On the transcritical mixing of fuels at diesel engine conditions

[Display omitted] •We observed microscopic fuel droplets transitioning to supercritical fluid.•A conceptual model and criteria for the transition to diffusive mixing are proposed.•Surface tension and primary atomization remain important features of diesel mixing.•Transition to diffusive mixing regim...

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Published in:Fuel (Guildford) Vol. 208; pp. 535 - 548
Main Authors: Crua, Cyril, Manin, Julien, Pickett, Lyle M.
Format: Journal Article
Language:English
Published: Kidlington Elsevier Ltd 15-11-2017
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Abstract [Display omitted] •We observed microscopic fuel droplets transitioning to supercritical fluid.•A conceptual model and criteria for the transition to diffusive mixing are proposed.•Surface tension and primary atomization remain important features of diesel mixing.•Transition to diffusive mixing regime is driven by gas pressure and temperature.•Timescales and fluid morphology for diffusive mixing are driven by fuel properties. Whilst the physics of both classical evaporation and supercritical fluid mixing are reasonably well characterized and understood in isolation, little is known about the transition from one to the other in the context of liquid fuel systems. The lack of experimental data for microscopic droplets at realistic operating conditions impedes the development of phenomenological and numerical models. To address this issue we performed systematic measurements using high-speed long-distance microscopy, for three single-component fuels (n-heptane, n-dodecane, n-hexadecane), into gas at elevated temperatures (700–1200K) and pressures (2–11MPa). We describe these high-speed visualizations and the time evolution of the transition from liquid droplet to fuel vapour at the microscopic level. The measurements show that the classical atomization and vaporisation processes do shift to one where surface tension forces diminish with increasing pressure and temperature, but the transition to diffusive mixing does not occur instantaneously when the fuel enters the chamber. Rather, subcritical liquid structures exhibit surface tension in the near-nozzle region and then, after time surrounded by the hot ambient gas and fuel vapour, undergo a transition to a dense miscible fluid. Although there was clear evidence of surface tension and primary atomization for n-dodecane and n-hexadecane for a period of time at all the above conditions, n-heptane appeared to produce a supercritical fluid from the nozzle outlet when injected at the most elevated conditions (1200K, 10MPa). This demonstrates that the time taken by a droplet to transition to diffusive mixing depends on the pressure and temperature of the gas surrounding the droplet as well as the fuel properties. We summarise our observations into a phenomenological model which describes the morphological evolution and transition of microscopic droplets from classical evaporation through a transitional mixing regime and towards diffusive mixing, as a function of operating conditions. We provide criteria for these regime transitions as reduced pressure–temperature correlations, revealing the conditions where transcritical mixing is important to diesel fuel spray mixing.
AbstractList [Display omitted] •We observed microscopic fuel droplets transitioning to supercritical fluid.•A conceptual model and criteria for the transition to diffusive mixing are proposed.•Surface tension and primary atomization remain important features of diesel mixing.•Transition to diffusive mixing regime is driven by gas pressure and temperature.•Timescales and fluid morphology for diffusive mixing are driven by fuel properties. Whilst the physics of both classical evaporation and supercritical fluid mixing are reasonably well characterized and understood in isolation, little is known about the transition from one to the other in the context of liquid fuel systems. The lack of experimental data for microscopic droplets at realistic operating conditions impedes the development of phenomenological and numerical models. To address this issue we performed systematic measurements using high-speed long-distance microscopy, for three single-component fuels (n-heptane, n-dodecane, n-hexadecane), into gas at elevated temperatures (700–1200K) and pressures (2–11MPa). We describe these high-speed visualizations and the time evolution of the transition from liquid droplet to fuel vapour at the microscopic level. The measurements show that the classical atomization and vaporisation processes do shift to one where surface tension forces diminish with increasing pressure and temperature, but the transition to diffusive mixing does not occur instantaneously when the fuel enters the chamber. Rather, subcritical liquid structures exhibit surface tension in the near-nozzle region and then, after time surrounded by the hot ambient gas and fuel vapour, undergo a transition to a dense miscible fluid. Although there was clear evidence of surface tension and primary atomization for n-dodecane and n-hexadecane for a period of time at all the above conditions, n-heptane appeared to produce a supercritical fluid from the nozzle outlet when injected at the most elevated conditions (1200K, 10MPa). This demonstrates that the time taken by a droplet to transition to diffusive mixing depends on the pressure and temperature of the gas surrounding the droplet as well as the fuel properties. We summarise our observations into a phenomenological model which describes the morphological evolution and transition of microscopic droplets from classical evaporation through a transitional mixing regime and towards diffusive mixing, as a function of operating conditions. We provide criteria for these regime transitions as reduced pressure–temperature correlations, revealing the conditions where transcritical mixing is important to diesel fuel spray mixing.
