Normal burning velocity and propagation speed of ethane–air: Pressure and temperature dependence

Fuel ◽  
2015 ◽  
Vol 147 ◽  
pp. 27-34 ◽  
Author(s):  
Maria Mitu ◽  
Domnina Razus ◽  
Venera Giurcan ◽  
Dumitru Oancea
Fuel ◽  
2019 ◽  
Vol 239 ◽  
pp. 1028-1037 ◽  
Author(s):  
Xinlu Han ◽  
Zhihua Wang ◽  
Shixing Wang ◽  
Ronald Whiddon ◽  
Yong He ◽  
...  

2002 ◽  
Vol 24 (4) ◽  
pp. 246-260 ◽  
Author(s):  
U. Techavipoo ◽  
T. Varghese ◽  
J.A. Zagzebski ◽  
T. Stiles ◽  
G. Frank

Previously reported data on the temperature dependence of propagation speed in tissues generally span only temperature ranges up to 60°C. However, with the emerging use of thermal ablative therapies, information on variation in this parameter over higher temperature ranges is needed. Measurements of the ultrasonic propagation speed and attenuation in tissue in vitro at discrete temperatures ranging from 25 to 95°C was performed for canine liver, muscle, kidney and prostate using 3 and 5 MHz center frequencies. The objective was to produce information for calibrating temperature-monitoring algorithms during ablative therapy. Resulting curves of the propagation speed vs. temperature for these tissues can be divided into three regions. In the 25–40°C range, the speed of sound increases rapidly with temperature. It increases moderately with temperature in the 40–70°C range, and it then decreases with increasing temperature from 70–95°C. Attenuation coefficient behavior with temperature is different for the various tissues. For liver, the attenuation coefficient is nearly constant with temperature. For kidney, attenuation increases approximately linearly with temperature, while for muscle and prostate tissue, curves of attenuation vs. temperature are flat in the 25–50°C range, slowly rise at medium temperatures (50–70°C), and level off at higher temperatures (70–90°C). Measurements were also conducted on a distilled degassed water sample and the results closely follow values from the literature.


Author(s):  
Luc Bauwens ◽  
C. Regis L. Bauwens ◽  
Ida Wierzba

A complete multiple-scale solution is constructed for the one-dimensional problem of an oscillating flame in a tube, ignited at a closed end, with the second end open. The flame front moves into the unburnt mixture at a constant burning velocity relative to the mixture ahead, and the heat release is constant. The solution is based upon the assumption that the propagation speed multiplied by the expansion ratio is small compared with the speed of sound. This approximate solution is compared with a numerical solution for the same physical model, assuming a propagation speed of arbitrary magnitude, and the results are close enough to confirm the validity of the approximate solution. Because ignition takes place at the closed end, the effect of thermal expansion is to push the column of fluid in the tube towards the open end. Acoustics set in motion by the impulsive start of the column of fluid play a crucial role in the oscillation. The analytical solution also captures the subsequent interaction between acoustics and the reaction front, the effect of which does not appear to be as significant as that of the impulsive start, however.


1977 ◽  
Vol 55 (7-8) ◽  
pp. 727-734
Author(s):  
K. T. Chee ◽  
F. L. Weichman

We report here on recent measurements made on our Pt–Cu2O–Cu diodes, annealed at an air pressure of 1 to 2 Torr, which we interpret as due to double injection, i.e. injection of holes from the platinum electrode and injection of electrons from the copper–Cu2O junction into the single crystal Cu2O region. The measurements discussed here include the forward I–V characteristics at various temperatures, current vs. thickness relationship at constant voltage, the effect of photo-memory on the I–V characteristics, and the discovery of a negative resistance regime at below room temperature at sufficiently high injection levels. The analysis of the temperature dependence of the current in the ohmic and the [Formula: see text] regimes, together with the effect of photomemory on the I–V characteristics enable us to identify the [Formula: see text] regime as the Ashley–Milnes regime with field dependent mobility.


Sign in / Sign up

Export Citation Format

Share Document