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| {{Short description|Jet engine where combustion takes place in supersonic airflow}} | | {{DISPLAYTITLE:Scramjet}} |
| {{multiple issues|
| | <noinclude>[[Category:Jet engines]]</noinclude> |
| {{Lead too short|date=August 2023}}
| | [[File:Scramjet operation en.svg|thumb|right|300px|Operational layout of a basic scramjet engine.]] |
| {{More footnotes needed|date=November 2022}}
| | [[File:X43a2 nasa scramjet.jpg|thumb|right|300px|Artist’s impression of NASA’s X-43A with scramjet underside.]] |
| }}
| | [[File:Turbo ram scramjet comparative diagram.svg|thumb|right|300px|Turbojet, Ramjet, and Scramjet section comparison.]] |
| {{Use dmy dates|date=October 2021}}
| | [[File:X-43A (Hyper - X) Mach 7 computational fluid dynamic (CFD).jpg|thumb|right|300px|CFD simulation of X-43A in Mach 7 flight.]] |
| [[File:Scramjet operation en.svg|thumb|300px]] | | [[File:SJX61 1EngineTest20070221 TransitionToJP7.jpg|thumb|right|300px|Test firing of a scramjet engine prototype.]] |
| {{Seriesbox aircraft propulsion}}
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| A '''scramjet''' ('''supersonic combustion ramjet''') is a variant of a [[ramjet]] [[airbreathing jet engine]] in which [[combustion]] takes place in [[supersonic]] [[airflow]]. As in ramjets,<ref>{{Cite web|url=https://www.enginehistory.org/Rockets/LorinRamjet/LorinRamjet.shtml|title=Lorin Ramjet|website=www.enginehistory.org}}</ref> a scramjet relies on high vehicle speed to compress the incoming air forcefully before combustion (hence ''ram''jet), but whereas a ramjet decelerates the air to [[speed of sound|subsonic]] velocities before combustion using [[shock cone]]s, a scramjet has no shock cone and slows the airflow using shockwaves produced by its ignition source in place of a shock cone.<ref>''Analysis of Ignition Process in a Scramjet at Low and High Fueling Rates'', Gareth Dunlap, Elias Fekadu, Ben Grove, Nick Gabsa, Kenneth Yu, Camilo Munoz, Jason Burr.</ref> This allows the scramjet to operate efficiently at extremely high speeds.<ref>{{cite journal |title=Supersonic combustion in air-breathing propulsion systems for hypersonic flight. |journal=[[Annual Review of Fluid Mechanics]] |year=2018 |last=Urzay |first=Javier |volume=50 |issue= 1|pages=593–627 |doi=10.1146/annurev-fluid-122316-045217|bibcode=2018AnRFM..50..593U |doi-access=free }}</ref>
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| Although scramjet engines have been used in a handful of operational military vehicles, scramjets have so far mostly been demonstrated in research test articles and experimental vehicles.
| | == Overview == |
| | A '''scramjet''' (supersonic combustion ramjet) is a type of airbreathing jet engine in which combustion occurs in a supersonic airflow. Unlike ramjets, scramjets do not slow the incoming air to subsonic speeds prior to combustion. This design enables more efficient propulsion at hypersonic velocities, typically above Mach 5. |
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| ==History== | | == Design and Principles == |
| | Scramjets are mechanically simple—no moving parts. They consist of an intake, a combustion chamber, and a nozzle. The engine compresses incoming high-speed air, mixes it with onboard fuel (typically hydrogen), ignites it, and accelerates the exhaust through a nozzle to generate thrust. This process relies entirely on the vehicle’s forward speed to compress air. |
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| ===Before 2000=== | | == History == |
| The [[Bell X-1]] attained [[Supersonic speed#Supersonic flight|supersonic flight]] in 1947 and, by the early 1960s, rapid progress toward faster aircraft suggested that operational aircraft would be flying at "hypersonic" speeds within a few years. Except for specialized rocket research vehicles like the [[North American X-15]] and other rocket-powered [[spacecraft]], aircraft top speeds have remained level, generally in the range of Mach{{nbsp}}1 to Mach{{nbsp}}3. | | === Early Concepts === |
| | The concept was born from ramjet experimentation during the mid-20th century. Antonio Ferri demonstrated net thrust in 1964. The 1980s saw successful ground tests in Australia and Russia. In 1991, the first successful scramjet flight occurred over the Soviet Union via the CIAM-NASA collaboration. |
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| During the US aerospaceplane program, between the 1950s and the mid 1960s, [[Alexander Kartveli]] and [[Antonio Ferri]] were proponents of the scramjet approach.
