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In the family of heat engines, ''Stirling engine'' defines a closed-cycle regenerative hot air engine, though the term is often used incorrectly to refer generically to a much wider range of hot air engine types. In this context, "closed-cycle" means that the working fluid is permanently contained within the system, whereas "open-cycle" engines such as internal combustion engine and some steam engines, exchange working fluid with their surroundings as part of the cycle; "regenerative" refers to the use of an internal heat exchanger - the regenerator - which greatly improves the engine's potential efficiency. There are many possible implementations of the Stirling engine, the majority of which fall into the category of a reciprocating piston engine. The Stirling engine is traditionally classified as an external combustion engine, though heat can equally well be supplied by non-combusting sources such as solar or nuclear energy. A Stirling engine operates through the use of an external heat source and an external heat sink, each maintained within a limited temperature range, and having a sufficiently large temperature difference between them.

Contents

Background

History

Functional Description

The engine cycle

The Stirling cycle

The Regenerator

Engine configurations

Alpha Stirling

Action of an Alpha type Stirling engine

Beta Stirling

Action of a Beta type Stirling engine

Gamma Stirling

Other types

Heat sources

Recent commercial development

Stirling cycle thermodynamics

Advantages of Stirling engines

Disadvantages of Stirling engines

Size and Cost Issues

Power and Torque Issues

Gas Choice Issues

Applications

Combined heat and power applications

Solar power generation

Stirling cryocoolers

Heat pump

Marine engines

Nuclear power

Aircraft engines

Geothermal energy

Low temperature difference engines

Notes

References

Academic References and Non-commercial Research

Academic Computer Tools

Further reading

Commercial manufacturers and suppliers

Commercial Computer Tools

External links

Background

In the conversion of heat into mechanical work, the Stirling engine has the potential to achieve the highest efficiency of any real heat engine, theoretically up to the full Carnot efficiency, though in practice this is limited by non-ideal properties of the working gas and engine materials, such as friction, thermal conductivity, tensile strength, creep, melting point, etc. The engines can run on any heat source of sufficient quality, including solar, chemical and nuclear.
In contrast to internal combustion engines, Stirling engines have the potential to be more energy efficient, quieter, and more reliable with lower maintenance requirements. They are preferred for certain niche applications that value these unique advantages, particularly in cases where the primary objective is ''not'' to minimize the capital cost per unit power ($/kW), but rather to minimize the cost per unit energy generated by the engine ($/kWh). Compared to an internal combustion engine of a given power rating, Stirling engines currently have a higher capital cost and are usually larger and heavier; therefore, the engine technology is rarely competitive on this basis alone. For some applications, however, a proper cost-benefit analysis can favor a Stirling engine over an internal combustion engine.
In recent years, the advantages of Stirling engines have become increasingly significant, given the general rise in energy costs, energy shortages and environmental concerns such as climate change. These growing interests in Stirling technology have fostered the ongoing research and development of Stirling devices. The applications include water pumping, space-based astronautics, and electrical generation from plentiful energy sources that are incompatible with the internal combustion engine, such as solar energy, agricultural waste and domestic refuse.
Another useful characteristic of the Stirling engine is that if supplied with mechanical power, it can function as a heat pump. Experiments have been performed using wind power driving a Stirling cycle heat pump for domestic heating and air conditioning.

