Axial compressor

Machine for continuous flow gas compression

Further information: Axial fan design

An animated simulation of an axial compressor. The static blades are the stators.

An axial compressor is a gas compressor that can continuously pressurize gases. It is a rotating, airfoil-based compressor in which the gas or working fluid principally flows parallel to the axis of rotation, or axially. This differs from other rotating compressors such as centrifugal compressor, axi-centrifugal compressors and mixed-flow compressors where the fluid flow will include a "radial component" through the compressor.

The energy level of the fluid increases as it flows through the compressor due to the action of the rotor blades which exert a torque on the fluid. The stationary blades slow the fluid, converting the circumferential component of flow into pressure. Compressors are typically driven by an electric motor or a steam or a gas turbine.[1]

Axial flow compressors produce a continuous flow of compressed gas, and have the benefits of high efficiency and large mass flow rate, particularly in relation to their size and cross-section. They do, however, require several rows of airfoils to achieve a large pressure rise, making them complex and expensive relative to other designs (e.g. centrifugal compressors).

Axial compressors are integral to the design of large gas turbines such as jet engines, high speed ship engines, and small scale power stations. They are also used in industrial applications such as large volume air separation plants, blast furnace air, fluid catalytic cracking air, and propane dehydrogenation. Due to high performance, high reliability and flexible operation during the flight envelope, they are also used in aerospace rocket engines, as fuel pumps and in other critical high volume applications.[2]

Typical application | Type of flow | Pressure ratio per stage | Efficiency per stage[2]

|
|
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Industrial | Subsonic | 1.05–1.2 | 88–92%
Aerospace | Transonic | 1.15–1.6 | 80–85%
Research | Supersonic | 1.8–2.2 | 75–85%

## Description

[edit]

The axial compressor in a Pratt & Whitney TF30 turbofan engine.

Axial compressors consist of rotating and stationary components. A shaft drives a central drum which is retained by bearings inside of a stationary tubular casing. Between the drum and the casing are rows of airfoils, each row connected to either the drum or the casing in an alternating manner. A pair of one row of rotating airfoils and the next row of stationary airfoils is called a stage. The rotating airfoils, also known as blades or rotors, accelerate the fluid in both the axial and circumferential directions. The stationary airfoils, also known as vanes or stators, convert the increased kinetic energy into static pressure through diffusion and redirect the flow direction of the fluid to prepare it for the rotor blades of the next stage.[3] The cross-sectional area between rotor drum and casing is reduced in the flow direction to maintain an optimum Mach number axial velocity as the fluid is compressed.

## Working

[edit]

As the fluid enters and leaves in the axial direction, the centrifugal component in the energy equation does not come into play. Here the compression is fully based on diffusing action of the passages. The diffusing action in the stator converts the absolute kinetic head of the fluid into a rise in pressure. The relative kinetic head in the energy equation is a term that exists only because of the rotation of the rotor. The rotor reduces the relative kinetic head of the fluid and adds it to the absolute kinetic head of the fluid i.e., the impact of the rotor on the fluid particles increases their velocity (absolute) and thereby reduces the relative velocity between the fluid and the rotor. In short, the rotor increases the absolute velocity of the fluid and the stator converts this into pressure rise. Designing the rotor passage with a diffusing capability can produce a pressure rise in addition to its normal functioning. This produces greater pressure rise per stage which constitutes a stator and a rotor together. This is the reaction principle in turbomachines. If 50% of the pressure rise in a stage is obtained at the rotor section, it is said to have a 50% reaction.[citation needed]

## Design

[edit]

The increase in pressure produced by a single stage is limited by the relative velocity between the rotor and the fluid, and the turning and diffusion capabilities of the airfoils. A typical stage in a commercial compressor will produce a pressure increase of between 15% and 60% (pressure ratios of 1.15–1.6) at design conditions with a polytropic efficiency in the region of 90–95%. To achieve different pressure ratios, axial compressors are designed with different numbers of stages and rotational speeds. As a rule of thumb we can assume that each stage in a given compressor has the same temperature rise (Delta T). Therefore, at the entry, temperature (Tstage) to each stage must increase progressively through the compressor and the ratio (Delta T)/(Tstage) entry must decrease, thus implying a progressive reduction in stage pressure ratio through the unit. Hence the rear stage develops a significantly lower pressure ratio than the first stage. Higher stage pressure ratios are also possible if the relative velocity between fluid and rotors is supersonic, but this is achieved at the expense of efficiency and operability. Such compressors, with stage pressure ratios of over 2, are only used where minimizing the compressor size, weight or complexity is critical, such as in military jets.

