Turbojet- An Airbreathing Jet Engine, How It Works and Its Evolution
Turbojets were widely used for early
supersonic fighters, up to and including many 3rd generation
fighters, with the MiG-25 being the most powerful turbojet-powered
fighter developed. As most fighters spend little time traveling
supersonically, 4th-generation fighters (as also some 3rd-generation
fighters like the F-111 and Hawker Siddeley Harrier jump jets
and many subsequent designs have been powered by more efficient low-bypass
turbofans. The turbofans use afterburners to raise exhaust speed for
bursts of supersonic travel. Turbojets were used on the Concorde and
the long-range versions of the Tu-144 which were required to spend a
long time travelling supersonically. Turbojets are still common in medium
range cruise missiles, due to their high exhaust speed, small frontal
area, and relative simplicity.
History of Turbojet Engine
Heinkel He 178, of 1930s Germany is the world's first aircraft to fly purely on turbojet power, using an HeS 3 engine. The first patent for use ofa gas turbine to power an aircraft was filed in 1921 by Maxime Guillaume of France. His engine was to be an axial-flow turbojet, but was never built, as it needed considerable advances over the state of the art in compressors. The Whittle W.2/700 engine flew in the Gloster E.28/39, the first British aircraft to fly with a turbojet engine, and the Gloster Meteor. In 1928, British RAF College Cranwell cadet Frank Whittle submitted his ideas for a turbojet to his superiors. He started working on it in October 1929 he developed his ideas further.
One of the last applications of a turbojet engine
was Concorde, which used the Olympus 593 engine. However,
joint studies by Rolls-Royce and Snecma for a 2nd generation SST engine using
the 593 core were done more than 3 years before Concorde entered service. They
evaluated bypass engines with bypass ratios between 0.1 and 1.0 to give
improved take-off and cruising performance. The 593 met all the
requirements of the Concorde programme. Estimates made in 1964 for the
Concorde design at Mach 2.2 showed the penalty in range for the supersonic
airliner, in terms of miles per gallon, compared to subsonic airliners at Mach
0.85 (Boeing 707, DC-8) was relatively small. This is because the large
increase in drag is largely compensated by an increase in powerplant efficiency
(the engine efficiency is increased by the ram pressure rise which adds to the
compressor pressure rise, the higher aircraft speed approaches the exhaust jet
speed increasing propulsive efficiency).
Turbojet engines had a significant impact on commercial
aviation. Aside from giving faster flight speeds turbojets had greater
reliability than piston engines, with some models demonstrating dispatch
reliability rating in excess of 99.9%. Pre-jet commercial aircraft were
designed with as many as 4 engines because of concerns over in-flight failures.
Overseas flight paths were plotted to keep planes within an hour of a landing
field, lengthening flights. The increase in reliability that came with the
turbojet enabled three- and two-engine designs, and more direct long-distance
flights. High-temperature alloys were a reverse salient, a key
technology that dragged progress on jet engines. Non-UK jet engines built in
the 1930s and 1940s had to be overhauled every 10 or 20 hours due to creep
failure and other types of damage to blades. British engines, however, used Nimonic alloys
which allowed extended use without overhaul, engines such as
the Rolls-Royce Welland and Rolls-Royce Derwent, and by 1949
the de Havilland Goblin, being type tested for 500 hours without
maintenance. It wasn’t until 1950s that superalloy technology
allowed other countries to produce economically practical engines.
Early Designs
Early German turbojets had severe limitations on the amount
of running they could do due to the lack of suitable high temperature materials
for the turbines. British engines such as the Rolls-Royce
Welland used better materials giving improved durability. The Welland
was type-certified for 80 hours initially, later extended to 150
hours between overhauls, as a result of an extended 500-hour run being achieved
in tests. General Electric in the USA was in a good position to enter the
jet engine business due to its experience with the high-temperature materials
used in their turbosuperchargers during World War II.