History

Stirling's air engine (as it is referred to in early text books - see hot air engine history) was invented by Reverend Dr Robert Stirling and patented by him in 1816. When the name became simplified to Stirling engine is not known, but may be as recently as the mid twentieth century when the Philips company began to experiment with working fluids other than air - the instruction book for their MP1002CA (see below) still refers to it as an 'air engine'. The main subject of that original patent was a heat exchanger which Stirling called the "economiser" for its enhancement of fuel economy in a variety of applications. The patent also described in detail the employment of one form of the economiser in an air engine, in which application it is now commonly known as a regenerator. An engine built by Stirling was put to work pumping water in a quarry in 1818. Subsequent development by Robert Stirling and his brother James, an engineer, resulted in patents for various improved configurations of the original engine, including pressurization which by 1845 had sufficiently increased the power output for it to successfully drive all the machinery at a Dundee iron foundry.
As well as conserving fuel, the inventors sought to create a safer alternative to the steam engines of the time whose boilers occasionally exploded with dire consequences, often including loss of life. However, the need for the Stirling engine to run at a very high temperature to maximise power and efficiency exposed limitations in the materials of the day and the few engines which were built in those early years had rather short and troublesome lives. In particular, 'hot end' failures occurred more frequently than could be tolerated, albeit with far less disastrous results than a steam boiler explosion.
Though it ultimately failed as a competitor to the steam engine in the field of industrial scale prime movers, during the latter nineteenth and early twentieth centuries smaller engines of the Stirling/hot air type (the boundary between the two is often blurred as in many the regenerator is of dubious efficiency or omitted altogether) were produced in large numbers, finding applications wherever a reliable source of low to medium power was required, most commonly perhaps for raising water. These generally operated at lower temperatures so as not to tax available materials and thus tended to be rather inefficient, their major selling point being that in contrast to a steam engine, they could be operated safely by anybody capable of managing the fire in a domestic range. As the century wore on, this role was eventually usurped by the electric motor and small internal combustion engines and by the late 1930s the Stirling engine was a largely forgotten scientific curiosity represented only by toys and a few small ventilating fans.
At this time Philips, the large Dutch electrical and electronic manufacturer, began research into the engine. Seeking to expand the market for its radio sets into areas where mains electricity power was unknown and the supply of short-lived batteries uncertain, Philips’ management decided that what was needed was a low-powered portable generator and tasked a group of engineers at the company research lab (the Nat. Lab) in Eindhoven to investigate the practicalities. Reviewing various prime movers old and new, each was rejected for one reason or another until the Stirling engine was considered. Inherently quiet and capable of running from any heat source (common lamp oil “cheap and available everywhere” was favoured), it seemed to offer real possibilities. Encouraged by their first experimental engine, which produced 16 watts of shaft power from a bore and stroke of 30x25mm, a development program was set in motion.
Remarkably, this work continued throughout World War II and by the late 1940s they had an engine – the Type 10 – which was sufficiently developed to be handed over to Philips’ subsidiary Johan de Witt in Dordrecht to be ‘productionied’ and incorporated into a generator set as originally planned. The set progressed through three prototypes (102A, B, and C), with the production version, rated at 200 watts electrical output from a bore and stroke of 55x27mm, being designated MP1002CA (affectionately known as the 'Bungalow set'). Production of an initial batch began in 1951, but it became clear that they could not be made at a price that the market would support, in addition to which the advent of transistor radios with their much lower power requirements meant that the market for the set was fast disappearing. Though the MP1002CA may have been a dead end, it represents the start of the modern age of Stirling engine development.
Philips went on to develop the Stirling engine for a wide variety of applications including vehicles, but only ever achieved any commercial success with the 'reversed Stirling engine' cryocooler. They did however take out a large number of patents and amass a wealth of information relating to Stirling engine technology, which was later licensed to other companies.
It was also employed in reverse as a heat pump to produce early refrigeration.

Functional Description

The engine cycle

Since the Stirling engine is a closed cycle, it contains a fixed mass of gas called the "working fluid", most commonly air, hydrogen or helium. In normal operation, the engine is sealed and no gas enters or leaves the engine. No valves are required, unlike other types of piston engines. The Stirling engine, like most heat-engines, cycles through four main processes: cooling, compression, heating and expansion. This is accomplished by moving the gas back and forth between hot and cold heat exchangers. The hot heat exchanger is in thermal contact with an external heat source, e.g. a fuel burner, and the cold heat exchanger being in thermal contact with an external heat sink, e.g. air fins. A change in gas temperature will cause a corresponding change in gas pressure, while the motion of the piston causes the gas to be alternately expanded and compressed.
The gas follows the behavior described by the gas laws which describe how a gas's pressure, temperature and volume are related. When the gas is heated, because it is in a sealed chamber, the pressure rises and this then acts on the power piston to produce a power stroke. When the gas is cooled the pressure drops and this means that less work needs to be done by the piston to compress the gas on the return stroke, thus yielding a net power output.
Most high performance Stirling engines are pressurised, that is the mean pressure of the working fluid is above atmospheric pressure. This increases the mass of working fluid processed per cycle, thus, all other things being equal, the engine produces more power. Unfortunately all other things seldom are equal and to realise the potential of pressurisation larger heat exhangers (including the regenerator) are required. This inevitably increases dead space and possibly gas flow resistance, both of which tend to reduce power output. Like most aspects of Stirling engine design, optimisation of this aspect is a delicate balancing act between often conflicting requirements. It was experimenting with pressurisation which initially lead Philips to move from atmospheric air to other gasses for the working fluid. At high temperatures and pressures, the oxygen in air tended to combine with any lubricating oil that made its way past the piston seals, giving problems with clogging the heat exhangers or even the possibility of an explosion. It was later found that some gasses, particularly hydrogen and helium, offered other advantages over air.

