Steam Turbine - An Invention & Long Journey
Steam Turbine - An Invention and a Long Journey
A steam turbine is a device that extracts thermal
energy from pressurized dry steam and uses it to do mechanical
work on a rotating output shaft coupled with generator. Its modern
manifestation was invented by Sir Charles Parsons long back in 1884.
Because the turbine generates rotary
motion, it is particularly suited to be used to drive an electrical generator - major percentage of all
electricity generation across the globe is by use of steam turbines. The steam
turbine is a form of heat engine that derives much of its improvement in thermodynamic efficiency through the use
of multiple stages in the expansion of the steam, which results in a closer
approach to the ideal reversible process.
History
The first device that may be classified as a reaction
steam turbine was little more than a toy, the classic Aeolipile,
described in the 1st century by Greek
mathematician Hero of Alexandria in Roman Egypt.
In 1551, Taqi al-Din in Ottoman
Egypt described a steam turbine with the practical application of rotating
a spit. Steam turbines were also described by the
Italian Giovanni Branca (1629) and John
Wilkins in England (1648). The devices described by al-Din and Wilkins are
today known as steam jacks.
The modern steam turbine was invented in 1884 by Sir Charles Parsons, whose first model was
connected to a dynamo
that generated 7.5 kW (10 hp) of electricity. The invention of
Parson's steam turbine made cheap and plentiful electricity possible and revolutionized
marine transport and naval warfare. His patent was licensed and the turbine
scaled-up shortly after by an American, George Westinghouse. The Parsons turbine also
turned out to be easy to scale up. Parsons had the satisfaction of seeing his
invention adopted for all major world power stations, and the size of
generators had increased from his first 7.5 kW set up to units of
50,000 kW capacity. Within Parson's lifetime the generating capacity of a
unit was scaled up by about 10,000 times, and the total output from
turbo-generators constructed by his firm C. A. Parsons and Company and by their
licensees, for land purposes alone, had exceeded thirty million horse-power.
A number of other variations of turbines have been
developed that work effectively with steam. The de Laval turbine (invented by Gustaf
de Laval) accelerated the steam to full speed before running it against a
turbine blade. Hence the (impulse) turbine is simpler, less expensive and does
not need to be pressure-proof. It can operate with any pressure of steam, but
is considerably less efficient.
One of the founders of the modern theory of steam and gas
turbines was also Aurel Stodola, a Slovak physicist and engineer and
professor at Swiss Polytechnical Institute (now ETH) in Zurich. His
mature work was Die Dampfturbinen und
ihre Aussichten als Wärmekraftmaschinen (English: The Steam Turbine and
its perspective as a Heat Energy Machine) which was published in Berlin in
1903. In 1922, in Berlin, was published another important book Dampf und Gas-Turbinen (English:
Steam and Gas Turbines).
The Brown-Curtis
turbine which had been originally developed and patented by the U.S. Company
International Curtis Marine Turbine Company was developed in the 1900s in
conjunction with John Brown & Company. It was used in
John Brown's merchant ships and warships, including liners and Royal Navy
warships.
Types
Steam turbines are made in a variety of sizes ranging
from very small i.e. less than 0.75 kW (less than 1 HP) units (rare) used
as mechanical drives for pumps, compressors and other shaft driven equipment, up
to 1,500,000 kW (2,000,000 HP) very big turbines used to generate
electricity. There are several classifications for modern steam turbines.
Steam supply and exhaust conditions
These types include condensing, non-condensing, reheat,
extraction and induction.
Condensing turbines are most commonly found in electrical
power plants. These turbines exhaust steam in a partially condensed state,
typically of a quality near 90%, at a pressure well below
atmospheric to a condenser.
Non-condensing or back pressure turbines are most widely
used for process steam applications. The exhaust pressure is controlled by a
regulating valve to suit the needs of the process steam pressure. These are
commonly found at power plants of refineries, district heating units, pulp and
paper plants, and desalination facilities where large amounts of low
pressure process steam are available.
