Accidental Release of Pressurized Gas
When gas stored under pressure in a closed vessel is discharged to the atmosphere through a hole or other opening, the gas velocity through that opening may be choked (i.e., it has attained a maximum) or it may be non-choked.
Choked velocity, also referred to as sonic velocity, occurs when the ratio of the absolute source pressure to the absolute downstream pressure is equal to or greater than k÷(k - 1 ), where k is the specific heat ratio of the discharged gas (sometimes called the isentropic expansion factor and sometimes denoted as ).
For many gases, k ranges from about 1.09 to about 1.41, and therefore k÷(k - 1 ) ranges from 1.7 to about 1.9, which means that choked velocity usually occurs when the absolute source vessel pressure is at least 1.7 to 1.9 times as high as the absolute downstream ambient atmospheric pressure.
When the gas velocity is choked, the equation for the mass flow rate in SI metric units is:
or this equivalent form:
For the above equations, it is important to note that although the gas velocity reaches a maximum and becomes choked, the mass flow rate is not choked. The mass flow rate can still be increased if the source pressure is increased.
Whenever the ratio of the absolute source pressure to the absolute downstream ambient pressure is less than k ÷ ( k - 1 ), then the gas velocity is non-choked (i.e., sub-sonic) and the equation for mass flow rate is:
or this equivalent form:
| where: | |
| Q | = mass flow rate, kg/s |
|---|---|
| C | = discharge coefficient, dimensionless (usually about 0.72) |
| A | = discharge hole area, m² |
| k | = cp/cv of the gas |
| cp | = specific heat of the gas at constant pressure |
| cv | = specific heat of the gas at constant volume |
| = real gas density at P and T, kg/m³ | |
| P | = absolute upstream pressure, Pa |
| PA | = absolute ambient or downstream pressure, Pa |
| M | = the gas molecular mass, kg/kmol (also known as the molecular weight) |
| R | = the Universal Gas Law Constant = 8314.5 Pa·m³/(kmol·K) |
| T | = absolute upstream gas temperature, K |
| Z | = the gas compressibility factor at P and T, dimensionless |
The above equations calculate the initial instantaneous mass flow rate for the pressure and temperature existing in the source vessel when a release first occurs. The initial instantaneous flow rate from a leak in a pressurized gas system or vessel is much higher than the average flow rate during the overall release period because the pressure and flow rate decrease with time as the system or vessel empties. Calculating the flow rate versus time since the initiation of the leak is much more complicated, but more accurate. Two equivalent methods for performing such calculations are presented and compared at www.air-dispersion.com/feature2.html.
The technical literature can be very confusing because many authors fail to explain whether they are using the universal gas law constant R which applies to any ideal gas or whether they are using the gas law constant Rs which only applies to a specific individual gas. The relationship between the two constants is Rs = R/M.
Notes:
- The above equations are for a real gas.
- For an ideal gas, Z = 1 and ρ is the ideal gas density.
- 1 kilomole (kmol) = 1000 moles = 1000 gram-moles = kilogram-mole.
Read more about this topic: Accidental Release Source Terms
Famous quotes containing the words accidental, release and/or gas:
“Of your philosophy you make no use
If you give place to accidental evils.”
—William Shakespeare (1564–1616)
“The near touch of death may be a release into life; if only it will break the egoistic will, and release that other flow.”
—D.H. (David Herbert)
“Papa died in the gas chamber,
slipping blue as an undressed minnow,
gulping in the shower to wash the Jew off him.”
—Anne Sexton (1928–1974)