The airfoil profiles are optimized and matched for specific velocities and turning. Although compressors can be run at other conditions with different flows, speeds, or pressure ratios, this can result in an efficiency penalty or even a partial or complete breakdown in flow (known as compressor stall and pressure surge respectively). Thus, a practical limit on the number of stages, and the overall pressure ratio, comes from the interaction of the different stages when required to work away from the design conditions. These “off-design” conditions can be mitigated to a certain extent by providing some flexibility in the compressor. This is achieved normally through the use of adjustable stators or with valves that can bleed fluid from the main flow between stages (inter-stage bleed). Modern jet engines use a series of compressors, running at different speeds; to supply air at around 40:1 pressure ratio for combustion with sufficient flexibility for all flight conditions.

## Kinetics and energy equations

[edit]

Velocity triangle of the swirling fluid entering and exiting the rotor blade

The law of moment of momentum states that the sum of the moments of external forces acting on a fluid which is temporarily occupying the control volume is equal to the net change of angular momentum flux through the control volume.

The swirling fluid enters the control volume at radius,  r 1 {\displaystyle r_{1}\,} , with tangential velocity,  V w 1 {\displaystyle V_{w1}\,} , and leaves at radius,  r 2 {\displaystyle r_{2}\,} , with tangential velocity,  V w 2 {\displaystyle V_{w2}\,} .

V 1 {\displaystyle V_{1}\,} and  V 2 {\displaystyle V_{2}\,} are the absolute velocities at the inlet and outlet respectively.
V f 1 {\displaystyle V_{f1}\,} and  V f 2 {\displaystyle V_{f2}\,} are the axial flow velocities at the inlet and outlet respectively.
V w 1 {\displaystyle V_{w1}\,} and  V w 2 {\displaystyle V_{w2}\,} are the swirl velocities at the inlet and outlet respectively.
V r 1 {\displaystyle V_{r1}\,} and  V r 2 {\displaystyle V_{r2}\,} are the blade-relative velocities at the inlet and outlet respectively.
U {\displaystyle U\,} is the linear velocity of the blade.
α {\displaystyle \alpha } is the guide vane angle and  β {\displaystyle \beta } is the blade angle.

Rate of change of momentum, F is given by the equation:

F = m ˙ ( V w 2 − V w 1 ) = m ˙ ( V f 2 tan ⁡ α 2 − V f 1 tan ⁡ α 1 ) {\displaystyle F={\dot {m}}\left(V_{w2}-V_{w1}\right)={\dot {m}}\left(V_{f2}\tan \alpha _{2}-V_{f1}\tan \alpha _{1}\right)\,} (from velocity triangle)

Power consumed by an ideal moving blade, P is given by the equation:

P = m ˙ U ( V f 2 tan ⁡ α 2 − V f 1 tan ⁡ α 1 ) {\displaystyle P={\dot {m}}U\left(V_{f2}\tan \alpha _{2}-V_{f1}\tan \alpha _{1}\right)\,}

Change in enthalpy of fluid in moving blades:

P = m ˙ ( h 02 − h 01 ) = m ˙ c p ( T 02 − T 01 ) {\displaystyle P={\dot {m}}\left(h_{02}-h_{01}\right)={\dot {m}}c_{p}\left(T_{02}-T_{01}\right)\,}

Therefore,

P = m ˙ U ( V f 2 tan ⁡ α 2 − V f 1 tan ⁡ α 1 ) = m ˙ c p ( T 02 − T 01 ) {\displaystyle P={\dot {m}}U\left(V_{f2}\tan \alpha _{2}-V_{f1}\tan \alpha _{1}\right)={\dot {m}}c_{p}\left(T_{02}-T_{01}\right)\,}

which implies,

δ ( T 0 ) isentropic = U c p ( V f 2 tan ⁡ α 2 − V f 1 tan ⁡ α 1 ) {\displaystyle \delta (T_{0})_{\text{isentropic}}={\frac {U}{c_{p}}}\left(V_{f2}\tan \alpha _{2}-V_{f1}\tan \alpha _{1}\right)\,}