Reheat turbines are also used almost exclusively in
electrical power plants. In a reheat turbine, steam leaves from the high
pressure outlet section of the turbine and is returned to the boiler unit where
additional superheat is added. The reheated steam then goes back into an
intermediate pressure section of the turbine and continues its expansion.
Extracting type turbines are common in all applications.
In an extracting type turbine, steam is released from various stages of the
turbine, and used for industrial process needs or sent to boiler feed
water heaters to improve overall cycle efficiency. Extraction flows may be
controlled with a valve, or left uncontrolled.
Induction turbines introduce low pressure steam at an
intermediate stage to produce additional power.
Casing or shaft arrangements
These arrangements include single casing, tandem compound
and cross compound turbines. Single casing units are the most basic style where
a single casing and shaft are coupled to a generator. Tandem compound are used
where two or more casings are directly coupled together to drive a single
generator. A cross compound turbine arrangement features two or more shafts not
in line driving two or more generators that often operate at different speeds.
A cross compound turbine is typically used for many large applications.
Twin-flow Rotors
The steam enters in the middle of
the shaft (butterfly type), expands and exits at each end, balancing the axial
force.
The moving steam imparts both a tangential and axial
thrust on the turbine shaft, but the axial thrust in a simple turbine is
unopposed. To maintain the correct rotor position and balancing, this force
must be counteracted by an opposing force. Either thrust
bearings can be used for the shaft bearings, or the rotor can be designed
so that the steam enters in the middle of the shaft and exits at both ends. The
blades in each half face opposite ways, so that the axial forces negate each
other but the tangential forces act together. This design of rotor is called two-flow
or double-exhaust. This arrangement is common in low-pressure casings of
a compound turbine.
Principle of Operation and Design
An ideal steam turbine is considered to be an isentropic process, or constant entropy process,
in which the entropy of the steam entering the turbine is equal to the entropy
of the steam leaving the turbine. No steam turbine is truly isentropic,
however, with typical isentropic efficiencies ranging from 20–90% based on the
application of the turbine. The interior of a turbine comprises several sets of
blades, or buckets as they are
more commonly referred to. One set of stationary blades is connected to the
casing and one set of rotating blades is connected to the shaft. The sets
intermesh with certain minimum clearances, with the size and configuration of
sets varying to efficiently exploit the expansion of steam at each stage.
Turbine Efficiency
To maximize turbine efficiency the steam is expanded,
doing work, in a number of stages. These stages are characterized by how the
energy is extracted from them and are known as either impulse or reaction
turbines. Most steam turbines use a mixture of the reaction and impulse
designs: each stage behaves as either one or the other, but the overall turbine
uses both. Typically, higher pressure sections are impulse type and lower pressure
stages are reaction type.
Impulse Turbines
An impulse turbine has fixed nozzles that orient the
steam flow into high speed jets. These jets contain significant kinetic energy,
which is converted into shaft rotation by the bucket-like shaped rotor blades,
as the steam jet changes direction. A pressure drop occurs across only the
stationary blades, with a net increase in steam velocity across the stage. As
the steam flows through the nozzle its pressure falls from inlet pressure to
the exit pressure (atmospheric pressure, or more usually, the condenser
vacuum). Due to this high ratio of expansion of steam, the steam leaves the
nozzle with a very high velocity. The steam leaving the moving blades has a
large portion of the maximum velocity of the steam when leaving the nozzle. The
loss of energy due to this higher exit velocity is commonly called the carry
over velocity or leaving loss.
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 time change of angular momentum flux through the
control volume.
Reaction Turbines
In the reaction
turbine, the rotor blades themselves are arranged to form
convergent nozzles.
This type of turbine makes use of the reaction force produced as the steam
accelerates through the nozzles formed by the rotor. Steam is directed onto the
rotor by the fixed vanes of the stator. It leaves the stator as a jet that fills the entire
circumference of the rotor. The steam then changes direction and increases its
speed relative to the speed of the blades. A pressure drop occurs across both
the stator and the rotor, with steam accelerating through the stator and
decelerating through the rotor, with no net change in steam velocity across the
stage but with a decrease in both pressure and temperature, reflecting the work
performed in the driving of the rotor.