Whilst the physics of both classical evaporation and supercritical fluid mixing are reasonably well characterized and understood in isolation, little is known about the transition from one to the other in the context of liquid fuel systems. The lack of experimental data for microscopic droplets at realistic operating conditions impedes the development of phenomenological and numerical models. To address this issue we performed systematic measurements using high-speed long-distance microscopy, for three single-component fuels (n-heptane, n-dodecane, n-hexadecane), into gas at elevated temperatures (700-1200 K) and pressures (2-11 MPa). We describe these high-speed visualizations and the time evolution of the transition from liquid droplet to fuel vapour at the microscopic level. The measurements show that the classical atomization and vaporisation processes do shift to one where surface tension forces diminish with increasing pressure and temperature, but the transition to diffusive mixing does not occur instantaneously when the fuel enters the chamber. Rather, subcritical liquid structures exhibit surface tension in the near-nozzle region and then, after time surrounded by the hot ambient gas and fuel vapour, undergo a transition to a dense miscible fluid. Although there was clear evidence of surface tension and primary atomization for n-dodecane and n-hexadecane for a period of time at all the above conditions, n-heptane appeared to produce a supercritical fluid from the nozzle outlet when injected at the most elevated conditions (1200K, 10 MPa). This demonstrates that the time taken by a droplet to transition to diffusive mixing depends on the pressure and temperature of the gas surrounding the droplet as well as the fuel properties. We summarise our observations into a phenomenological model which describes the morphological evolution and transition of microscopic droplets from classical evaporation through a transitional mixing regime and towards diffusive mixing, as a function of operating conditions. We provide criteria for these regime transitions as reduced pressure-temperature correlations, revealing the conditions where transcritical mixing is important to diesel fuel spray mixing.
Whilst the physics of both classical evaporation and supercritical fluid mixing are reasonably well characterized and understood in isolation, little is known about the transition from one to the other in the context of liquid fuel systems. The lack of experimental data for microscopic droplets at realistic operating conditions impedes the development of phenomenological and numerical models. To address this issue we performed systematic measurements using high-speed long-distance microscopy, for three single-component fuels (n-heptane, n-dodecane, n-hexadecane), into gas at elevated temperatures (700–1200 K) and pressures (2–11 MPa). We describe these high-speed visualizations and the time evolution of the transition from liquid droplet to fuel vapour at the microscopic level. The measurements show that the classical atomization and vaporisation processes do shift to one where surface tension forces diminish with increasing pressure and temperature, but the transition to diffusive mixing does not occur instantaneously when the fuel enters the chamber. Rather, subcritical liquid structures exhibit surface tension in the near-nozzle region and then, after time surrounded by the hot ambient gas and fuel vapour, undergo a transition to a dense miscible fluid. Although there was clear evidence of surface tension and primary atomization for n-dodecane and n-hexadecane for a period of time at all the above conditions, n-heptane appeared to produce a supercritical fluid from the nozzle outlet when injected at the most elevated conditions (1200 K, 10 MPa). This demonstrates that the time taken by a droplet to transition to diffusive mixing depends on the pressure and temperature of the gas surrounding the droplet as well as the fuel properties. We summarise our observations into a phenomenological model which describes the morphological evolution and transition of microscopic droplets from classical evaporation through a transitional mixing regime and towards diffusive mixing, as a function of operating conditions. We provide criteria for these regime transitions as reduced pressure–temperature correlations, revealing the conditions where transcritical mixing is important to diesel fuel spray mixing.
Author Manin, Julien
Crua, Cyril
Pickett, Lyle M.
Author_xml – sequence: 1
  givenname: Cyril
  orcidid: 0000-0003-4992-9147
  surname: Crua
  fullname: Crua, Cyril
  email: c.crua@brighton.ac.uk
  organization: Advanced Engineering Centre, University of Brighton, Brighton BN2 4GJ, United Kingdom
– sequence: 2
  givenname: Julien
  surname: Manin
  fullname: Manin, Julien
  organization: Sandia National Laboratories, 7011 East Avenue, 94550 Livermore, CA, United States
– sequence: 3
  givenname: Lyle M.
  surname: Pickett
  fullname: Pickett, Lyle M.
  organization: Sandia National Laboratories, 7011 East Avenue, 94550 Livermore, CA, United States
BackLink https://www.osti.gov/servlets/purl/1473932$$D View this record in Osti.gov
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Keywords Mixing
Immiscible-miscible
Breakup
State transition
Atomization
Transcritical
Language English
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SSID ssj0007854
Score 2.6062772
Snippet [Display omitted] •We observed microscopic fuel droplets transitioning to supercritical fluid.•A conceptual model and criteria for the transition to diffusive...
Whilst the physics of both classical evaporation and supercritical fluid mixing are reasonably well characterized and understood in isolation, little is known...
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SubjectTerms 02 PETROLEUM
Atomization
Atomizing
Breakup
Diesel
Diesel engines
Dodecane
Droplets
Evaporation
Evolution
Fuel sprays
Fuel systems
Fuels
Heptanes
Hexadecane
High speed
Immiscible-miscible
Liquid fuels
Mathematical models
Microscopy
Mixing
Physics
Pressure
Product mixes
State transition
Studies
Surface tension
Temperature effects
Tension
Transcritical
Transitions
Vaporization
Title On the transcritical mixing of fuels at diesel engine conditions
URI https://dx.doi.org/10.1016/j.fuel.2017.06.091
https://www.proquest.com/docview/1952479380
https://www.osti.gov/servlets/purl/1473932
Volume 208
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