Isentropic compression in rotor blade,

p 2 − p 1 = p 1 ( [ T 2 T 1 ] γ γ − 1 − 1 ) {\displaystyle p_{2}-p_{1}=p_{1}\left(\left[{\frac {T_{2}}{T_{1}}}\right]^{\frac {\gamma }{\gamma -1}}-1\right)\,}

Therefore,

( p 02 ) actual p 01 = ( 1 + η stage δ ( T 0 ) isentropic T 01 ) γ γ − 1 {\displaystyle {\frac {(p_{02})_{\text{actual}}}{p_{01}}}=\left(1+{\frac {\eta _{\text{stage}}\delta (T_{0})_{\text{isentropic}}}{T_{01}}}\right)^{\frac {\gamma }{\gamma -1}}\,}

which implies

( p 02 ) actual p 01 = ( 1 + η stage U T 01 c p [ V f 2 tan ⁡ α 2 − V f 1 tan ⁡ α 1 ] ) γ γ − 1 {\displaystyle {\frac {(p_{02})_{\text{actual}}}{p_{01}}}=\left(1+{\frac {\eta _{\text{stage}}U}{T_{01}c_{p}}}\left[V_{f2}\tan \alpha _{2}-V_{f1}\tan \alpha _{1}\right]\right)^{\frac {\gamma }{\gamma -1}}\,}

Degree of Reaction, The pressure difference between the entry and exit of the rotor blade is called reaction pressure. The change in pressure energy is calculated through degree of reaction.

R = h 2 − h 1 h 02 − h 01 P = m ˙ c p ( T 2 + V 2 2 2 c p − [ T 1 + V 1 2 2 c p ] ) P = m ˙ ( h 2 − h 1 + [ V 2 2 2 − V 1 2 2 ] ) h 2 − h 1 = V r 1 2 2 − V r 2 2 2 T 2 − T 1 = V r 1 2 2 c p − V r 2 2 2 c p {\displaystyle {\begin{aligned}R&={\frac {h_{2}-h_{1}}{h_{02}-h_{01}}}\\\P&={\dot {m}}c_{p}\left(T_{2}+{\frac {V_{2}^{2}}{2c_{p}}}-\left[T_{1}+{\frac {V_{1}^{2}}{2c_{p}}}\right]\right)\\\P&={\dot {m}}\left(h_{2}-h_{1}+\left[{\frac {V_{2}^{2}}{2}}-{\frac {V_{1}^{2}}{2}}\right]\right)\\\h_{2}-h_{1}&={\frac {V_{r1}^{2}}{2}}-{\frac {V_{r2}^{2}}{2}}\\\T_{2}-T_{1}&={\frac {V_{r1}^{2}}{2c_{p}}}-{\frac {V_{r2}^{2}}{2c_{p}}}\end{aligned}}}

Therefore,

R = V r 1 2 − V r 2 2 V r 1 2 − V r 2 2 + V 1 2 − V 2 2 {\displaystyle R={\frac {V_{r1}^{2}-V_{r2}^{2}}{V_{r1}^{2}-V_{r2}^{2}+V_{1}^{2}-V_{2}^{2}}}\,}

## Performance characteristics

[edit]

Reasons stating difference in ideal and actual performance curve in an axial compressor

## Instabilities

[edit]

Greitzer[4] used a Helmholtz resonator type of compression system model to predict the transient response of a compression system after a small perturbation superimposed on a steady operating condition. He found a non-dimensional parameter which predicted which mode of compressor instability, rotating stall or surge, would result. The parameter used the rotor speed, Helmholtz resonator frequency of the system and an "effective length" of the compressor duct. It had a critical value which predicted either rotating stall or surge where the slope of pressure ratio against flow changed from negative to positive.

## Steady-state performance

[edit]

Axial compressor performance is shown on a compressor map, also known as a characteristic, by plotting pressure ratio and efficiency against corrected mass flow at different values of corrected compressor speed.

