spacehugo":1mjlxa8f said:
if you fill a ballon with air , it will have a certain volume and a tube filled with air will also have volume in addition to length. open this under water and you will see bubbles rising towards the surface, also in this ballon or tube with air, sound can travel at 360 m/s. the same procedure with the vacuum tube will not make any bubbles rising towards the surface and further more, sound can not travel thru vacuum and sound travel in a similar way (or the same way) as pressure do. so if you have 360 m of air between you and the source of sound, the sound use 1 s. to reach you, but if there is 1mm or 10 km of vacuum between you and the source of sound, the sound will never reach you.
You have managed to start with a poorly posed question and then scramble it into compeete incoherence.
Basically this is, or ought to be, a standard compartment venting problem. Here you start with one volume, which happens to be evacuated, separated from another volume that contains some volume (unspecified) of some gas (unspecified) at some pressure (apparently unspecified though mention was made later of 14.67 psi). Then at time 0 a diaphram separting the two compartments if broken (or a valve is opened) and gas from the first compartment flows into the second compartment.
The problem is that you asked WHEN the first pressure would be seen at the far end of the tube. That is fairly difficult to answer since you have not specified criteria for what you mean by "first pressure". If you mean when might the first molecule hit the far end, then that could be pretty quick, since the question one of what the HIGHEST speed might be of the molecules that make up the gas at the specified initial temperatue. Even then you will have to be more precise, since the distribution permits extremely high, but low probability speeds.
On the other hand you might be considering a classical continuum mechanics model of a compressible fluid, which would provide a solution, somewhat complex, in terms of the Navier-Stokes equation. That should provide flow vectors, pressure, temperatureand density throughout the volumes as a function of time. This will be complicated by the expansion of the gas into the vacuum which changes the temperature, which affects the speed of sound. There is additinal complication because when you vent into a vacuum you will at times find that the flow is supersonic.
You might also be asking what speed gas can reach when it is expanded isentropically from a given pressure to zero pressure. This is precisely the quantity that is used as a measure of the efficiency of rocket propellants -- vacuum specific impulse. It is dependent in detail on the thermodynamics properties of the gas but basically varies like the square root of temperature divided by molecular weight.
Finally, this has nothing whatever to do with the "speed of vacuum" which as a term makes no sense at all. The vacuum is not moving.