When one side of the piston is open to the atmosphere, the operation is slightly different. As the sealed volume of working gas comes in contact with the hot side, it expands, doing work on both the piston and on the atmosphere. When the working gas contacts the cold side, the atmosphere does work on the gas and "compresses" it. Atmospheric pressure, which is greater than the cooled working gas, pushes on the piston.
To summarize, the Stirling engine uses the temperature difference between its hot end and cold end to establish a cycle of a fixed mass of gas expanding and contracting within the engine, thus converting thermal energy into mechanical power. The greater the temperature difference between the hot and cold sources, the greater the potential Carnot cycle efficiency.
Small demonstration engines have been built which will run on a temperature difference of as little as 7 °C, e.g. between the palm of a hand and the surrounding air, or between room temperature and melting water ice.
^{[1]
[2] [3]}

The Stirling cycle

:''For a detailed description see the Stirling cycle thermodynamics section below''
The idealised or "text book" Stirling cycle is a thermodynamic cycle with two isochores and two isotherms. It is the most efficient thermodynamic cycle capable of practical implementation in an engine - its theoretical efficiency equaling that of the hypothetical carnot cycle. However technical issues limit its efficiency when applied - for instance a simpler mechanism may be favored over attaining a close fit to the theoretical cycle.

The Regenerator

The regenerator was the key feature invented by Robert Stirling and its presence or otherwise should be used to distinguish a true Stirling engine from other closed cycle hot air engines. That said, many engines which have no apparent regenerator can still with some justification be called Stirling engines as, in the simple beta and gamma configurations with a 'loose fitting' displacer, the surfaces of the displacer and its cylinder will cyclically exchange heat with the working fluid providing some regenerative effect. This is most often seen in small model and LTD types where the additional flow losses and dead space associated with a separate regenerator could actually prove counterproductive and the 'no regenerator' approach is probably near optimal.
In a stirling engine, the regenerator retains within the system that heat which would otherwise be exchanged with the environment at temperatures intermediate to the maximum and minimum, thus enabling the efficiency of the engine to approach the limiting Carnot efficiency defined by those maxima and minima.
The regenerator is a type of heat exchanger where the flow of a single fluid stream periodically reverses directions - not to be confused with a reverse flow heat exchanger which has two separate streams running in opposite directions. The effect of regeneration in a Stirling engine is to greatly increase the thermal efficiency by 'recycling' heat internally it thus reduces the thermal load on the hot and cold heat exchangers, often allowing an engine to produce higher power with the same set of exchangers.
The ''regenerator'' is typically a mass of fine metal wire, preferably with low porosity to reduce unswept volume (dead space), and with the wire axes perpendicular to the gas flow, as in a stack of wire meshes. The regenerator is located in the path of the gas between the hot and cold heat exchangers. As the gas cycles between the hot and cold spaces, over 90% of its heat is temporarily transferred to and from the regenerator. The regenerator essentially recycles unused heat, and thus reduces the heat flow requirements of the hot and cold heat exchangers.
There is a performance trade off and, particularly for high power density, HTD engines, the regenerator must be carefully designed to obtain high heat transfer with low viscous pumping losses and low dead space. As with the hot and cold exchangers, achieving a successful regenerator is a delicate balancing act between these three conflicting requirements.
Also see: Economiser

Engine configurations

Engineers classify Stirling engines into three distinct types. The Alpha type engine relies on interconnecting the power pistons of multiple cylinders to move the working gas, with the cylinders held at different temperatures. The Beta and Gamma type Stirling engines use a displacer piston to move the working gas back and forth between hot and cold heat exchangers in the same cylinder.

Alpha Stirling

★ An 'alpha Stirling' contains two separate power pistons in separate cylinders, one "hot" piston and one "cold" piston. The hot piston cylinder is situated inside the higher temperature heat exchanger and the cold piston cylinder is situated inside the low temperature heat exchanger. This type of engine has a very high power-to-volume ratio but has technical problems due to the usually high temperature of the "hot" piston and the durability of its seals. (See animation here^[4])

Action of an Alpha type Stirling engine

The following diagrams do not show a regenerator, which would be placed in the pipe connecting the two cylinders. The crankshaft has also been omitted.

1. Most of the working gas is in contact with the hot cylinder walls , it has been heated and expansion has pushed the hot piston to the top of the cylinder. Expansion continues in the cold cylinder piston, which is 90o behind the hot piston in its cycle, extracting still more work from the hot gas.	2. The gas is now at its maximum volume. The hot cylinder piston begins to move most of the gas into the cold cylinder , where it cools and the pressure drops.	Alpha type Stirling. Animated version.
3. Almost all the gas is now in the cold cylinder and cooling continues. The cold piston, powered by flywheel momentum or other piston pairs on the same shaft, compresses the remaining part of the gas.	4. The gas reaches its minimum volume and the hot cylinder piston will now allow it to expand in the hot cylinder where it will be heated once more and drive the hot piston in its power stroke.