Axial compressors, particularly near their design point are usually amenable to analytical treatment, and a good estimate of their performance can be made before they are first run on a rig. The compressor map shows the complete running range, i.e. off-design, of the compressor from ground idle to its highest corrected rotor speed, which for a civil engine may occur at top-of-climb, or, for a military combat engine, at take-off on a cold day.[5] Not shown is the sub-idle performance region needed for analyzing normal ground and in-flight windmill start behaviour.

The performance of a single compressor stage may be shown by plotting stage loading coefficient ( ψ {\displaystyle \psi \,} ) as a function of flow coefficient ( ϕ {\displaystyle \phi \,} )

Stage pressure ratio against flow rate is lower than for a no-loss stage as shown. Losses are due to blade friction, flow separation, unsteady flow and vane-blade spacing.

### Off-design operation

[edit]

Off design characteristics curve of an axial compressor. Stage loading coefficient ( ψ {\displaystyle \psi \,} ) as function of flow coefficient ( ϕ {\displaystyle \phi \,} )

The performance of a compressor is defined according to its design. But in actual practice, the operating point of the compressor deviates from the design- point which is known as off-design operation.

ψ = ϕ ( tan ⁡ α 2 − tan ⁡ α 1 ) {\displaystyle \psi =\phi (\tan \alpha _{2}-\tan \alpha _{1})\,} |  | 1

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|

tan ⁡ α 2 = 1 ϕ − tan ⁡ β 2 {\displaystyle \tan \alpha _{2}={\frac {1}{\phi }}-\tan \beta _{2}\,} |  | 2

|
|

from equation (1) and (2)

ψ = 1 − ϕ ( tan ⁡ β 2 + tan ⁡ α 1 ) {\displaystyle \psi =1-\phi (\tan \beta _{2}+\tan \alpha _{1})\,}

The value of  ( tan ⁡ β 2 + tan ⁡ α 1 ) {\displaystyle (\tan \beta _{2}+\tan \alpha _{1})\,} doesn't change for a wide range of operating points till stalling. Also  α 1 = α 3 {\displaystyle \alpha _{1}=\alpha _{3}\,} because of minor change in air angle at rotor and stator, where  α 3 {\displaystyle \alpha _{3}\,} is diffuser blade angle.

J = tan ⁡ β 2 + tan ⁡ α 3 ) {\displaystyle J=\tan \beta _{2}+\tan \alpha _{3})\,} is constant

Representing design values with (')

ψ ′ = 1 − J ( ϕ ′ ) J = 1 − ψ ′ ϕ ′ {\displaystyle {\begin{aligned}\psi '&=1-J(\phi ')\,\\\J&={\frac {1-\psi '}{\phi '}}\end{aligned}}} |  | 3

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|

for off-design operations (from eq. 3):

ψ = 1 − J ( ϕ ) ψ = 1 − ϕ ( 1 − ψ ′ ϕ ′ ) {\displaystyle {\begin{aligned}\psi &=1-J(\phi )\,\\\\\psi &=1-\phi \left({\frac {1-\psi '}{\phi '}}\right)\,\end{aligned}}}

for positive values of J, slope of the curve is negative and vice versa.

### Surging

[edit]

Various points on the performance curve depending upon the flow rates and pressure difference

In the plot of pressure-flow rate the line separating graph between two regions- unstable and stable is known as the surge line. This line is formed by joining surge points at different rpms. Unstable flow in axial compressors due to complete breakdown of the steady through flow is termed as surging.[1] This phenomenon affects the performance of compressor and is undesirable.

### Surge cycle

[edit]

The following explanation for surging refers to running a compressor at a constant speed on a rig and gradually reducing the exit area by closing a valve. What happens, i.e. crossing the surge line, is caused by the compressor trying to deliver air, still running at the same speed, to a higher exit pressure. When the compressor is operating as part of a complete gas turbine engine, as opposed to on a test rig, a higher delivery pressure at a particular speed can be caused momentarily by burning too-great a step-jump in fuel which causes a momentary blockage until the compressor increases to the speed which goes with the new fuel flow and the surging stops.