Operation and Maintenance
When warming up a steam turbine for use, the main steam
stop valves (after the boiler) have a bypass line to allow superheated steam to
slowly bypass the valve and proceed to heat up the lines in the system along
with the steam turbine. Also, a turning
gear is engaged when there is no steam to the turbine to slowly rotate the
turbine to ensure even heating to prevent uneven expansion. After first
rotating the turbine by the turning gear, allowing time for the rotor to assume
a straight plane (no bowing; minimum eccentricity), then the turning gear automatically
gets disengaged when minimum quantity of steam is admitted to the turbine,
first to the astern blades then to the ahead blades slowly rotating the turbine
at 10 - 15 RPM (0.17 - 0.25 Hz) to allow slow gradual warm up of the
turbine.
Any imbalance of the rotor can lead to vibration, which
in extreme cases can lead to a blade breaking away from the rotor at high
velocity and being ejected directly through the casing. To minimize risk it is
essential that the turbine be very well balanced and turned with dry steam -
that is, superheated steam with minimal liquid water content. If water gets
into the steam and is blasted onto the blades (moisture carry over), rapid
impingement and erosion of the blades can occur leading to imbalance and
catastrophic failure. Also, water entering the blades will result in the
destruction of the thrust bearing for the turbine shaft. To prevent this, along
with controls and baffles in the boilers to ensure high quality steam,
condensate drains are installed in the steam piping leading to the turbine.
Modern designs are sufficiently refined that problems with turbines are rare and
maintenance requirements are relatively small.
Speed Regulation
The control of a turbine with a governor is essential, as
turbines need to be run up slowly, to prevent damage while some applications
(such as the generation of alternating current electricity) require precise
speed control. Uncontrolled acceleration of the turbine rotor can lead to an over
speed trip, which causes the nozzle valves that control the flow of steam to
the turbine to close. If this fails then the turbine may continue accelerating
until it breaks apart, often spectacularly. Turbines are expensive to make,
requiring precision manufacture and special quality materials.
During normal operation in synchronization with the
electricity network, power plants are governed with a five percent droop speed control. This means the full load
speed is 100% and the no-load speed is 105%. This is required for the stable
operation of the network without hunting and drop-outs of power plants.
Normally the changes in speed are minor. Adjustments in power output are made
by slowly raising the droop curve by increasing the spring pressure on a centrifugal governor. Generally this is a
basic system requirement for all power plants because the older and newer
plants have to be compatible in response to the instantaneous changes in
frequency without depending on outside communication.
Thermodynamics of Steam Turbines
The steam turbine operates on basic principles of thermodynamics
using the part of the Rankine cycle. Superheated
vapor (or dry saturated vapor, depending on application) enters the turbine,
after it having exited the boiler, at high temperature and high pressure. The
high heat/pressure steam is converted into kinetic energy using a nozzle (a
fixed nozzle in an impulse type turbine or the fixed blades in a reaction type
turbine). Once the steam has exited the nozzle it is moving at high velocity
and is sent to the blades of the turbine. A force is created on the blades due
to the pressure of the vapor on the blades causing them to move. A generator or
other such device can be placed on the shaft, and the energy that was in the
vapor can now be stored and used. The gas exits the turbine as a saturated
vapor (or liquid-vapor mix depending on application) at a lower temperature and
pressure than it entered with and is sent to the condenser to be cooled.
Isentropic Turbine Efficiency
To measure how well a turbine is performing we can look
at its isentropic
efficiency. This compares the actual performance of the turbine with the
performance that would be achieved by an ideal, isentropic, turbine. When
calculating this efficiency, heat lost to the surroundings is assumed to be
zero. The starting pressure and temperature is the same for both the actual and
the ideal turbines, but at turbine exit the energy content ('specific enthalpy')
for the actual turbine is greater than that for the ideal turbine because of
irreversibility in the actual turbine. The specific enthalpy is evaluated at
the same pressure for the actual and ideal turbines in order to give a good
comparison between the two.
