Supersonic wind tunnel
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A supersonic wind tunnel is a wind tunnel that produces supersonic speeds (1.2<M<5) The Mach number and flow are determined by the nozzle geometry. The Reynolds number is varied changing the density level (pressure in the settling chamber). Therefore a high pressure ratio is required (for a supersonic regime at M=4, this ratio is of the order of 10). Apart from that, condensation or liquefaction can occur. This means that a supersonic wind tunnel needs a drying or a pre-heating facility. A supersonic wind tunnel has a large power demand leading to only intermittent operation.
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[edit] Restrictions for supersonic tunnel operation
[edit] Minimum required pressure ratio
Optimistic estimate: Pressure ratio the total pressure ratio over normal shock at M in test section:
Examples:
[edit] Temperature effects: condensation
Temperature in the test section:
with Tt = 330K: Tm = 70K at Mm = 4
The Mach range is limited by reservoir temperature
[edit] Power requirements
The power required to run a supersonic windtunnel is enormous, of the order of 50 MW per square meter of test section. For this reason most wind tunnels operate intermittently using energy stored in high-pressure tanks. These windtunnels are also called intermittent supersonic blowdown wind tunnels (of which a schematic preview is given below). Another way of achieving the huge power output is with the use of a vacuum storage tank. These tunnels are called indraft supersonic wind tunnels. Other problems operating a supersonic wind tunnel include:
- enough supply of dry air
- wall interference effects
- fast instruments needed for intermittent measurements
Tunnels such as a Ludwieg tube have short test times (usually less than one second), relatively high Reynolds number, and low power requirements.
[edit] Further reading
- Pope, A.; Goin, K. (1978). High-speed Wind Tunnel Testing. Krieger. ISBN 088275727X.
[edit] See also
- Wind tunnel
- Low speed wind tunnel
- High speed wind tunnel
- Hypersonic wind tunnel
- Ludwieg tube
- Shock tube