Suppose the initial operating point D ( m ˙ , P D {\displaystyle {\dot {m}},P_{D}\,} ) at some rpm N. On decreasing the flow-rate at same rpm along the characteristic curve by partial closing of the valve, the pressure in the pipe increases which will be taken care by increase in input pressure at the compressor. Further increase in pressure till point P (surge point), compressor pressure will increase. Further moving towards left keeping rpm constant, pressure in pipe will increase but compressor pressure will decrease leading to back air-flow towards the compressor. Due to this back flow, pressure in pipe will decrease because this unequal pressure condition cannot stay for a long period of time. Though valve position is set for lower flow rate say point G but compressor will work according to normal stable operation point say E, so path E-F-P-G-E will be followed leading to breakdown of flow, hence pressure in the compressor falls further to point H( P H {\displaystyle P_{H}\,} ). This increase and decrease of pressure in pipe will occur repeatedly in pipe and compressor following the cycle E-F-P-G-H-E also known as the surge cycle.

This phenomenon will cause vibrations in the whole machine and may lead to mechanical failure. That is why left portion of the curve from the surge point is called unstable region and may cause damage to the machine. So the recommended operation range is on the right side of the surge line.

### Stalling

[edit]

Stalling is an important phenomenon that affects the performance of the compressor. An analysis is made of rotating stall in compressors of many stages, finding conditions under which a flow distortion can occur which is steady in a traveling reference frame, even though upstream total and downstream static pressure are constant. In the compressor, a pressure-rise hysteresis is assumed.[6] It is a situation of separation of air flow at the aero-foil blades of the compressor. This phenomenon depending upon the blade-profile leads to reduced compression and drop in engine power.

Positive stalling
Flow separation occur on the suction side of the blade.
Negative stalling
Flow separation occur on the pressure side of the blade.

Negative stall is negligible compared to the positive stall because flow separation is least likely to occur on the pressure side of the blade.

In a multi-stage compressor, at the high pressure stages, axial velocity is very small. Stalling value decreases with a small deviation from the design point causing stall near the hub and tip regions whose size increases with decreasing flow rates. They grow larger at very low flow rate and affect the entire blade height. Delivery pressure significantly drops with large stalling which can lead to flow reversal. The stage efficiency drops with higher losses.

#### Rotating stalling

[edit]

See also: Compressor stall

Non-uniformity of air flow in the rotor blades may disturb local air flow in the compressor without upsetting it. The compressor continues to work normally but with reduced compression. Thus, rotating stall decreases the effectiveness of the compressor.

In a rotor with blades moving say towards right. Let some blades receives flow at higher incidence, this blade will stop positively. It creates obstruction in the passage between the blade to its left and itself. Thus the left blade will receive the flow at higher incidence and the blade to its right with decreased incidence. The left blade will experience more stall while the blade to its right will experience lesser stall. Towards the right stalling will decrease whereas it will increase towards its left. Movement of the rotating stall can be observed depending upon the chosen reference frame.

#### Effects

[edit]

* This reduces efficiency of the compressor
* Forced vibrations in the blades due to passage through stall compartment.
* These forced vibrations may match with the natural frequency of the blades causing resonance and hence failure of the blade.

## Development

[edit]

From an energy exchange point of view axial compressors are reversed turbines. Steam-turbine designer Charles Algernon Parsons, for example, recognized that a turbine which produced work by virtue of a fluid's static pressure (i.e. a reaction turbine) could have its action reversed to act as an air compressor, calling it a turbo compressor or pump. His rotor and stator blading described in one of his patents[7] had little or no camber although in some cases the blade design was based on propeller theory.[8] The machines, driven by steam turbines, were used for industrial purposes such as supplying air to blast furnaces. Parsons supplied the first commercial axial flow compressor for use in a lead smelter in 1901.[9] Parsons' machines had low efficiencies, later attributed to blade stall, and were soon replaced with more efficient centrifugal compressors. Brown Boveri & Cie produced "reversed turbine" compressors, driven by gas turbines, with blading derived from aerodynamic research which were more efficient than centrifugal types when pumping large flow rates of 40,000 cu.ft. per minute at pressures up to 45 p.s.i.[9]

Because early axial compressors were not efficient enough a number of papers in the early 1920s claimed that a practical axial-flow turbojet engine would be impossible to construct. Things changed after A. A. Griffith published a seminal paper in 1926, noting that the reason for the poor performance was that existing compressors used flat blades and were essentially "flying stalled". He showed that the use of airfoils instead of the flat blades would increase efficiency to the point where a practical jet engine was a real possibility. He concluded the paper with a basic diagram of such an engine, which included a second turbine that was used to power a propeller.