Direct Drive
Electrical power stations use large steam
turbines driving electric generators to produce most (about 80%)
of the world's electricity. The advent of large steam turbines made
central-station electricity generation practical, since reciprocating steam
engines of large rating became very bulky, and operated at slow speeds. Most
central stations are fossil fuel power plants and nuclear power plants; some installations use geothermal
steam, or use concentrated solar power (CSP) to create
the steam. Steam turbines can also be used directly to drive large centrifugal
pumps, such as feed water pumps at a thermal power plant.
The turbines used for electric power generation are most
often directly coupled to their generators. As the generators must rotate at
constant synchronous speeds according to the frequency of the electric power
system, the most common speeds are 3,000 RPM for 50 Hz systems and
3,600 RPM for 60 Hz systems. Since nuclear reactors have lower temperature
limits than fossil-fired plants, with lower steam quality,
the turbine generator sets may be arranged to operate at half these speeds, but
with four-pole generators, to reduce erosion of turbine blades.
Marine Propulsion
In ships, compelling advantages of steam turbines over
reciprocating engines are smaller size, lower maintenance, lighter weight, and
lower vibration. A steam turbine is only efficient when operating in the thousands
of RPM, while the most effective propeller designs are for speeds less than 100
RPM; consequently, precise (thus expensive) reduction gears are usually
required, although several ships, such as Turbinia,
had direct drive from the steam turbine to the propeller shafts. Another
alternative is turbo-electric drive, where an electrical generator
run by the high-speed turbine is used to run one or more slow-speed electric
motors connected to the propeller shafts; precision gear cutting may be a
production bottleneck during wartime. The purchase cost is offset by much lower
fuel and maintenance requirements and the small size of a turbine when compared
to a reciprocating engine having an equivalent power. However, diesel engines
are capable of higher efficiencies: propulsion steam turbine cycle efficiencies
have yet to break 50%, yet diesel engines routinely exceed 50%, especially in
marine applications.
Nuclear-powered ships and submarines use
a nuclear reactor to create steam. Nuclear power is often chosen where diesel
power would be impractical (as in submarine
applications) or the logistics of refuelling pose significant problems (for
example, icebreakers).
It has been estimated that the reactor fuel for the Royal Navy's
Vanguard class submarine is sufficient to
last 40 circumnavigations of the globe – potentially sufficient for the
vessel's entire service life. Nuclear propulsion has only been applied to a
very few commercial vessels due to the expense of maintenance and the
regulatory controls required on nuclear fuel cycles.
Locomotives
A steam turbine locomotive engine is a steam
locomotive driven by a steam turbine.
The main advantages of a steam turbine locomotive are
better rotational balance and reduced hammer blow
on the track. However, a disadvantage is less flexible power output power so
that turbine locomotives were best suited for long-haul operations at a
constant output power.
The first steam turbine rail locomotive was built in 1908
for the Officine Meccaniche Miani Silvestri Grodona Comi, Milan, Italy. In 1924
Krupp built the
steam turbine locomotive T18 001, operational in 1929, for Deutsche Reichsbahn.
Testing
British, German, other national and international test
codes are used to standardize the procedures and definitions used to test steam
turbines. Selection of the test code to be used is an agreement between the
purchaser and the manufacturer, and has some significance to the design of the
turbine and associated systems. ASME has produced several performance test codes on steam
turbines. These include ASME PTC 6-2004, Steam Turbines, ASME PTC 6.2-2011,
Steam Turbines in Combined Cycles, PTC 6S-1988, Procedures for Routine
Performance Test of Steam Turbines. These ASME performance test codes have
gained international recognition and acceptance for testing steam turbines.
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۰ create detailed method statements and inspection criteria
۰ quantify manpower needs to reduce downtime
۰ review special tooling requirements
۰ identify spare parts requirements and manufacture and source these in advance
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Posted
in the Blog on September 9, 2012