| | === Breakthroughs and Flight Tests === |
| | Key developments include: |
| | * NASA X-43A achieving Mach 9.6 (2004) |
| | * DARPA’s HAWC cruise missile flights (2021–2022) |
| | * India's Hypersonic Technology Demonstrator Vehicle (2019) |
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| In the 1950s and 1960s, a variety of experimental scramjet engines were built and ground tested in the US and the UK. Antonio Ferri successfully demonstrated a scramjet producing net thrust in November 1964, eventually producing 517 pounds-force (2.30 kN), about 80% of his goal. In 1958, an analytical paper discussed the merits and disadvantages of supersonic combustion ramjets.<ref name="weber">{{cite journal|last1=Weber|first1=Richard J.|last2=Mackay|first2=John S.|title=An Analysis of Ramjet Engines Using Supersonic Combustion|url=https://ntrs.nasa.gov/search.jsp?R=19930085282&hterms=weber+mackay&qs=N%3D0%26Ntk%3DAll%26Ntt%3Dweber%2520mackay%26Ntx%3Dmode%2520matchallpartial%26Nm%3D123%7CCollection%7CNASA%2520STI%7C%7C17%7CCollection%7CNACA|website=ntrs.nasa.gov|date=September 1958|publisher=NASA Scientific and Technical Information|access-date=3 May 2016}}</ref> In 1964, [[Frederick S. Billig]] and Gordon L. Dugger submitted a patent application for a supersonic combustion ramjet based on Billig's PhD thesis. This patent was issued in 1981 following the removal of an order of secrecy.<ref name="UMD">{{cite web |url=http://www.eng.umd.edu/ihof/inductees/billig.html |title=Frederick S. Billig, Ph.D. |work=The Clark School Innovation Hall of Fame |publisher=[[University of Maryland]] |archive-url=https://web.archive.org/web/20100609221913/http://www.eng.umd.edu/ihof/inductees/billig.html |archive-date=9 June 2010 |access-date=30 April 2010 }}</ref>
| | == Operating Characteristics == |
| | * Operates efficiently between Mach 5 and Mach 15 |
| | * No need to carry onboard oxidizer (unlike rockets) |
| | * Requires high-speed booster (rocket or turbojet) to initiate airflow conditions |
| | * High specific impulse (1000–4000 seconds) |
| | * No moving parts = fewer mechanical failure points |
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| In 1981, tests were made in Australia under the guidance of Professor Ray Stalker in the T3 ground test facility at ANU.<ref name="aus">{{cite news |url=https://www.uq.edu.au/news/article/2002/07/milestones-history-of-scramjets |title=Milestones in the history of scramjets |work=UQ News |publisher=[[University of Queensland]] |date=27 July 2002 |url-status=live |archive-url=https://web.archive.org/web/20160211221907/https://www.uq.edu.au/news/article/2002/07/milestones-history-of-scramjets |archive-date=11 February 2016 |access-date=11 February 2016 }}</ref>
| | == Challenges == |
| | * Sustaining combustion in supersonic flow is technically complex |
| | * Requires high-temperature materials and active cooling systems |
| | * Testing and development are extremely expensive |
| | * Lower thrust-to-weight ratio than rockets (typically around 2:1) |