Although Griffith was well known due to his earlier work on metal fatigue and stress measurement, little work appears to have started as a direct result of his paper. The only obvious effort was a test-bed compressor built by Hayne Constant, Griffith's colleague at the Royal Aircraft Establishment. Other early jet efforts, notably those of Frank Whittle and Hans von Ohain, were based on the more robust and better understood centrifugal compressor which was widely used in superchargers. Griffith had seen Whittle's work in 1929 and dismissed it, noting a mathematical error, and going on to claim that the frontal size of the engine would make it useless on a high-speed aircraft.

Real work on axial-flow engines started in the late 1930s, in several efforts that all started at about the same time. In England, Hayne Constant reached an agreement with the steam turbine company Metropolitan-Vickers (Metrovick) in 1937, starting their turboprop effort based on the Griffith design in 1938. In 1940, after the successful run of Whittle's centrifugal-flow design, their effort was re-designed as a pure jet, the Metrovick F.2. In Germany, von Ohain had produced several working centrifugal engines, some of which had flown including the world's first jet aircraft (He 178), but development efforts had moved on to Junkers (Jumo 004) and BMW (BMW 003), which used axial-flow designs in the world's first jet fighter (Messerschmitt Me 262) and jet bomber (Arado Ar 234). In the United States, both Lockheed and General Electric were awarded contracts in 1941 to develop axial-flow engines, the former a pure jet, the latter a turboprop. Northrop also started their own project to develop a turboprop, which the US Navy eventually contracted in 1943. Westinghouse also entered the race in 1942, their project proving to be the only successful one of the US efforts, later becoming the J30.

As Griffith had originally noted in 1929, the large frontal size of the centrifugal compressor caused it to have higher drag than the narrower axial-flow type. Additionally the axial-flow design could improve its compression ratio simply by adding additional stages and making the engine slightly longer. In the centrifugal-flow design the compressor itself had to be larger in diameter, which was much more difficult to fit properly into a thin and aerodynamic aircraft fuselage (although not dissimilar to the profile of radial engines already in widespread use). On the other hand, centrifugal-flow designs remained much less complex (the major reason they "won" in the race to flying examples) and therefore have a role in places where size and streamlining are not so important.

## Axial-flow jet engines

[edit]

Low-pressure axial compressor scheme of the Olympus BOl.1 turbojet.

In the jet engine application, the compressor faces a wide variety of operating conditions. On the ground at takeoff the inlet pressure is high, inlet speed zero, and the compressor spun at a variety of speeds as the power is applied. Once in flight the inlet pressure drops, but the inlet speed increases (due to the forward motion of the aircraft) to recover some of this pressure, and the compressor tends to run at a single speed for long periods of time.

There is simply no "perfect" compressor for this wide range of operating conditions. Fixed geometry compressors, like those used on early jet engines, are limited to a design pressure ratio of about 4 or 5:1. As with any heat engine, fuel efficiency is strongly related to the compression ratio, so there is very strong financial need to improve the compressor stages beyond these sorts of ratios.

Additionally the compressor may stall if the inlet conditions change abruptly, a common problem on early engines. In some cases, if the stall occurs near the front of the engine, all of the stages from that point on will stop compressing the air. In this situation the energy required to run the compressor drops suddenly, and the remaining hot air in the rear of the engine allows the turbine to speed up[citation needed] the whole engine dramatically. This condition, known as surging, was a major problem on early engines and often led to the turbine or compressor breaking and shedding blades.

For all of these reasons, axial compressors on modern jet engines are considerably more complex than those on earlier designs.