Water injection was a common method used to increase thrust, usually during takeoff, in early turbojets that were thrust-limited by their allowable turbine entry temperature. The water increased thrust at the temperature limit, but prevented complete combustion, often leaving a very visible smoke trail. Allowable turbine entry temperatures have increased steadily over time both with the introduction of superior alloys and coatings, and with the introduction and progressive effectiveness of blade cooling designs. On early engines, the turbine temperature limit had to be monitored, and avoided, by the pilot, typically during starting and at maximum thrust settings. Automatic temperature limiting was introduced to reduce pilot workload and reduce the likelihood of turbine damage due to over-temperature.
Components
The compressor is driven by the turbine stage and throws the
air outwards, requiring it to be redirected parallel to the axis of thrust.
Schematic diagram showing the operation of an axial flow turbojet engine.
Here, the compressor is again driven by the turbine, but the air flow remains parallel to the axis of thrust.
Schematic diagram of a Turbine Based Combined Cycle (TBCC)
engine integration.
1) Air intake for low flight speeds
2) Air intake for high flight speeds
3) Turbojet
4) Statoreactor
5) Stator reactor nozzle
6) Turbojet nozzle.
Nose bullet
A nose bullet is a component of a turbojet used to divert air
into the intake, in front of the accessory drive and to house the starter
motor.
Air intake
An intake, or tube, is needed in front of the compressor to
help direct the incoming air smoothly into the rotating compressor
blades. Older engines had stationary vanes in front of the moving blades. These
vanes also helped to direct the air onto the blades. The air flowing into a
turbojet engine is always subsonic, regardless of the speed of the aircraft
itself.
The intake has to supply air to the engine with an acceptably
small variation in pressure (known as distortion) and having lost as little
energy as possible on the way (known as pressure recovery). The ram pressure
rise in the intake is the inlet's contribution to the propulsion
system's overall pressure ratio and thermal efficiency. The
intake gains prominence at high speeds when it generates more compression than
the compressor stage. Well-known examples are the Concorde and Lockheed
SR-71 Blackbird propulsion systems where the intake and engine
contributions to the total compression were 63%/8% at Mach 2 and
54%/17% at Mach 3+. Intakes have ranged from
"zero-length" on Pratt & Whitney
TF33 turbofan installation in the Lockheed C-141 Starlifter, to
the twin 65 feet (20 m) long, intakes on the North American XB-70
Valkyrie, each feeding three engines with an intake airflow of about 800 pounds
per second (360 kg/s).
General Electric J85-GE-17A turbojet engine (1970)
Compressor
The turbine rotates the compressor at high speed, adding
energy to the airflow while squeezing (compressing) it into a smaller space.
Compressing the air increases its pressure and temperature. The
smaller the compressor, the faster it turns. The
(large) GE90-115B fan rotates at about 2,500 RPM, while a small
helicopter engine compressor rotates around 50,000 RPM. Turbojets
supply bleed air from the compressor to the aircraft for the
operation of various sub-systems. Examples include environmental control system, anti-icing,
and fuel tank pressurization. The engine itself needs air at various pressures
and flow rates to keep it running. This air comes from the compressor, and
without it, the turbines would overheat, the lubricating oil would leak from
the bearing cavities, the rotor thrust bearings would skid or be overloaded,
and ice would form on the nose cone.
The air from the compressor, called secondary air, is used
for turbine cooling, bearing cavity sealing, anti-icing, and ensuring that the
rotor axial load on its thrust bearing will not wear it out prematurely.
Supplying bleed air to the aircraft decreases the efficiency of the engine
because it has been compressed, but then does not contribute to producing
thrust. Compressor types used in turbojets were typically axial or centrifugal.
Early turbojet compressors had low pressure ratios up to about 5:1. Aerodynamic
improvements including splitting the compressor into two separately rotating
parts, incorporating variable blade angles for entry guide vanes and stators,
and bleeding air from the compressor enabled later turbojets to have overall
pressure ratios of 15:1 or more. After leaving the compressor, the air enters
the combustion chamber.