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| The first successful flight test of a scramjet was performed as a joint effort with [[NASA]], over the Soviet Union in 1991. It was an axisymmetric hydrogen-fueled dual-mode scramjet developed by [[Central Institute of Aviation Motors]] (CIAM), Moscow in the late 1970s, but modernized with a FeCrAl alloy on a converted SM-6 missile to achieve initial flight parameters of Mach 6.8, before the scramjet flew at Mach 5.5. The scramjet flight was flown captive-carry atop the [[S-200 (missile)|SA-5]] [[surface-to-air missile]] that included an experimental flight support unit known as the "Hypersonic Flying Laboratory" (HFL), "Kholod".<ref>{{cite book |last1=Roudakov |first1=Alexander S. |last2=Schickhmann |first2=Y. |last3=Semenov |first3=Vyacheslav L. |last4=Novelli |first4=Ph. |last5=Fourt |first5=O. |title=44th Congress of the International Astronautical Federation |chapter=Flight Testing an Axisymmetric Scramjet – Recent Russian Advances |volume=10 |location=Graz, Austria |publisher=International Astronautical Federation |year=1993 }}</ref>
| | == Applications == |
| | Scramjets are being explored for: |
| | * Hypersonic cruise missiles |
| | * Rapid point-to-point transport |
| | * Single-stage-to-orbit (SSTO) reusable spacecraft |
| | * Military strike platforms |
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| Then, from 1992 to 1998, an additional six flight tests of the axisymmetric high-speed scramjet-demonstrator were conducted by CIAM together with France and then with [[NASA]].<ref name="AIAA 96-4572">{{cite web |url=http://www.nasa.gov/centers/dryden/pdf/88431main_H-2115.pdf |title=Future Flight Test Plans of an Axisymmetric Hydrogen-Fueled Scramjet Engine on the Hypersonic Flying Laboratory |last1=Roudakov |first1=Alexander S. |last2=Semenov |first2=Vyacheslav L. |last3=Kopchenov |first3=Valeriy I. |last4=Hicks |first4=John W. |work=7th International Spaceplanes and Hypersonics Systems & Technology Conference November 18–22, 1996/Norfolk, Virginia |publisher=[[AIAA]] |date=1996 |url-status=live |archive-url=https://web.archive.org/web/20160212141135/http://www.nasa.gov/centers/dryden/pdf/88431main_H-2115.pdf |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref><ref name="NASA/TP-1998-206548">{{cite web |url=http://www.nasa.gov/centers/dryden/pdf/88580main_H-2243.pdf |title=Recent Flight Test Results of the Joint CIAMNASA Mach 6.5 Scramjet Flight Program |last1=Roudakov |first1=Alexander S. |last2=Semenov |first2=Vyacheslav L. |last3=Hicks |first3=John W. |work=Central Institute of Aviation Motors, Moscow, Russia/NASA Dryden Flight Research Center Edwards, California, USA |publisher=[[NASA]] Center for AeroSpace Information (CASI) |date=1998 |url-status=live |archive-url=https://web.archive.org/web/20160212144411/http://www.nasa.gov/centers/dryden/pdf/88580main_H-2243.pdf |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref> Maximum flight speed greater than Mach{{nbsp}}6.4 was achieved and scramjet operation during 77 seconds was demonstrated. These flight test series also provided insight into autonomous hypersonic flight controls.
| | == See Also == |
| | | * [[Ramjet]] |
| ===2000s===
| | * [[Hypersonic flight]] |
| {{Main|Scramjet programs}}
| | * [[Airbreathing engines]] |
| [[File:X43a2 nasa scramjet.jpg|thumb|Artist's conception of the [[NASA X-43]] with scramjet attached to the underside|alt=Artist's conception of black, wingless jet with pointed nose profile and two vertical stabilizers traveling high in the atmosphere.]]
| | * [[NASA X-43]] |
| | | * [[HAWC (DARPA)]] |
| In the 2000s, significant progress was made in the development of hypersonic technology, particularly in the field of scramjet engines.