Beta Stirling

★ A 'beta Stirling' has a single power piston arranged within the same cylinder on the same shaft as a displacer piston. The displacer piston is a loose fit and does not extract any power from the expanding gas but only serves to shuttle the working gas from the hot heat exchanger to the cold heat exchanger. When the working gas is pushed to the hot end of the cylinder it expands and pushes the power piston. When it is pushed to the cold end of the cylinder it contracts and the momentum of the machine, usually enhanced by a flywheel, pushes the power piston the other way to compress the gas. Unlike the alpha type, the beta type avoids the technical problems of hot moving seals. (See animation here^[5])

Action of a Beta type Stirling engine

A beta Stirling has two pistons within the same cylinder both connected to the same crankshaft. One of these is the tightly fitted power piston and the other a loosely fitted displacement piston.

1. Power piston (dark grey) has compressed the gas, the displacer piston (light grey) has moved so that most of the gas is adjacent to the hot heat exchanger.

2. The heated gas increases its pressure and pushes the power piston along the cylinder. This is the 'power stroke'.

3. The displacer piston now moves to shunt the gas to the cold end of the cylinder.

4. The cooled gas is now compressed by the flywheel momentum. This takes less energy since when it cooled its pressure also dropped.

Beta type Stirling. Animated version. Note the Power piston lags the Displacer piston by 90o. In this design the displacer piston shaft passes through the power piston in a gas proof sleeve.

Gamma Stirling

★ A 'gamma Stirling' is simply a beta Stirling in which the power piston is mounted in a separate cylinder alongside the displacer piston cylinder, but is still connected to the same flywheel. The gas in the two cylinders can flow freely between them but remains a single body. This configuration produces a lower compression ratio but is mechanically simpler and often used in multi-cylinder Stirling engines.

Other types

Changes to the configuration of mechanical Stirling engines continue to interest engineers and inventors. Notably, some are in pursuit of the 'rotary Stirling' engine; the goal here is to convert power from the Stirling cycle directly into torque, a similar goal to that which led to the design of the rotary combustion engine. No practical engine has yet been built but a number of concepts, models and patents have been produced. ^{[6] [7]}
There is also a field of '"free piston" Stirling' cycles engines, including those with liquid pistons and those with diaphragms as pistons.
An alternative to the mechanical Stirling engine is the fluidyne pump, which uses the Stirling cycle via a hydraulic piston. In its most basic form it contains a working gas, a liquid and two non-return valves.
The work produced by the fluidyne goes into pumping the liquid.

Heat sources

Virtually any temperature difference will power a Stirling engine. The heat source may be derived from fuel combustion, hence the term "external combustion engine", although the heat source may also be solar, geothermal, nuclear or even biological. Likewise a "cold source" below the ambient temperature can be used as the temperature difference. (see liquid nitrogen economy). A cold source may be the result of a cryogenic fluid or iced water. In the case where a small temperature differential is used to generate a significant amount of power, large mass flows of heating and cooling fluids must be pumped through the external heat exchangers, thus causing parasitic losses that tend to reduce the efficiency of the cycle.
Because a heat exchanger separates the working gas from the heat source, a wide range of heat sources can be used, including any fuel or waste heat from some other process. Since the combustion products do not contact the internal moving parts of the engine, a Stirling engine can run on landfill gas containing siloxanes without the accumulation of silica that damages internal combustion engines running on this fuel. The life of lubricating oil is longer than for internal-combustion engines.
The U.S. Department of Energy in Washington, NASA Glenn Research Center in Cleveland, and Stirling Technology Co. of Kennewick, Wash., are developing a free-piston Stirling converter for a Stirling Radioisotope Generator. This device would use a plutonium source to supply heat.

Recent commercial development

In the late 1940s, the Philips Electronics company in The Netherlands was searching for a versatile electricity generator to enable worldwide expansion of sales of its electronic devices in areas with no reliable electricity infrastructure. The company put a huge R&D research effort into Stirling engines building on research it had started in the 1930s and which lasted until the 1970s. The only lasting commercial product for Philips was its reversed Stirling engine: the Stirling cryocooler (see below).
Los Alamos National Laboratory has developed an "Acoustic Stirling Heat Engine"
^[8]
with no moving parts. It converts heat into intense acoustic power which (quoted from given source) "can be used directly in acoustic refrigerators or pulse-tube refrigerators to provide heat-driven refrigeration with no moving parts, or ... to generate electricity via a linear alternator or other electroacoustic power transducer".
Think Nordic, an electric car company in Norway, is working with inventor Dean Kamen on plans to install Stirling engines in the Think City, an otherwise all-electric vehicle that will be commercially available at the end of 2007, at least in Europe.

