...since it has been assumed that u = 0 at T = 0, then h = 0 at T = 0). 2.8.6. Ratio of Specific Heats The ratio of specific heat at constant pressure to the specific heat at constant volume is given the symbol y (gamma). ie, y = ^ ...(2.25) cv Since cp = cu + R, it is clear that cp must be...

...since it has been assumed that и = 0 at Т = 0, then h = 0 at Т = 0). 2.8.6. Ratio of Specific Heats The ratio of specific heat at constant pressure to the specific heat at constant volume is given the symbol у (gamma). ie, y = — ...(2.25) с„ Since cp = cv + R, it is clear that cp...

...since it has been assumed that u = 0 at T = 0, then h = 0 at T = 0). 3.8.6. Ratio of Specific Heats The ratio of specific heat at constant pressure to the specific heat at constant volume is given the symbol y (gamma). ie, y = — ...(3.25) cv Since cp = cv + R, it is clear that cp must...

...(6.53) The velocity of sound in a gas is Vsound = — ' ( 6 -5 4 ) \mnj where y is the ratio of the specific heat at constant pressure to the specific heat at constant volume thus: y^. (6.55) Lv The second dimensionless parameter is Knudsen's number, Kn, and is the ratio of...

...coordinate, / the time, 11 the radial velocity of gas, p the density, p the pressure and y the ratio of the specific heat at constant pressure to the specific heat at constant volume. At t = 0 the explosive instantaneously releases an energy EQ of dimensionality [£"Q] = J and a spherical...

...the process is said to be adiabatic. According to this process, pV* = Constant where k = Ratio of the specific heat at constant pressure to the specific heat at constant volume C. = — = 1 .4 for air. Q The above relation is also written as -^- = Constant. ...(12.4) P In the...