7 MPa0

10

20

30

40

2 5 7

Num

ber o

f Stre

aks Number of Streaks at Dotted Boxes

Pinj = 7 MPa

Probability of Feature Size

Turbulent flow from nozzle exit from strong swirl flow Ligaments, droplets and bubbles at downstream Decrease in feature size at higher injection pressure Increase in feature density at higher injection pressure

Streaks with less turbulent flow from weakened swirl Increase in number of streaks at higher injection pressure Streaks are from hydrodynamic instability

500 m