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| The [[HyShot]] project demonstrated scramjet combustion on 30 July 2002. The scramjet engine worked effectively and demonstrated supersonic combustion in action. However, the engine was not designed to provide thrust to propel a craft. It was designed more or less as a technology demonstrator.<ref name="AIAA-44-10-2366">{{cite journal |title=Flight Data Analysis of the HyShot 2 Scramjet Flight Experiment |journal=AIAA Journal |year=2006 |last1=Smart |first1=Michael K. |last2=Hass |first2=Neal E. |last3=Paull |first3=Allan |volume=44 |issue=10 |pages=2366–2375 |issn=0001-1452 |doi=10.2514/1.20661|bibcode=2006AIAAJ..44.2366S }}</ref>
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| A joint British and Australian team from UK defense company [[Qinetiq]] and the [[University of Queensland]] were the first group to demonstrate a scramjet working in an atmospheric test.<ref name="1001 inventions">{{cite book |last1=Challoner |first1=Jack |title=1001 Inventions That Changed the World |location=London |publisher=[[Cassell Illustrated]] |date=2 February 2009 |page=932 |isbn=978-1-84403-611-0 }}</ref>
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| [[Hyper-X]] claimed the first flight of a thrust-producing scramjet-powered vehicle with full aerodynamic maneuvering surfaces in 2004 with the [[NASA X-43|X-43A]].<ref name="AIAA 2005-3334">{{cite book|title=AIAA/CIRA 13th International Space Planes and Hypersonics Systems and Technologies Conference|last1=Harsha|first1=Philip T.|last2=Keel|first2=Lowell C.|last3=Castrogiovanni|first3=Anthony|last4=Sherrill|first4=Robert T.|date=17 May 2005|publisher=[[AIAA]]|isbn=978-1-62410-068-0|location=[[Capua]], Italy|chapter=2005-3334: X-43A Vehicle Design and Manufacture|doi=10.2514/6.2005-3334}}</ref><ref name="X-43 McClinton">{{cite web |url=https://info.aiaa.org/tac/pc/HYTAPC/Shared%20Documents/Meeting%20Presentations/2006%20ASM/AIAA_DL_McClinton.pdf |title=X-43: Scramjet Power Breaks the Hypersonic Barrier |last=McClinton |first=Charles |publisher=[[AIAA]] |date=9 January 2006 |url-status=live |archive-url=https://web.archive.org/web/20160212152951/https://info.aiaa.org/tac/pc/HYTAPC/Shared%20Documents/Meeting%20Presentations/2006%20ASM/AIAA_DL_McClinton.pdf |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref> The last of the three X-43A scramjet tests achieved Mach{{nbsp}}9.6 for a brief time.<ref>{{Cite web|url=https://www.nasa.gov/news-release/nasas-x-43a-scramjet-breaks-speed-record/|title=NASA – NASA's X-43A Scramjet Breaks Speed Record|website=www.nasa.gov|language=en|access-date=13 June 2019}}</ref>
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| On 15 June 2007, the US Defense Advanced Research Project Agency ([[DARPA]]), in cooperation with the Australian Defence Science and Technology Organisation (DSTO)<!--Please note that "Defence" and "Defense" are different for the US and Australian organizaions/organisations respectively -->, announced a successful scramjet flight at Mach{{nbsp}}10 using rocket engines to boost the test vehicle to hypersonic speeds.<ref name="NewSc 15-06-2007">{{cite news |url=https://www.newscientist.com/article/dn12075-scramjet-hits-mach-10-over-australia-/ |title=Scramjet hits Mach{{nbsp}}10 over Australia |work=[[New Scientist]] |publisher=[[Reed Business Information]] |date=15 June 2007 |url-status=live |archive-url=https://web.archive.org/web/20160212154205/https://www.newscientist.com/article/dn12075-scramjet-hits-mach-10-over-australia-/ |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref><ref>{{Citation |last=Ballard |first=Terry |title=Google Maps and Google Earth |date=2012 |url=http://dx.doi.org/10.1016/b978-1-84334-677-7.50009-7 |work=Google This! |pages=113–124 |access-date=2023-06-02 |publisher=Elsevier|doi=10.1016/b978-1-84334-677-7.50009-7 |isbn=9781843346777 }}</ref>
