Numerical simulation of the growth and interaction of vapour bubbles in superheated liquid jets

2019 ◽  
Vol 121 ◽  
pp. 103112 ◽  
Author(s):  
D. Dietzel ◽  
T. Hitz ◽  
C.-D. Munz ◽  
A. Kronenburg
2004 ◽  
Vol 35 (1-2) ◽  
pp. 59-66
Author(s):  
A. V. Reshetnikov ◽  
V. P. Skripov ◽  
V. P. Koverda ◽  
V. N. Skokov ◽  
N. A. Mazheiko ◽  
...  

1994 ◽  
Vol 37 (2) ◽  
pp. 313-321 ◽  
Author(s):  
Erasmus Mhina Peter ◽  
Akira Takimoto ◽  
Yujiro Hayashi

2018 ◽  
Vol 859 ◽  
pp. 819-838 ◽  
Author(s):  
Josef Hasslberger ◽  
Sebastian Ketterl ◽  
Markus Klein ◽  
Nilanjan Chakraborty

The local flow topology analysis of the primary atomization of liquid jets has been conducted using the invariants of the velocity-gradient tensor. All possible small-scale flow structures are categorized into two focal and two nodal topologies for incompressible flows in both liquid and gaseous phases. The underlying direct numerical simulation database was generated by the one-fluid formulation of the two-phase flow governing equations including a high-fidelity volume-of-fluid method for accurate interface propagation. The ratio of liquid-to-gas fluid properties corresponds to a diesel jet exhausting into air. Variation of the inflow-based Reynolds number as well as Weber number showed that both these non-dimensional numbers play a pivotal role in determining the nature of the jet break-up, but the flow topology behaviour appears to be dominated by the Reynolds number. Furthermore, the flow dynamics in the gaseous phase is generally less homogeneous than in the liquid phase because some flow regions resemble a laminar-to-turbulent transition state rather than fully developed turbulence. Two theoretical models are proposed to estimate the topology volume fractions and to describe the size distribution of the flow structures, respectively. In the latter case, a simple power law seems to be a reasonable approximation of the measured topology spectrum. According to that observation, only the integral turbulent length scale would be required as an input for the a priori prediction of the topology size spectrum.


2008 ◽  
Vol 2008.2 (0) ◽  
pp. 291-292
Author(s):  
Koichi Tsujimoto ◽  
Tomoki Wada ◽  
Makoto Nagaoka ◽  
Toshihiko Shakouchi ◽  
Toshitake Ando

2007 ◽  
Vol 2007.20 (0) ◽  
pp. 575-576
Author(s):  
Koichi TSUJIMOTO ◽  
Makoto NAGAOKA ◽  
Toshihiko SHAKOUCHI ◽  
Toshitake ANDO

1992 ◽  
Vol 236 ◽  
pp. 43-59 ◽  
Author(s):  
Th. Kurschat ◽  
H. Chaves ◽  
G. E. A. Meier

A nozzle expansion into a vacuum chamber was used to investigate the evaporation of highly superheated liquid jets. The large molar specific heat of fluids with high molecular complexity — in this case C6F14 — is responsible for the new phenomena reported here. A model was developed to describe the basic physical effects. A cubic equation of state was used to describe the thermodynamic properties of the fluid. The evaporation was modelled as a sonic deflagration followed by an axisymmetric supersonic expansion. As in the case of hypersonic gas jets the final state is reached by a normal shock. For sufficiently high temperatures and expansion ratios a complete adiabatic evaporation of the liquid was found. At even higher temperatures the liquid evaporates completely within a rarefaction discontinuity. The predictions of the model are in good agreement with the experimental results.


Author(s):  
Ehsan Farvardin ◽  
Ali Dolatabadi

Numerical simulation of liquid jets ejecting from a set of elliptical jets with different aspect ratios between 1 (circular) to 3.85 is performed for several Weber numbers ranging 15 to 330. The axis-switching phenomenon and breakup length of the jets are characterized by means of a Volume of Fluid (VOF) method together with a dynamic mesh refinement model. This three dimensional simulation is compared with a recent experimental work and the results agree well. It is concluded that at Weber numbers less than 100, the breakup length of the liquid jet increases, reaches a peak and then decreases suddenly.


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