adiabatic evaporation
Recently Published Documents


TOTAL DOCUMENTS

11
(FIVE YEARS 1)

H-INDEX

4
(FIVE YEARS 0)

2021 ◽  
Vol 2057 (1) ◽  
pp. 012061
Author(s):  
M S Makarov ◽  
S N Makarova

Abstract The results of numerical studies of heat and mass transfer during adiabatic evaporation of an aqueous solution of ethanol into an accelerated steam-air laminar boundary layer on a flat wetted plate are presented. The flow acceleration is realized due to the inclination of the upper channel wall, which ensures the constancy of the Kays acceleration parameter. The dependences of the evaporation intensity of the components of solutions of various compositions are obtained for the acceleration parameter 0 and 10-6 for the flow temperature from 20 to 50 °C. A significant effect of the accelerating pressure gradient on the evaporation intensity and its weak effect on the equilibrium wall temperature are shown.


2012 ◽  
Vol 21 (2) ◽  
pp. 136-143 ◽  
Author(s):  
V. V. Kuznetsov ◽  
I. A. Kozulin ◽  
O. V. Vitovsky

2007 ◽  
Vol 14 (4) ◽  
pp. 493-504 ◽  
Author(s):  
E. P. Volchkov ◽  
A. I. Leontiev ◽  
S. N. Makarova

1999 ◽  
Vol 382 ◽  
pp. 63-86 ◽  
Author(s):  
J. R. SIMÕES-MOREIRA ◽  
J. E. SHEPHERD

We have observed propagating adiabatic evaporation waves in superheated liquid dodecane, C12H26. Experiments were performed with a rapid decompression apparatus at initial temperatures of 180–300°C. Saturated dodecane in a tube was suddenly depressurized by rupturing a diaphragm. Motion pictures and still photographic images, and pressure and temperature data were obtained during the evaporation event that followed depressurization. Usually, a front or wave of evaporation started at the liquid free surface and propagated into the undisturbed regions of the metastable liquid. The evaporation wave front moved with a steady mean velocity but the front itself was unstable and fluctuating in character. At low superheats, no waves were observed until a threshold superheat was exceeded. At moderate superheats, subsonic downstream states were observed. At higher superheats, the downstream flow was choked, corresponding to a Chapman–Jouguet condition. At the most extreme superheat tested, a vapour content of over 90% was estimated from the measured data, indicating a nearly complete evaporation wave. Our results are interpreted by modelling the evaporation wave as a discontinuity, or jump, between a superheated liquid state and a two-phase liquid–vapour downstream state. Reasonable agreement is found between the model and observations; however, there is a fundamental indeterminacy that prevents the prediction of the observed wave speeds.


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.


Desalination ◽  
1970 ◽  
Vol 7 (2) ◽  
pp. 179-186 ◽  
Author(s):  
A.I. Korneichev ◽  
A.V. Izvekov ◽  
A.A. Myagkov

Sign in / Sign up

Export Citation Format

Share Document