### Spools

[edit]

A dual-spool axial-flow compressor. N1 and N2 represent the rotational speed of the low- and high-pressure compressors respectively. Both are presented on the indicator as a percentage of design rpm.[10]

All compressors have an optimum point relating rotational speed and pressure, with higher compressions requiring higher speeds. Early engines were designed for simplicity, and used a single large compressor spinning at a single speed. Later designs added a second turbine and divided the compressor into low-pressure and high-pressure sections, the latter spinning faster. This two-spool design, pioneered on the Bristol Olympus, resulted in increased efficiency. Further increases in efficiency may be realised by adding a third spool, but in practice the added complexity increases maintenance costs to the point of negating any economic benefit. That said, there are several three-spool engines in use, perhaps the most famous being the Rolls-Royce RB211 (and its successor, the Rolls-Royce Trent), used on a wide variety of commercial aircraft.

### Bleed air, variable stators

[edit]

See also: Bleed air

As an aircraft changes speed or altitude, the pressure of the air at the inlet to the compressor will vary. In order to "tune" the compressor for these changing conditions, designs starting in the 1950s would "bleed" air out of the middle of the compressor in order to avoid trying to compress too much air in the final stages. This was also used to help start the engine, allowing it to be spun up without compressing much air by bleeding off as much as possible. Bleed systems were already commonly used anyway, to provide airflow into the turbine stage where it was used to cool the turbine blades, as well as provide pressurized air for the air conditioning systems inside the aircraft.

A more advanced design, the variable stator, used blades that can be individually rotated around their axis, as opposed to the power axis of the engine.[11] For startup they are rotated to "closed", reducing compression, and then are rotated back into the airflow as the external conditions require. The General Electric J79 was the first major example of a variable stator design, and today it is a common feature of most military engines.

Closing the variable stators progressively, as compressor speed falls, reduces the slope of the surge (or stall) line on the operating characteristic (or map), improving the surge margin of the installed unit. By incorporating variable stators in the first five stages, General Electric Aircraft Engines has developed a ten-stage axial compressor capable of operating at a 23:1 design pressure ratio.

## Design notes

[edit]

### Energy exchange between rotor and fluid

[edit]

The relative motion of the blades to the fluid adds velocity or pressure or both to the fluid as it passes through the rotor. The fluid velocity is increased through the rotor, and the stator converts kinetic energy to pressure energy. Some diffusion also occurs in the rotor in most practical designs.

The increase in velocity of the fluid is primarily in the tangential direction (swirl) and the stator removes this angular momentum.

The pressure rise results in a stagnation temperature rise. For a given geometry the temperature rise depends on the square of the tangential Mach number of the rotor row. Current turbofan engines have fans that operate at Mach 1.7 or more, and require significant containment and noise suppression structures to reduce blade loss damage and noise.

### Compressor maps

[edit]

A map shows the performance of a compressor and allows determination of optimal operating conditions. It shows the mass flow along the horizontal axis, typically as a percentage of the design mass flow rate, or in actual units. The pressure rise is indicated on the vertical axis as a ratio between inlet and exit stagnation pressures.

A surge or stall line identifies the boundary to the left of which the compressor performance rapidly degrades and identifies the maximum pressure ratio that can be achieved for a given mass flow. Contours of efficiency are drawn as well as performance lines for operation at particular rotational speeds.

### Compression stability

[edit]

Operating efficiency is highest close to the stall line. If the downstream pressure is increased beyond the maximum possible the compressor will stall and become unstable.

Typically the instability will be at the Helmholtz frequency of the system, taking the downstream plenum into account.

## See also

[edit]

* Centrifugal compressor – Sub-class of dynamic axisymmetric work-absorbing turbomachinery
* Components of jet engines – Brief description of components needed for jet engines
* Axial fan design – Fan that induces gas flow mostly parallel to the shaft
* Axial-flow pump – Type of pump consisting of a propeller in a pipe
* Turbopump – Pump driven by a gas turbine

## References

[edit]