Stirling cycle thermodynamics

The 'ideal' Stirling cycle consists of four thermodynamic processes acting on the working fluid ( See diagram to right):

★ Points 1 to 2, Isothermal Expansion

★ Points 2 to 3, Constant-Volume (aka isometric or isochoric) heat-removal

★ Points 3 to 4, Isothermal Compression

★ Points 4 to 1, Constant-Volume (aka isometric or isochoric) heat-addition
This 'ideal Stirling cycle' is commonly known as a "squared-cycle", because when graphed on a Pressure-Volume plot, the rapid transitions between the processes produce a shape with corners. In a real Stirling engine, physical design constraints limit the net force on each engine component, and thus limit the maximum acceleration (or rate-of-change of velocity). Thus a 'real Stirling cycle' in a Stirling engine requires relatively smooth motion, which is commonly sinusoidal or quasi-sinusoidal. In this case the shape of the PV-plot is quasi-elliptical. Also in a real engine cycle, the heat transfer performance of the heat exchangers ranges from 100% effectiveness in an isothermal process, to 0% effectiveness in an adiabatic process (no heat transfer). The compression and expansion processes can be modeled as a polytropic processes
^[9]


::'',


where 'k' is constant, and 'n' is bounded by:


::.


where $\{c\_V\}$ is the specific heat capacity at constant volume (J/kgK)
and $\{c\_p\}$ is the specific heat capacity at constant pressure (J/kgK)


Compared to the ideal cycle, the efficiency of a real engine is reduced by irreversibilities, friction, and the loss of ''short-circuit'' conducted heat, so that the overall efficiency is often only about half of the ideal (Carnot) efficiency.
^[10]

1. The working gas is heated at a constant volume to a higher temperature. This increases its pressure. (points 4 to 1 on the graph)	2. The working gas expands at a constant temperature to a larger volume. This decreases its pressure. The gas does work to move the piston up. (points 1 to 2 on the graph)	2a. The gas is now fully transferred to the cool cylinder. (Point 2 on the graph)
3. The working gas is cooled at constant volume to a lower temperature. This decreases its pressure. (Points 2 to 3 on the graph)	4. The working gas contracts at a constant temperature to a smaller volume. This increases its pressure. (Points 3 to 4 on the graph)The Piston does work to compress the gas as it moves down. But this is less than that delivered to the piston on cycle 2	4a. The gas is now fully transferred to the hot cylinder. (Point 4 on the graph)

Advantages of Stirling engines

★ Waste heat is relatively easily harvested (compared to waste heat from an internal combustion engine) making Stirling engines useful for dual-output systems such as WhisperGen.

★ They can run directly on any available heat source, not just one produced by combustion, so they can be employed to run on heat from solar, geothermal, biological or nuclear sources.

★ A continuous combustion process can be used to supply heat, so most types of emissions can be greatly reduced.

★ Most types of Stirling engines have the bearing and seals on the cool side of the engine; consequently, they require less lubricant and last significantly longer between overhauls than other reciprocating engine types.

★ The engine mechanisms are in some ways simpler than other types of reciprocating engine types, i.e. no valves are needed, and the fuel burner system can be relatively simple.

★ A Stirling engine uses a single-phase working fluid which maintains an internal pressure close to the design pressure, and thus for a properly designed system the risk of explosion is relatively low. In comparison, a steam engine uses a two-phase gas/liquid working fluid, so a faulty relief valve can cause an over-pressure condition and a potentially dangerous explosion.

★ In some cases, low operating pressure allows the use of lightweight cylinders.

★ They can be built to run very quietly and without an air supply, for air-independent propulsion use in submarines or in space.

★ They start easily (albeit slowly, after a warm-up period) and run more efficiently in cold weather, in contrast to the internal combustion which starts quickly in warm weather, but not in cold weather.

★ A Stirling engine used for pumping water can be configured so that the pumped water cools the compression space. This is, of course, most effective when pumping cold water.

★ They are extremely flexible. They can be used as CHP (Combined Heat and Power) in the winter and as coolers in summers.

Disadvantages of Stirling engines

Size and Cost Issues

★ Stirling engine designs require heat exchangers for heat input and for heat output, and these must contain the pressure of the working fluid, where the pressure is proportional to the engine power output. In addition, the expansion-side heat exchanger is often at very high temperature, so the materials must resist the corrosive effects of the heat source, and have low creep (deformation). Typically these material requirements substantially increase the cost of the engine. The materials and assembly costs for a high temperature heat exchanger typically accounts for 40% of the total engine cost. (Hargraves)

★ All thermodynamic cycles require large temperature differentials for efficient operation; however, in an external combustion engine, the heater temperature always equals or exceeds the expansion temperature. This means that the metallurgical requirements for the heater material are very demanding. This is similar to a Gas turbine, but is in contrast to a Otto engine or Diesel engine, where the expansion temperature can far exceed the metallurgical limit of the engine materials, because the input heat-source is not conducted through the engine; so the engine materials operate closer to the average temperature of the working gas.

