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{{Short description|Type of thermodynamic cycle}}
{{thermodynamics|cTopic=Processes and Cycles}}
[[Image:Ericsson engine4.PNG|thumb|Rendering of an Ericsson engine. A cold gaseous working fluid, such as atmospheric air (shown in blue), enters the cylinder via a [[Non return valve|non-return valve]] at the top-right. The air is compressed by the [[piston]] (black) as the piston moves upward. The compressed air is stored in the pneumatic tank (at left). A two-way valve (gray) moves downward to allow pressurized air to pass through the [[Regenerative heat exchanger|regenerator]] where it is preheated. 

The air then enters the space below the piston, which is an externally heated [[Expansion chamber|expansion-chamber]]. The air expands and does work on the piston as it moves upward. After the expansion stroke, the two-way [[valve]] moves upward, thus closing off the tank and opening the [[exhaust port]]. 

As the piston moves back downward in the exhaust stroke, hot air is pushed back through the [[Regenerative heat exchanger|regenerator]], which reclaims most of the heat, before passing out the exhaust port (left) as cool air.]]

The '''Ericsson cycle''' is named after inventor [[John Ericsson]] who designed and built many unique [[heat engine]]s based on various [[thermodynamic cycle]]s.  He is credited with inventing two unique heat engine cycles and developing practical engines based on these cycles.  His ''first'' cycle is now known as the [[closed Brayton cycle]], while his second cycle is what is now called the Ericsson cycle.
Ericsson is one of the few who built open-cycle engines,<ref name="haeericsson1852">{{cite web|url=http://hotairengines.org/open-cycle-engine/ericsson-1851|title=Ericsson's open-cycle engine of 1852|work=hotairengines.org}}</ref> but he also built closed-cycle ones.<ref name="haeericsson1833">{{cite web|url=http://hotairengines.org/closed-cycle-engine/ericsson-1833|title=Ericsson's closed-cycle engine of 1833|work=hotairengines.org}}</ref>

==Ideal Ericsson cycle==
[[File:Ericsson-Prozess Diagramme.png|thumb|Ideal Ericsson cycle]]
The following is a list of the four processes that occur between the four stages of the ideal Ericsson cycle:
*Process 1 -> 2: [[Isothermal process|Isothermal]] compression.  The compression space is assumed to be [[intercooler|intercooled]], so the gas undergoes isothermal compression. The compressed air flows into a storage tank at constant pressure.  In the ideal cycle, there is no heat transfer across the tank walls.
*Process 2 -> 3: [[Isobaric process|Isobaric]] heat addition.  From the tank, the compressed air flows through the [[Regenerative heat exchanger|regenerator]] and picks up heat at a high constant-pressure on the way to the heated power-cylinder.
*Process 3 -> 4: [[Isothermal process|Isothermal]] expansion.  The power-cylinder expansion-space is heated externally, and the gas undergoes isothermal expansion.
*Process 4 -> 1: Isobaric heat removal.  Before the air is released as exhaust, it is passed back through the regenerator, thus cooling the gas at a low constant pressure, and heating the regenerator for the next cycle.

===Comparison with Carnot, Diesel, Otto, and Stirling cycles===

The ideal [[Otto cycle|Otto]] and [[Diesel cycle|Diesel cycles]] are not totally reversible because they involve heat transfer through a finite temperature difference during the irreversible [[Isochoric process|isochoric]]/[[Isobaric process|isobaric]] heat-addition and isochoric heat-rejection processes. The aforementioned irreversibility renders the [[thermal efficiency]] of these cycles less than that of a [[Carnot engine]] operating within the same limits of temperature. Another cycle that features isobaric heat-addition and heat-rejection processes is the Ericsson cycle. The Ericsson cycle is an altered version of the [[Carnot cycle]] in which the two isentropic processes featured in the Carnot cycle are replaced by two [[Isothermal process|isothermal]] regeneration processes.

The Ericsson cycle is often compared with the [[Stirling cycle]], since the engine designs based on these respective cycles are both [[external combustion engine]]s with [[Regenerative heat exchanger|regenerators]]. The Ericsson is perhaps most similar to the so-called "double-acting" type of Stirling engine, in which the [[displacer]] piston also acts as the power piston.  Theoretically, both of these cycles have so called ''ideal'' efficiency, which is the highest allowed by the [[second law of thermodynamics]].  The most well-known ideal cycle is the [[Carnot cycle]], although a useful ''Carnot engine'' is not known to have been invented.
The theoretical efficiencies for both, Ericsson and Stirling cycles acting in the same limits are equal to the Carnot Efficiency for same limits.

===Comparison with the Brayton cycle===
{{Main|Brayton cycle}}
The first cycle Ericsson developed is now called the "[[Brayton cycle]]", commonly applied to [[gas turbine engine]]s.

The second Ericsson cycle is the cycle most commonly referred to as simply the "Ericsson cycle".  The (second) Ericsson cycle is also the limit of an ideal gas-turbine Brayton cycle, operating with multistage intercooled [[Gas compression|compression]], and multistage expansion with reheat and regeneration.  Compared to the Brayton cycle which uses [[adiabatic compression]] and expansion, the second Ericsson cycle uses isothermal compression and expansion, thus producing more net work per stroke.  Also the use of regeneration in the Ericsson cycle increases efficiency by reducing the required heat input.  For further comparisons of thermodynamic cycles, see [[heat engine]].