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| A series of scramjet ground tests was completed at [[NASA]] [[Langley Research Center|Langley]] Arc-Heated Scramjet Test Facility (AHSTF) at simulated [[Mach number|Mach]]{{nbsp}}8 flight conditions. These experiments were used to support HIFiRE flight 2.<ref name="NTRS">{{cite conference |last1=Cabell |first1=Karen |last2=Hass |first2=Neal |last3=Storch |first3=Andrea |last4=Gruber |first4=Mark |date=11 April 2011 |title=HIFiRE Direct-Connect Rig (HDCR) Phase I Scramjet Test Results from the NASA Langley Arc-Heated Scramjet Test Facility |conference=17th AIAA International Space Planes and Hypersonic Systems and Technologies Conference |website=NASA Technical Reports Server |hdl=2060/20110011173 |hdl-access=free}}</ref>
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| On 22 May 2009, Woomera hosted the first successful test flight of a hypersonic aircraft in HIFiRE (Hypersonic International Flight Research Experimentation). The launch was one of ten planned test flights. The series of flights is part of a joint research program between the Defence Science and Technology Organisation and the US Air Force, designated as the HIFiRE.<ref name="dailytelegraph.com.au">{{cite news |last=Dunning |first=Craig |url=http://www.dailytelegraph.com.au/woomera-hosts-first-hifire-hypersonic-test-flight/story-e6frewsr-1225715365056 |title=Woomera hosts first HIFiRE hypersonic test flight |work=[[The Daily Telegraph (Sydney)|The Daily Telegraph]] |publisher=[[News Corp Australia]] |date=24 May 2009 |access-date=12 February 2016 |archive-date=August 28, 2014|archive-url=https://archive.today/20140828195858/http://www.dailytelegraph.com.au/woomera-hosts-first-hifire-hypersonic-test-flight/story-e6frewsr-1225715365056}}</ref> HIFiRE is investigating hypersonics technology and its application to advanced scramjet-powered space launch vehicles; the objective is to support the new [[Boeing X-51]] scramjet demonstrator while also building a strong base of flight test data for quick-reaction space launch development and hypersonic "quick-strike" weapons.<ref name="dailytelegraph.com.au"/>
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| ===2010s===
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| On 22 and 23 March 2010, Australian and American defense scientists successfully tested a (HIFiRE) hypersonic rocket. It reached an atmospheric speed of "more than 5,000 kilometres per hour" (Mach{{nbsp}}4) after taking off from the [[Woomera Test Range]] in outback South Australia.<ref name="SMH 2010-03-22">{{cite news |last=AAP |author-link=Australian Associated Press |url=http://www.smh.com.au//breaking-news-national/scientists-conduct-second-hifire-test-20100322-qqrp.html |title=Scientists conduct second HIFiRE test |work=[[The Sydney Morning Herald]] |publisher=[[Fairfax Media]] |date=22 March 2010 |url-status=live |archive-url=https://web.archive.org/web/20160212160428/http://www.smh.com.au//breaking-news-national/scientists-conduct-second-hifire-test-20100322-qqrp.html |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref><ref name="AuBC 2010-03-23">{{cite news |url=http://www.abc.net.au/news/2010-03-23/success-for-hypersonic-outback-flight/375654 |title=Success for hypersonic outback flight |work=ABC News |publisher=[[Australian Broadcasting Corporation|ABC]] |date=23 March 2010 |url-status=live |archive-url=https://web.archive.org/web/20160212161059/http://www.abc.net.au/news/2010-03-23/success-for-hypersonic-outback-flight/375654 |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| On 27 May 2010, [[NASA]] and the [[United States Air Force]] successfully flew the [[Boeing X-51|X-51A Waverider]] for approximately 200 seconds at Mach{{nbsp}}5, setting a new world record for flight duration at hypersonic airspeed.<ref>{{cite web|title=Longest Flight at Hypersonic Speed|url=http://www.guinnessworldrecords.com/world-records/longest-flight-at-hypersonic-speed|website=Guinness World Records|archive-url=https://web.archive.org/web/20170706212226/http://www.guinnessworldrecords.com/world-records/longest-flight-at-hypersonic-speed|archive-date=6 July 2017 |access-date=6 July 2017 }}</ref> The Waverider flew autonomously before losing acceleration for an unknown reason and destroying itself as planned. The test was declared a success. The X-51A was carried aboard a [[B-52]], accelerated to Mach{{nbsp}}4.5 via a solid rocket booster, and then ignited the [[Pratt & Whitney]] Rocketdyne scramjet engine to reach Mach{{nbsp}}5 at {{convert|70000|ft|m}}.