(2) zdas04 (Mechanical) |
6 Apr 12 13:09 |
It really depends on the length and size of the tailpipe. If it is bigger than the orifice (which it certainly is) and shorter than about 10D then you can safely assume that it is "infinitely wide and infinitely short" which means that the choked flow exiting the orifice stays at near sonic velocity until it has exited the tailpipe.
The important fact is that friction loss in the tailpipe does not push up the outlet pressure at the orifice to more than the critical pressure for choked flow.
At about 10D the infinite assumption starts getting a bit flaky and you have to do real work. Above 0.6 Mach, the flow is compressible and cannot use any of the incompressible equations. The simplifying assumption that I use is that the transonic region is 10D and that I'm below 0.6 Mach after that point. This is not assured, but I've found it to be a reasonable approximation. At that point I can look at the pressure at the exhaust (atmospheric pressure), the mass flow rate through the orifice, and use the Isothermal Gas Flow Equation to calculate the upstream pressure (i.e. the pressure at 10D downstream of the PSV). If that pressure is "well under" the critical pressure for choked flow at the orifice then I call it good. If not, then the tail pipe is too long and/or too small.
"Well under" is more than a bit mushy, but for 6 ft tail pipes I usually find that this exercise results in a pressure at 10D that is less than half of critical, sometimes a lot less. If I'm going to a flare, then I often find that I need more care. In those cases I use <95% of critical pressure is acceptable and don't feel very good about it.
I've always found that in these gray areas it is crucial that you document your assumptions and calculations. I've been audited several times and this calculation has withstood serious scrutiny. The key seems to be that you've applied an objective criteria consistently. I find the "guidance" in the standards to be so full of exceptions that it isn't much help.
David |
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