Turbine Engine Surge Stall
Turbine Engine Surge Stall
(OP)
Can someone please provide a basic explanation of a turbine engine surge and stall. The specific application is for Rotorcraft (Turbo-Shaft Engines. What are the specific differences between and surge and stall? What causes them? How do you prevent them? Does this happen only in the compressor area of the engine? Thanks For Your Help





RE: Turbine Engine Surge Stall
An axial compressor generates a flow and pressure increase down the engine. It achieves this through the flow of air over successive rows of rotor blades and stator vanes. Both the blades and the vanes are similar to aircraft wing airfoils. If the flow separates over the airfoils badly the airfoil can be said to stall.
Once stalled, the airfoil looses the ability to pump gas down the engine. There is then nothing to prevent the high pressure gas at the rear of the engine from flowing forwards to the lower pressure stages. This reverse flow is called a surge. It lasts for 10-50 milliseconds.
What causes stalls? Strong cross-flows into the engine inlet during 'unusual' aircraft manouvres, bird injestion, maybe a few others.
The only surge protection system I have seen was a series of blow-out holes in the casing controled by a rotating ring - but that was on a very old engine.
Hope this helps.
gwolf.
RE: Turbine Engine Surge Stall
RE: Turbine Engine Surge Stall
Some devices to prevent surge is to allow the air flow go downstream trought the compressor. This systems are known like bleed air valves or air bleed port. They light the pressure in order to gain air momentum of the air mass flow downstream.
Fran Ale
RE: Turbine Engine Surge Stall
http://en.wikipedia.org/wiki/Compressor_map
Compressor surge is the reason that a gas turbine takes time to get from idle to maximum power - anything up to 15 seconds. Certification regs say that on approach to landing the engine speed needs to be higher, so that the pilot can get maximum power in 5 secs for a go-around.
RE: Turbine Engine Surge Stall
This is WAY outta my league, but, isn't that why they come in at like 85-90% power (albeit in a high drag configuration)? I know they take time to spool up and the extra drag from flap/slat deployment also adds lift, but it seems like the engine is closer to max power this way. Basically in it's "powerband" as would be with an internal combustion engine as in a car. Been thru a few go-arounds in my life as a passenger-unnerving I find them!
Scott
In a hundred years, it isn't going to matter anyway.
RE: Turbine Engine Surge Stall
It's not in a power band as such though. Gas turbines take time to run up from idle to max power. You can't just whack the throttles wide open like on a car (the pilot thinks he can, the fuel control unit thinks otherwise), otherwise the engine surges. Clever control units let the pilot do (more or less) what he likes with the throttle.
RE: Turbine Engine Surge Stall
A note regading this phenomena... Stall/stagnation over-pressure loading is brutal on air-inlets. If I remember correctly the peek over-pressure design requirement [limit load?] for the F-15 engine air inlet duct [F-100-100 engine] and the associated mechanical elements [such as the variable inlet componnents] was roughly 60-PSIG [4.1 Bar]. This made for a VERY stiff/strong/heavy duct design... but I have seen fasteners loosen-up and/or crack after these events. I believe that there was also a perforated skin section just forward of the engine face-plane to bleed-off pressure disturbances [spikes] due to various factors including stall/stag and reflected shock-waves from the blades.
Regards, Wil Taylor
RE: Turbine Engine Surge Stall
SURGE
In the figure you can see the map curve for a given number of rpm for a compressor.
If you consider the pressure ratio of project the compressor can work in 2 point of the curve,
the one on the right is stable (B)
the one on the left is unstable(A)
If your compressor is working in B and an inconvenience make the flow of mass increase the pressure ratio go down,
this means that the pressure of the air flow, going out the compressor, is lower than p2=const.
So the flow decelerates because there is gradient of pressure opposing
and the flow of mass decrease and consequently the compressor return to work in B.
In a similar way if the flow of mass decrease a positive gradient of pressure accelerates the air flow and the compressor return to work in B.
If we are in A every little variation of the flow of mass is amplified, so a compressor mustn't work on the left of the surge line.
If a compressor work on the left of the surge line the air is pumped instead of being aspirated.
And the compressor can crash.
Usually the surge line interpolate the maximum of the map curves (but this is not a rule).
In axial compressor the field of stability is restricted if there are a lot of stages.
STALL
when the laminar air flow become tubolent there is stall. This situation can happen over the casing or over the blading.
the stall is favoured by a positive gradient of pressure (delta_p/delta_x > 0) and it is delayed by negative gradient of pressure (delta_p/delta_x < 0),
for this reason it's really difficult to have stall in a turbine (delta_p/delta_x in a turbine is negative).
Blading:
Over a blade we can have stall by the suction side or by the pressure side, it depends on the angle between tangential velocity (U) and relative velocity (W).
If this angle differs too much from the angle of project there is stall. If there is stall it means that a part of the flow of mass can't pass through two consecutive blade.
So the exceeding flow of mass must pass through the nearest vanes(Z-A & B-C in the figure); in this way the direction of the relative velocity of the nearest blades changes and after a short time the stall is passed in the next blade (from B to A).
We have a rotating stall.
By experimental tests we know that if the Lieblein coefficient is < 0.4 there isn't stall on blading. (c is the blade chord, s is the step between two blades, Wu is the component of W directed like U and Wa is the axial component of W).
(in the figure number 1 indicates the entrance of rotor and number 2 the exit of rotor)
Casing:
there isn't stall in the casing if the pressure coefficient in the rotor and the the pressure coefficient in the stator are < 0.5
the most critical point is the hub of stator blade.
It's usual to project with simmetric triangles of velocity (modulus of W2 = modulus of c1 and modulus of W1 = modulus of C2).
So the gap of pressure (delta_p) is the same for rotor and stator.
Besides is usual to have the absolute velocity in entrance of the stage-disc equal in modulus of abslolute velocity at the exit. (modulus of c1 = modulus of c3).
(in the figure p3 is the pressure at the exit of stator, c2 is the absolute velocity - c2= W2 + U, it's a vectorial sum).
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excuse me for my english, but I'm italian.
RE: Turbine Engine Surge Stall
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RE: Turbine Engine Surge Stall
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Regards
Fernando
RE: Turbine Engine Surge Stall
RE: Turbine Engine Surge Stall
Gordon, can you be a bit more specific when you say "wavy?" Are you refering to the swept/blended fan blade designs most of us have moved to?
RE: Turbine Engine Surge Stall
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