1. ^ a b Yahya, S.M. (2011). Turbines, Compressors and Fans. Tata McGraw Hill Education Private Limited. ISBN 978-0-07-070702-3.
2. ^ a b Meherwan, P.Boyce. "2.0 Axial Flow Compressors".
3. ^ Perry, R.H. and Green, D.W. (Eds.) (2007). Perry's Chemical Engineers' Handbook (8th ed.). McGraw Hill.ISBN 0-07-142294-3.
4. ^ Greitzer, E. M. (1 April 1976). "Surge and Rotating Stall in Axial Flow Compressors—Part I: Theoretical Compression System Model". Journal of Engineering for Gas Turbines and Power. 98 (2): 190–198\. doi:10.1115/1.3446138.
5. ^ "Practical considerations when designing the engine cycle" (PDF). www.sto.nato.int.
6. ^ McDougall, NM; Cumpsty, NA; Hynes, TP (2012). "Stall inception in axial compressors". Journal of Turbomachinery. 112 (1): 116–123\. doi:10.1115/1.2927406.
7. ^ "Turbo Compressor and Pump Patent" (PDF). patentimages.storage.googleapis.
8. ^ "NASA-SP36_extracto" (PDF). webserver.dmt.upm.es.
9. ^ a b https://gracesguide.co.uk/Main_Page The Engineer magazine May 27, 1938 Supplement The Development Of Blowers And Compressors p.xxxiii
10. ^ Pilot's Handbook of Aeronautical Knowledge. Federal Aviation Administration. 2016-08-24. pp. 7–23.
11. ^ "The Nuclear-Powered Jet Engine, Ceramic Turbines and Other Gems from the History of Flight | GE News".

## Bibliography

[edit]

* Treager, Irwin E. 'Aircraft Gas Turbine Engine Technology' 3rd edn, McGraw-Hill Book Company, 1995, ISBN 978-0-02-8018287
* Hill, Philip and Carl Peterson. 'Mechanics and Thermodynamics of Propulsion,' 2nd edn, Prentice Hall, 1991. ISBN 0-201-14659-2.
* Kerrebrock, Jack L. 'Aircraft Engines and Gas Turbines,' 2nd edn, Cambridge, Massachusetts: The MIT Press, 1992. ISBN 0-262-11162-4.
* Rangwalla, Abdulla. S. 'Turbo-Machinery Dynamics: Design and Operation,' New York: McGraw-Hill: 2005. ISBN 0-07-145369-5.
* Wilson, David Gordon and Theodosios Korakianitis. 'The Design of High-Efficiency Turbomachinery and Turbines,' 2nd edn, Prentice Hall, 1998. ISBN 0-13-312000-7.

* v
* t
* e

Jet engines and aircraft gas turbines

Gas turbines
and jet propulsion|

| Types|

* Air turborocket
* Pulsejet/Valveless pulsejet/Gluhareff Pressure Jet
* Pulse detonation engine
* Propfan
* Turbofan
* Turbojet
* Turboprop
* Turboshaft
* Ramjet
* Scramjet
* Shcramjet
* Rocket
* Rotating detonation engine

|

Mechanical
components|

* Accessory drive
* Air intake
* Afterburner (reheat)
* Axial compressor
* Centrifugal compressor
* Combustor
* Constant speed drive
* Impeller
* Nose bullet
* Propelling nozzle
* Turbine blade

Principles|

* Aircraft engine starting
* Bleed air
* Brayton cycle
* Bypass ratio
* Compressor stall
* Engine pressure ratio (EPR)
* Flameout
* Jet engine performance
* Overall pressure ratio
* Propulsive efficiency
* Specific impulse
* Thrust
* Thrust lapse
* Thrust specific fuel consumption
* Thrust to weight ratio
* Variable cycle engine
* Windmill restart

Propellers|

| Components|

* Propeller governor
* Propeller speed reduction unit

|

Principles|

* Autofeather
* Blade pitch
* Constant-speed
* Contra-rotating
* Counter-rotating
* Proprotor
* Scimitar
* Variable-pitch

Engine
instruments|

* Annunciator panel
* Electronic centralised aircraft monitor (ECAM)
* Electronic flight instrument system (EFIS)
* Engine-indicating and crew-alerting system (EICAS)
* Flight data recorder
* Glass cockpit

Engine controls|

* Autothrottle
* Full Authority Digital Engine/Electronics (FADEC)
* Thrust lever
* Thrust reversal

Fuel and induction
systems|

* Flame holder
* Jet fuel

Other systems|

* Air-start system
* Auxiliary power unit (APU)
* Bleed air system
* Hydraulic system
* Ice protection system

Authority control databases

National|

* United States
* Israel

Other|

* Yale LUX

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