{| class="wikitable"
|+
! Cycle/Process !! Compression !! Heat addition  !! Expansion !! Heat rejection
|-
! Ericsson (First, 1833)
|[[Adiabatic process|adiabatic]] || [[Isobaric process|isobaric]] || [[Adiabatic process|adiabatic]] || [[Isobaric process|isobaric]]
|-
! Ericsson (Second, 1853)
|[[isothermal]] || [[Isobaric process|isobaric]] || [[isothermal]] || [[Isobaric process|isobaric]]
|-
! Brayton (Turbine)
|[[Adiabatic process|adiabatic]] || [[Isobaric process|isobaric]] || [[Adiabatic process|adiabatic]] || [[Isobaric process|isobaric]]
|}

==Ericsson engine==

[[File:Ericsson Caloric engine.jpg|thumb|Ericsson Caloric engine]]

[[File:Ericsson Caloric Engine.JPG|thumb|Ericsson Caloric Engine]]
The Ericsson engine is based on the Ericsson cycle, and is known as an "[[external combustion engine]]", because it is externally heated. To improve efficiency, the engine has a [[regenerative heat exchanger|regenerator]] or [[recuperator]] between the compressor and the expander. The engine can be run open- or closed-cycle.  Expansion occurs simultaneously with compression, on opposite sides of the piston.

==Regenerator==
{{Main|Regenerative heat exchanger}}
Ericsson coined the term "regenerator" for his independent invention of the mixed-flow counter-current heat exchanger.  However, Rev. [[Robert Stirling]] had invented the same device, prior to Ericsson, so the invention is credited to Stirling.  Stirling called it an "economiser" or "economizer", because it increased the fuel economy of various types of heat processes.  The invention was found to be useful, in many other devices and systems, where it became more widely used, since other types of engines became favored over the Stirling engine.  The term "regenerator" is now the name given to the component in the Stirling engine.

The term "[[recuperator]]" refers to a separated-flow, counter-current heat exchanger.  As if this weren't confusing enough, a mixed-flow regenerator is sometimes used as a quasi-separated-flow recuperator. This can be done through the use of moving [[valves]], or by a rotating regenerates with fixed baffles, or by the use of other moving parts.  When heat is recovered from exhaust gases and used to preheat combustion air, typically the term recuperator is used, because the two flows are separate.

==History==
In 1791, before Ericsson, [[John Barber (engineer)|John Barber]] proposed a similar engine. The Barber engine used a bellows compressor and a turbine expander, but it lacked a regenerator/recuperator. There are no records of a working Barber engine. Ericsson invented and patented his first engine using an external version of the Brayton cycle in 1833 (number 6409/1833 British). This was 18&nbsp;years before [[James Prescott Joule|Joule]] and 43&nbsp;years before [[George Brayton|Brayton]]. Brayton engines were all piston engines and for the most part, [[internal combustion]] versions of the un-recuperated Ericsson engine. The "[[Brayton cycle]]" is now known as the [[gas turbine]] cycle, which differs from the original "Brayton cycle" in the use of a turbine compressor and expander. The gas turbine cycle is used for all modern gas turbine and [[turbojet]] engines, however simple cycle turbines are often recuperated to improve efficiency and these recuperated turbines more closely resemble Ericsson's work.

Ericsson eventually abandoned the open cycle in favor of the traditional closed Stirling cycle.

Ericsson's engine can easily be modified to operate in a closed-cycle mode, using a second, lower-pressure, cooled container between the original exhaust and intake. In closed cycle, the lower pressure can be significantly above ambient pressure, and He or H<sub>2</sub> working gas can be used. Because of the higher pressure difference between the upward and downward movement of the work-piston, specific output can be greater than of a valveless [[Stirling engine]]. The added cost is the [[valve]]. Ericsson's engine also minimizes mechanical losses: the power necessary for compression does not go through crank-bearing frictional losses, but is applied directly from the expansion force. The piston-type Ericsson engine can potentially be the highest efficiency heat engine arrangement ever constructed. Admittedly, this has yet to be proven in practical applications.{{Citation needed|date=February 2011}}

Ericsson designed and built a very great number of engines running on various cycles including steam, Stirling, Brayton, externally heated diesel air fluid cycle. He ran his engines on a great variety of fuels including coal and solar heat.

Ericsson was also responsible for an early use of the screw [[propeller]] for ship propulsion, in the [[USS Princeton (1843)|USS ''Princeton'']], built in 1842–43.