★ Dissipation of waste heat is especially complicated because the coolant temperature is kept as low as possible to maximize thermal efficiency. This increases the size of the radiators, which can make packaging difficult. Along with materials cost, this has been one of the factors limiting the adoption of Stirling engines as automotive prime movers. However, for other applications high power density is not required, such as Ship propulsion, and stationary microgeneration systems using combined heat and power (CHP).^[11]

Power and Torque Issues

★ Stirling engines, especially those that run on small temperature differentials, are quite large for the amount of power that they produce (i.e. they have low specific power). This is primarily due to the low heat transfer coefficient of gaseous convection which limits the heat flux that can be attained in an internal heat exchanger to about 4 - 20 W/(m
★ K). This makes it very challenging for the engine designer to transfer heat into and out of the working gas. Increasing the temperature differential and/or pressure allows Stirling engines to produce more power, assuming the heat exchangers are designed for the increased heat load, and can deliver the convected heat flux necessary.

★ A Stirling engine cannot start instantly; it literally needs to "warm up". This is true of all external combustion engines, but the warm up time may be shorter for Stirlings than for others of this type such as steam engines. Stirling engines are best used as constant speed engines.

★ Power output of a Stirling tends to be constant and to adjust it can sometimes require careful design and additional mechanisms. Typically, changes in output are achieved by varying the displacement of the engine (often through use of a swashplate crankshaft arrangement), or by changing the quantity of working fluid, or by altering the piston/displacer phase angle, or in some cases simply by altering the engine load. This property is less of a drawback in hybrid electric propulsion or "base load" utility generation where constant power output is actually desirable.

Gas Choice Issues

★ Hydrogen's low viscosity, high thermal conductivity and specific heat make it the most efficient working gas, in terms of thermodynamics and fluid dynamics, to use in a Stirling engine. However, given the high diffusion rate associated with this low molecular weight gas, hydrogen will leak through solid metal, thus it is very difficult to maintain pressure inside the engine for any length of time without replacement of the gas. Typically, auxiliary systems need to be added to maintain the proper quantity of working fluid. These systems can be a gas storage bottle or a gas generator. Hydrogen can be generated either by electrolysis of water, or by the reaction of acid on metal. Hydrogen can also cause the embrittlement of metals. Hydrogen is also a very flammable gas, while helium is inert.

★ Most technically advanced Stirling engines, like those developed for United States government labs, use helium as the working gas, because it functions close to the efficiency and power density of hydrogen with fewer of the material containment issues. Helium is relatively expensive, and must be supplied by bottled gas.

★ Some engines use air or nitrogen as the working fluid. These gases are less thermodynamically efficient but they minimize the problems of gas containment and supply. The use of Compressed air in contact with flammable materials or substances such as lubricating oil, introduces an explosion hazard, because compressed air contains a high partial pressure of oxygen. However, oxygen can be removed from air through an oxidation reaction, or bottled nitrogen can be used.

Applications

Combined heat and power applications

CHP is an economical source of mechanical or electrical power, which uses a heat source in conjunction with a secondary heating application, usually a pre-existing energy use, such as an industrial process. Usually the primary heat source will enter the Stirling engine heater, since that will usually be at a higher temperature than the heating application, and the "waste" heat from the engine's heater will supply the secondary heating application. The power produced by the engine is often used to run an industrial or agricultural process, which in turn creates biomass waste refuse that can be used as free fuel for the engine, thus reducing waste removal costs. The overall process is very resourceful, thus making it efficient and cost-effective overall.
WhisperGen, a New Zealand firm with offices in Christchurch, has developed an "AC Micro Combined Heat and Power" Stirling cycle engine. These microCHP units are gas-fired central heating boilers which sell power back into the electricity grid. WhisperGen announced in 2004 that they were producing 80,000 units for the residential market in the United Kingdom. A 20 unit trial in Germany started in 2006.

Solar power generation

Placed at the focus of a parabolic mirror a Stirling engine can convert solar energy to electricity with an efficiency better than non-concentrated photovoltaic cells, and comparable to Concentrated Photo Voltaics. On August 11 2005, Southern California Edison announced
^[12]
[13]
over a twenty year period and in quantity (20,000 units) sufficient to generate 500 megawatts of electricity. These systems, on a 4,500 acre (19 km²) solar farm, will use mirrors to direct and concentrate sunlight onto the engines which will in turn drive generators.

