Gas number density varied between 102 and 1010 cm - 3, though the total amount of gas in the simulation stayed constant at 105 M ☉.
Not exact matches
Hydrogen is an excellent fuel which, due to its high energetic
density and zero greenhouse
gas emission, is essential in a great
number of industrial processes.
The conditions for mechanical equilibrium doesn't depend on whether the
gases are ideal or not, although for an ideal
gas, the
density depends on the temperature so that there are an infinite
number of ways one can stack up the
gas with a thermal gradient that are all still in mechanical equilibrium.
The result of our theory is that the final distribution of any
number of kinds of
gas in a vertical vessel is such that the
density of each
gas at a given height is the same as if all the other
gases had been removed, leaving it alone in the vessel.
OTOH, if by this you mean that both
gases will have equilibrium
densities and partial pressures that more or less exponentially decay, with distinct exponential constants so that the static equilibrium mixture will not end up being perfectly homogeneous over very large vertical distances, especially if one molecule is physically much larger than and more massive than the other, I don't have a quarrel with that (and neither does Dalton), although I would want to work out the
numbers.
The molar
density of a
gas tells you the average
number of molecules per cubic metre of the
gas.
According to the ideal
gas law PV = nRT, additional warmth (increased T) reduces
density when P is held constant, namely by increasing V while leaving n (the
number of moles and hence the mass) unchanged.
It comprises a
number for the amount of energy required for the necessary work done (in Joules) to lift 1 kg of mass in a
gas to a height at which it can become 1 degree kelvin cooler due to the decrease in
density with height.