===Caloric ship ''Ericsson''===
[[File:Caloric Ship Ericsson, burthen 2200 tons, Built for John B Kitching and Associates, A B Lowber, Commander RMG PU6745.jpg|thumb|right|Drawing of ''Ericsson'' ship]]In 1851 the Ericsson-cycle engine (the second of the two discussed here) was used to power a 2,000-ton ship, the caloric ship ''Ericsson'' ({{coord|48.830379|-125.243956|display=inline}}),<ref>{{Cite web |title=HistoricPlaces.ca |url=https://www.historicplaces.ca/en/rep-reg/place-lieu.aspx?id=19306 |access-date=2025-11-17 |website=www.historicplaces.ca}}</ref><ref name="haeericssonship">{{cite web|url=http://hotairengines.org/open-cycle-engine/ericsson-1851/story-of-ericsson-caloric-ship|title=Ericsson's Caloric Ship|work=hotairengines.org}}</ref> and ran flawlessly for 73&nbsp;hours.<ref>{{cite web|url=http://www.genuineideas.com/HallofInventions/SolarPivots/ericssonengine.htm |title=Ericsson Caloric Engine |publisher=Genuineideas.com |access-date=2015-12-15}}</ref> The combination engine produced about {{convert|300|hp}}. It had a combination of four&nbsp;dual-piston engines; the larger expansion piston/cylinder, at {{convert|14|ft}} in diameter, was perhaps the largest piston ever built. Rumor has it that tables were placed on top of those pistons (obviously in the cool compression chamber, not the hot power chamber) and dinner was served and eaten, while the engine was running at full power.{{Citation needed|date=February 2011}} At 6.5&nbsp;[[revolutions per minute|RPM]] the pressure was limited to {{convert|8|psi|abbr=on}}. According to the official report it only consumed 4200&nbsp;kg coal per 24 hours (original target was 8000&nbsp;kg, which is still better than contemporary steam engines). The one [[sea trial]] proved that even though the engine ran well, the ship was underpowered. Some time after the trials, the ''Ericsson'' sank. When it was raised, the Ericsson-cycle engine was removed and a steam engine took its place. The ship was wrecked when blown aground in November 1892 at the entrance to [[Barkley Sound]], British Columbia, Canada.<ref>{{cite web |url=http://www.pacificshipwrecks.ca/english/wrecks.html |title=Graveyard of the Pacific - the Shipwrecks of Vancouver Island |website=www.pacificshipwrecks.ca |access-date=13 January 2022 |archive-url=https://web.archive.org/web/20040710180500/http://www.pacificshipwrecks.ca/english/wrecks.html |archive-date=10 July 2004 |url-status=dead}}</ref>

==Today's potential==

The Ericsson cycle (and the similar Brayton cycle) receives renewed interest<ref>{{cite web|url=http://www.assystem.com/en/markets/projects-detail/36/indeho.html |title=Projects - detail |publisher=Assystem |date=2015-11-18 |access-date=2015-12-15 |url-status=dead |archive-url=https://web.archive.org/web/20151222112555/http://www.assystem.com/en/markets/projects-detail/36/indeho.html |archive-date=2015-12-22 }}</ref> today to extract power from the exhaust heat of gas (and [[producer gas]]) engines and [[Solar concentrator|solar concentrators]].  An important advantage of the Ericsson cycle over the widely known [[Stirling engine]] is often not recognized : the volume of the heat exchanger does not adversely affect the efficiency.

(...)''despite having significant advantages over the Stirling. Amongst them, it is worth to note that the Ericsson engine heat exchangers are not dead volumes, whereas the Stirling engine heat exchangers designer has to face a difficult compromise between as large heat transfer areas as possible, but as small heat exchanger volumes as possible.''<ref>{{cite conference |url=http://www.icrepq.com/icrepq%2713/594-fula.pdf |title=In-Cylinder Heat Transfer in an Ericsson Engine Prototype |vauthors = Fula A, Stouffs P, Sierra F|date=22 March 2013 |location=Bilbao Spain |conference= International Conference on Renewable Energies and Power Quality (ICREPQ’13)}}</ref>

For medium and large engines the cost of valves can be small compared to this advantage. [[Turbocompressor]] plus turbine implementations seem favorable in the MWe range, positive displacement compressor plus turbine for Nx100&nbsp;kWe power, and positive displacement compressor+expander below 100&nbsp;kW. With high temperature [[hydraulic fluid]], both the compressor and the expander can be [[liquid-ring pump]]s even up to 400&nbsp;°C, with rotating casing for best efficiency.

==References==

<references />
* Ericsson's patents. 1833 British and 1851 USA ([https://patents.google.com/patent/US8481 US8481])
* The evolution of the heat engine, by: Ivo Kolin Published Moriya Press, 1972 by Longman
* Hot Air Caloric and Stirling Engines, by: Robert Sier. Published 1999, by L A Mair.
* [https://query.nytimes.com/gst/abstract.html?res=990CE1DB133AE334BC4953DFB5668388649FDE ''New York Times'' 1853-03-01 The Caloric Ship Ericsson - Official Report and Correspondence]

==External links==
{{commons category}}
* 1979 RAND report on a new "Ericsson Cycle Gas Turbine Powerplant" design [http://www.rand.org/pubs/reports/R2327/]
* [http://hotairengines.org Inquiry into the Hot Air Engines of the 19th Century]

{{Thermodynamic cycles|state=uncollapsed}}

[[Category:Thermodynamic cycles]]
[[Category:Piston engines]]