<ref name="CNET 2010-05-26">{{cite news |last=Skillings |first=Jon |url=http://www.cnet.com/news/x-51a-races-to-hypersonic-record/ |title=X-51A races to hypersonic record |work=[[CNET]] |publisher=[[CBS Interactive]] |date=26 May 2010 |url-status=live |archive-url=https://web.archive.org/web/20160212161352/http://www.cnet.com/news/x-51a-races-to-hypersonic-record/ |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref> However, a second flight on 13 June 2011 was ended prematurely when the engine lit briefly on ethylene but failed to transition to its primary [[JP-7]] fuel, failing to reach full power.<ref name="Space.com 2011-07-29">{{cite news |url=http://www.space.com/12441-hypersonic-x51a-waverider-scramjet-failure.html |title=Hypersonic X-51A Scramjet Failure Perplexes Air Force |work=[[Space.com]] |publisher=[[Purch]] |date=27 July 2011 |url-status=live |archive-url=https://web.archive.org/web/20160212161955/http://www.space.com/12441-hypersonic-x51a-waverider-scramjet-failure.html |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| On 16 November 2010, Australian scientists from the [[Australian Defence Force Academy#Academic education|University of New South Wales at the Australian Defence Force Academy]] successfully demonstrated that the high-speed flow in a naturally non-burning scramjet engine can be ignited using a pulsed laser source.<ref name="AuBC 2010-11-16">{{cite news |last=Cooper |first=Dani |url=http://www.abc.net.au/science/articles/2010/11/16/3067887.htm |title=Researchers put spark into scramjets |work=ABC Science |publisher=[[Australian Broadcasting Corporation|ABC]] |date=16 November 2010 |access-date=12 February 2016 }}</ref>
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| A further [[Boeing X-51|X-51A Waverider]] test failed on 15 August 2012. The attempt to fly the scramjet for a prolonged period at Mach{{nbsp}}6 was cut short when, only 15 seconds into the flight, the X-51A craft lost control and broke apart, falling into the Pacific Ocean north-west of Los Angeles. The cause of the failure was blamed on a faulty control fin.<ref name="BBC 2012-08-15">{{cite news |url=https://www.bbc.com/news/technology-19277620 |title=Hypersonic jet Waverider fails Mach 6 test |work=[[BBC News]] |publisher=[[BBC]] |date=15 August 2012 |url-status=live |archive-url=https://web.archive.org/web/20160212163058/http://www.bbc.com/news/technology-19277620 |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| In May 2013, an X-51A Waverider reached 4828 km/h (Mach{{nbsp}}3.9) during a three-minute flight under scramjet power. The WaveRider was dropped at {{convert|50000|ft|m}} from a B-52 bomber, and then accelerated to Mach{{nbsp}}4.8 by a solid rocket booster which then separated before the WaveRider's scramjet engine came into effect.<ref name="2013-05-smh">{{cite news |last=AP |author-link=Associated Press |url=http://www.smh.com.au/technology/sci-tech/experimental-hypersonic-aircraft-hits-4828-kmh-20130506-2j2e6.html |title=Experimental hypersonic aircraft hits 4828 km/h |work=[[The Sydney Morning Herald]] |publisher=[[Fairfax Media]] |date=6 May 2013 |url-status=live |archive-url=https://web.archive.org/web/20160212163341/http://www.smh.com.au/technology/sci-tech/experimental-hypersonic-aircraft-hits-4828-kmh-20130506-2j2e6.html |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| On 28 August 2016, the Indian space agency [[Indian Space Research Organisation|ISRO]] conducted a successful test of a scramjet engine on a two-stage, solid-fueled rocket. Twin scramjet engines were mounted on the back of the second stage of a two-stage, solid-fueled [[sounding rocket]] called [[Advanced Technology Vehicle]] (ATV), which is ISRO's advanced sounding rocket. The twin scramjet engines were ignited during the second stage of the rocket when the ATV achieved a speed of 7350 km/h (Mach{{nbsp}}6) at an altitude of 20 km. The scramjet engines were fired for a duration of about 5 seconds.