Stirling cryocoolers

Any Stirling engine will also work in reverse as a heat pump: i.e. when a motion is applied to the shaft, a temperature difference appears between the reservoirs. One of their modern uses is in refrigeration and cryogenics.
The essential mechanical components of a Stirling cryocooler are identical to a Stirling engine. The turning of the shaft will compress the working gas causing its temperature to rise. This heat will then be dissipated by pushing the gas against a heat exchanger. Heat would then flow from the gas into this heat exchanger which would probably be cooled by passing a flow of air or other fluid over its exterior. The further turning of the shaft will then expand the working gas. Since it had just been cooled the expansion will reduce its temperature even further. The now very cold gas will be pushed against the other heat exchanger and heat would flow from it into the gas. The external side of this heat exchanger would be inside a thermally insulated compartment such as a refrigerator. This cycle would be repeated once for each turn of the shaft. Heat is in effect pumped out of this compartment, through the working gas of the cryocooler and dumped into the environment. The temperature inside the compartment will drop because its insulation prevents ambient heat from coming in to replace that pumped out.
As with the Stirling engine, efficiency is improved by passing the gas through a “Regenerator” which buffers the flow of heat between the hot and cold ends of the gas chamber.
The first Stirling-cycle cryocooler was developed at Philips in the 1950s and commercialized in such places as liquid nitrogen production plants. The Philips Cryogenics business evolved until it was split off in 1990 to form the Stirling Cryogenics & Refrigeration BV
^[14],
The Netherlands. This company is still active in the development and manufacturing Stirling cryocoolers and cryogenic cooling systems.
A wide variety of smaller size Stirling cryocoolers are commercially available for tasks such as the cooling of sensors.
Thermoacoustic refrigeration uses a Stirling cycle in a working gas which is created by high amplitude sound waves.

Heat pump

A Stirling heat pump is very similar to a Stirling cryocooler, the main difference being that it usually operates at room-temperature and its principal application to date is to pump heat from the outside of a building to the inside, thus cheaply heating it.
As with any other Stirling device, heat flows from the expansion space to the compression space; however, in contrast to the Stirling engine, the expansion space is at a lower temperature than the compression space, so instead of producing work, an input of mechanical work is required by the system (in order to satisfy the second law of thermodynamics). When the mechanical work for the heat-pump is provided by a second Stirling engine, then the overall system is called a "heat-driven, heat-pump".
The expansion-side of the heat-pump is thermally coupled to the heat-source, which is often the external environment. The compression side of the Stirling device is placed in the environment to be heated, for example a building, and heat is "pumped" into it. Typically there will be thermal insulation between the two sides so there will be a temperature rise inside the insulated space.
Heat-pumps are by far the most energy-efficient types of heating systems. Stirling heat-pumps also often have a higher coefficient of performance than conventional heat-pumps. To date, these systems have seen limited commercial use; however, use is expected to increase along with market demand for energy conservation, and adoption will likely be accelerated by technological refinements.

Marine engines

Kockums
^[15],
the Swedish shipbuilder, had built at least 8 commercially successful Stirling powered submarines during the 1980s. As of 2005 they have started to carry compressed oxygen with them (see Gotland class submarine).

Nuclear power

There is a potential for nuclear-powered Stirling engines in electric power generation plants. Replacing the steam turbines of nuclear power plants with Stirling engines might simplify the plant, yield greater efficiency, and reduce the radioactive by-products. A number of breeder reactor designs use liquid sodium as coolant. If the heat is to be employed in a steam plant, a water/sodium heat exchanger is required, which raises some concern as sodium reacts violently with water. A Stirling engine obviates the need for water anywhere in the cycle.
United States government labs have developed a modern Stirling engine design known as the Stirling Radioisotope Generator for use in space exploration. It is designed to generate electricity for deep space probes on missions lasting decades. The engine uses a single displacer to reduce moving parts and uses high energy acoustics to transfer energy. The heat source is a dry solid nuclear fuel slug and the cold source is space itself.

Aircraft engines

Stirling engines hold theoretical promise as aircraft engines. They are quieter, less polluting, gain efficiency with altitude, are more reliable due to fewer parts and the absence of an ignition system, produce much less vibration (airframes last longer) and safer, less explosive fuels may be used. (see below "Argument on why the Stirling engine can be applied in aviation" or "Why Aviation Needs the Stirling Engine" by Darryl Phillips, a 4-part series in the March 1993 to March 1994 issues of Stirling Machine World)

Geothermal energy

Some believe that the ability of the Stirling engine to convert geothermal energy to electricity and then to hydrogen may well hold the key to replacement of fossil fuels in a future hydrogen economy.
^[16]
This belief was also founded on research conducted at Los Alamos Labs that began as a hot dry rocks research, but later calculated the near limitless energy potential from molten rock on one side of a Stirling engine and ocean water on the other. Although currently the most feasible source of commercial electrical generation is solar, very long range predictions show advances in deep drilling and development of methods to work with molten rock could yield exponential levels of clean energy generation for thousands of years.

Low temperature difference engines

A low temperature difference (Low Delta T) Stirling engine will run on any low temperature differential, for example the difference between the palm of a hand and room-temperature or room temperature and an ice cube. Usually they are designed in a gamma configuration, for simplicity, and without a regenerator. They are typically unpressurized, running at near-atmospheric pressure. The power produced is less than one watt, and they are intended for demonstration purposes only. They are sold as toys and educational models.