Combustion Chamber
The burning process in the combustor is
significantly different from that in a piston engine. In a piston engine,
the burning gases are confined to a small volume, and as the fuel burns, the
pressure increases. In a turbojet, the air and fuel mixture burn in the
combustor and pass through to the turbine in a continuous flowing process with
no pressure build-up. Instead, a small pressure loss occurs in the combustor. The
fuel-air mixture can only burn in slow-moving air, so an area of reverse flow
is maintained by the fuel nozzles for the approximately stoichiometric burning
in the primary zone. Further compressed air is introduced which completes the
combustion process and reduces the temperature of the combustion products to a
level which the turbine can accept. Less than 25% of the air is typically used
for combustion, as an overall lean mixture is required to keep within the
turbine temperature limits.
Turbine
Hot gases leaving the combustor expand through the turbine.
Typical materials for turbines include Inconel and Nimonic. The
hottest turbine vanes and blades in an engine have internal cooling passages.
Air from the compressor is passed through these to keep the metal temperature
within limits. The remaining stages do not need cooling. In the first stage,
the turbine is largely an impulse turbine (similar to a pelton wheel) and
rotates because of the impact of the hot gas stream. Later stages are
convergent ducts that accelerate the gas. Energy is transferred into the shaft
through momentum exchange in the opposite way to energy transfer in the
compressor. The power developed by the turbine drives the compressor and
accessories, like fuel, oil, and hydraulic pumps that are driven by the
accessory gearbox.
Inconel
Nozzle
After the turbine, the gases expand through the exhaust
nozzle producing a high velocity jet. In a convergent nozzle, the ducting
narrows progressively to a throat. The nozzle pressure ratio on a turbojet is
high enough at higher thrust settings to cause the nozzle to choke. If,
however, a convergent-divergent de Laval nozzle is fitted, the
divergent (increasing flow area) section allows the gases to reach supersonic
velocity within the divergent section. Additional thrust is generated by the
higher resulting exhaust velocity.
Thrust Augmentation
Thrust was most commonly increased in turbojets
with water/methanol injection or afterburning. Some engines used
both methods. Liquid injection was tested on the Power Jets W.1 in
1941 initially using ammonia before changing to water and then
water-methanol. A system to trial the technique in the Gloster
E.28/39 was devised but never fitted.
Afterburner
An afterburner or "reheat jetpipe" is a combustion
chamber added to reheat the turbine exhaust gases. The fuel consumption is very
high, typically four times that of the main engine. Afterburners are used
almost exclusively on supersonic aircraft, most being military aircraft.
Two supersonic airliners, Concorde and the Tu-144, also used afterburners
as well as the Scaled Composites White Knight, a carrier aircraft for the
experimental SpaceShipOne suborbital spacecraft,
and the Boom XB-1, an experimental supersonic aircraft. Reheat
was first flight-trialled in 1944 on the W.2/700 engines in
a Gloster Meteor I.
Net Thrust
Cycle Improvements
The operation of a turbojet is modelled approximately by
the Brayton cycle. The efficiency of a gas turbine is increased by raising
the overall pressure ratio, requiring higher-temperature compressor materials,
and raising the turbine entry temperature, requiring better turbine materials
and/or improved vane/blade cooling. It is also increased by reducing the losses
as the flow progresses from the intake to the propelling nozzle. These losses
are quantified by compressor and turbine efficiencies and ducting pressure
losses. When used in a turbojet application, where the output from the gas
turbine is used in a propelling nozzle, raising the turbine temperature
increases the jet velocity. At normal subsonic speeds this reduces the
propulsive efficiency, giving an overall loss, as reflected by the higher fuel
consumption, or SFC. However, for supersonic aircraft this can be
beneficial, and is part of the reason why the Concorde employed turbojets.
Turbojet systems are complex systems therefore to secure optimal function of
such system, there is a call for the newer models being developed to advance
its control systems to implement the newest knowledge from the areas of
automation, so increase its safety and effectiveness.
Turbojet- An Airbreathing Jet Engine, How It Works and Its Evolution
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