<ref name="Firstpost 2016">{{cite web | title=Scramjet engines successfully tested: All you need to know about Isro's latest feat | website=Firstpost | date=28 August 2016 | url=http://www.firstpost.com/india/scramjet-engines-successfully-tested-all-you-need-to-know-about-isros-latest-feat-2979992.html | access-date=28 August 2016}}</ref><ref>{{cite web|url=http://www.isro.gov.in/update/28-aug-2016/successful-flight-testing-of-isros-scramjet-engine-technology-demonstrator|title=Successful Flight Testing of ISRO's Scramjet Engine Technology Demonstrator – ISRO|website=www.isro.gov.in|archive-date=December 1, 2017|archive-url=https://web.archive.org/web/20171201182039/http://www.isro.gov.in/update/28-aug-2016/successful-flight-testing-of-isros-scramjet-engine-technology-demonstrator}}</ref>
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| On 12 June 2019, India successfully conducted the maiden flight test of its indigenously developed uncrewed scramjet demonstration aircraft for hypersonic speed flight from a base from [[Abdul Kalam Island]] in the [[Bay of Bengal]] at about 11:25 am. The aircraft is called the [[Hypersonic Technology Demonstrator Vehicle]]. The trial was carried out by the [[Defence Research and Development Organisation]]. The aircraft forms an important component of the country's programme for development of a hypersonic [[cruise missile]] system.<ref>{{Cite journal|date=12 June 2019|title=India successfully conducts flight test of unmanned scramjet demonstration aircraft|url=https://timesofindia.indiatimes.com/india/india-successfully-conducts-flight-test-of-unmanned-scramjet-demonstration-aircraft/articleshow/69753799.cms?from=mdr|journal=The Times of India}}</ref><ref>{{Cite journal|date=12 June 2019|title=India test fires Hypersonic Technology Demonstrator Vehicle|url=https://www.business-standard.com/article/news-ians/india-test-fires-hypersonic-technology-demonstrator-vehicle-119061200454_1.html|journal=Business Standard}}</ref>
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| ===2020s===
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| On 27 September 2021, DARPA announced successful flight of its [[Hypersonic Air-breathing Weapon Concept]] scramjet [[cruise missile]].<ref name="DARPA 2021-09-27">{{cite news |url=https://www.darpa.mil/news-events/2021-09-27 |title= DARPA'S Hypersonic Air-breathing Weapon Concept (HAWC) Achieves Successful Flight |work=[[DARPA]] press release |publisher=[[DARPA]] |date=27 September 2021 }}</ref> Another successful test was carried out in mid-March 2022 amid the [[2022 Russian invasion of Ukraine|Russian invasion of Ukraine]]. Details were kept secret to avoid escalating tension with [[Russia]], only to be revealed by an unnamed [[The Pentagon|Pentagon]] official in early April.<ref>{{Cite web|url=https://www.cnn.com/2022/04/04/politics/us-hypersonic-missile-test/index.html|title = US tested hypersonic missile in mid-March but kept it quiet to avoid escalating tensions with Russia|website = [[CNN]]| date=5 April 2022 }}</ref><ref>{{Cite web | title=Second Successful Flight for DARPA Hypersonic Air-breathing Weapon Concept (HAWC) | url=https://www.darpa.mil/news-events/2022-04-05 | access-date=2025-01-11 | website=www.darpa.mil}}</ref>
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| == Design principles ==
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| Scramjet engines are a type of jet engine, and rely on the combustion of fuel and an oxidizer to produce thrust. Similar to conventional jet engines, scramjet-powered aircraft carry the fuel on board, and obtain the oxidizer by the ingestion of atmospheric oxygen (as compared to [[rockets]], which carry both fuel and an [[oxidizing agent]]). This requirement limits scramjets to suborbital atmospheric propulsion, where the oxygen content of the air is sufficient to maintain combustion.