Notes

1. Palm Top Stirling Engine Quote: "...This engine is running on PALMTOP! by using heat of Palm. Then temperature difference of it is 7K..."
2. [ftp://ftp.pasco.com/Support/Documents/English/SE/SE-8575/012-06055A.pdf Pasco model SE-8575: The visible Stirling engine (pdf)]
3. Working cardboard model of a stirling engine (German website translated with translate.google.com)
4. Animation: keveney.com: Two Cylinder Stirling Engine
5. Animation: keveney.com: Single Cylinder Stirling Engine
6. Rotary Stirling Engines This site is intended to assist and support all enthusiasts who work to advance the cause of the Stirling Cycle engine. Accessed October 2006
7. Rotary piston array machine Concept from Gangolf Jobb . Accessed August 2007
8. Los Alamos National Laboratory: Acoustic Stirling Heat Engine Home Quote: "...More Efficient than Other No-Moving-Parts Heat Engines..."
9. David Haywood: An introduction to Stirling-cycle machines (pdf)
10. Israel Urieli (Dr. Iz), Associate Professor Mechanical Engineering: Stirling Cycle Machine Analysis
11. 31 October, 2003, BBC News: Power from the people Quote: "...The boiler is based on the Stirling engine, dreamed up by the Scottish inventor Robert Stirling in 1816....The technical name given to this particular use is Micro Combined Heat and Power or Micro CHP..."
12. PureEnergySystems.com: World's largest solar installation to use Stirling engine technology
an agreement to purchase solar powered Stirling engines from Stirling Energy Systems
13. stirlingenergy.com
14. Stirling Cryogenics & Refrigeration BV
15. kockums.se
16. The American Stirling Company Opinion on Geothermal Energy and the Stirling engine. Accessed December 2006.

References

★ Fundamentals of Classical Thermodynamics SI Version 2nd Ed., Van Wylan, Gordon J. and Sontag, Richard F., , , John Wiley and Sons, , ISBN 0-471-04188-2

★ Free Piston Stirling Cycle Engines, Walker, G., , , Springer-Verlag, , ISBN 0-387-15495-7

★ The Philips Stirling Engine, Hargreaves, C. M., , , Elsevier Publishers, , ISBN 0-444-88463-7

Academic References and Non-commercial Research

★ David Haywood University of Canterbury NZ "Introduction to Stirling-Cycle Analysis" (PDF)

★ Stirling-Cycle Research Group, University of Canterbury NZ

★ Ohio University Israel Urieli

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★ Stirling Engine Simple Analysis

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★ Alpha Stirlings,

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★ Beta Stirlings,

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★ Gamma Stirlings

★ Peter Fette: Stirling Engine Researcher, mirror

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★ Animation,

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★ Regenerator efficiency and simulation

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★ Stirling Engine with 8 cylinders, twice double acting

★ Argument on why the Stirling engine can be applied in aviation, mirror

★ regarding design of a Fluidyne pump 15 pages (pdf)

★ Rotary piston array machine

★ Stirling Engine Design Manual

★ Stirling Engine Research

★ Stirling Engines

Academic Computer Tools

★ Performance Calculator

Further reading

★ A pistonless Stirling engine — The traveling wave heat engine, P. H. Ceperley, , , J. Acoust. Soc. Am.,

★ Thermomechanical generator, a Stirling Engine invented by Cooke-Yarborough

★ Beale Number, used for estimating the power output of a Stirling Engine

★ West Number, used for estimating the power output of a Stirling Engine

★ Fluidyne, a liquid-piston Stirling engine

Commercial manufacturers and suppliers

★ Kontax Stirling Engines - Hand-held Low Temperature differential Stirling engines.

★ ShinyShack.com - Low Temperature and flame driven Stirling engines.

★ Thermal Engine Corporation - Stirling-powered wood stove fan.

★ American Stirling Company - Power Producing Engines

★ Stirling Technology, Inc. - Energy recovery ventilator technology.

★ STM Power - Combined heat and power Stirling engine-generator sets.

★ QRMC - Stirling engine manufacturer.

★ EADS Astrium - Stirling cooler manufacturer for space applications.

★ AIM Infrared Modules - Stirling cooler manufacturer.

★ Carl Aero GmbH - Maker of working model Stirling engines.

★ WhisperGen - Domestic Stirling-engine central heating boilers which generate electricity.

★ Sunpower - "the world's leading developer of free-piston machines."

★ Stirling Energy Systems - Building a 29.4% efficient, 500 MW Stirling energy plant (expandable to 850 MW), using satellite dish compound mirrors, north of Los Angeles. Larger than all other U.S. solar power projects combined.

★ exergia - Solar Stirling Engines

★ Pro Stirling Engines - Stirling Engine Models and Kits.

Commercial Computer Tools

★ SNAP - Stirling Numerical Analysis Program

External links

★ (temporary)

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