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| The scramjet is composed of three basic components: a converging inlet, where incoming air is compressed; a combustor, where gaseous fuel is burned with atmospheric [[oxygen]] to produce heat; and a diverging nozzle, where the heated air is accelerated to produce [[thrust]].<ref name=":0">{{Cite web |last=LaRC |first=Bob Allen |title=NASA - How Scramjets Work |url=https://www.nasa.gov/centers/langley/news/factsheets/X43A_2006_5.html |access-date=2022-12-02 |website=www.nasa.gov |language=en |archive-date=2 December 2022 |archive-url=https://web.archive.org/web/20221202230846/http://www.nasa.gov/centers/langley/news/factsheets/X43A_2006_5.html |url-status=dead }}</ref> Unlike a typical jet engine, such as a [[turbojet]] or [[turbofan]] engine, a scramjet does not use rotating, fan-like components to compress the air; rather, the achievable speed of the aircraft moving through the atmosphere causes the air to compress within the inlet.<ref name=":0" /> As such, no [[moving parts]] are needed in a scramjet. In comparison, typical turbojet engines require multiple stages of rotating [[axial-flow compressor|compressor rotors]], and multiple rotating [[turbine]] stages, all of which add weight, complexity, and a greater number of failure points to the engine.
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| Due to the nature of their design, scramjet operation is limited to near-[[hypersonic]] velocities. As they lack mechanical compressors, scramjets require the high [[kinetic energy]] of a hypersonic flow to compress the incoming air to operational conditions. Thus, a scramjet-powered vehicle must be accelerated to the required velocity (usually about Mach{{nbsp}}4) by some other means of propulsion, such as turbojet, or rocket engines.{{sfn |Segal|2009| pp=1}} In the flight of the experimental scramjet-powered [[Boeing X-51A]], the test craft was lifted to flight altitude by a [[Boeing B-52 Stratofortress]] before being released and accelerated by a detachable rocket to near Mach{{nbsp}}4.5.<ref name="PWR-2010-05-26">{{cite press release |url=http://www.pw.utc.com/Media+Center/Press+Releases/Pratt+&+Whitney+Rocketdyne+Scramjet+Powers+Historic+First+Flight+of+X-51A+WaveRider |title=Pratt & Whitney Rocketdyne Scramjet Powers Historic First Flight of X-51A WaveRider |last1=Colaguori |first1=Nancy |last2=Kidder |first2=Brian |location=[[West Palm Beach, Florida]] |publisher=[[Pratt & Whitney Rocketdyne]] |date=26 May 2010 |archive-url=https://web.archive.org/web/20110101213232/http://www.pw.utc.com/Media+Center/Press+Releases/Pratt+%26+Whitney+Rocketdyne+Scramjet+Powers+Historic+First+Flight+of+X-51A+WaveRider |archive-date=1 January 2011 |access-date=12 February 2016 }}</ref> In May 2013, another flight achieved an increased speed of Mach{{nbsp}}5.1.<ref name="Phys 2013-05-03">{{cite news |url=http://phys.org/news/2013-05-experimental-air-aircraft-hypersonic.html |title=Experimental Air Force aircraft goes hypersonic |work=[[Phys.org]] |publisher=Omicron Technology Limited |date=3 May 2013 |url-status=live |archive-url=https://web.archive.org/web/20160212173726/http://phys.org/news/2013-05-experimental-air-aircraft-hypersonic.html |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| While scramjets are conceptually simple, actual implementation is limited by extreme technical challenges. Hypersonic flight within the atmosphere generates immense drag, and temperatures found on the aircraft and within the engine can be much greater than that of the surrounding air. Maintaining combustion in the supersonic flow presents additional challenges, as the fuel must be injected, mixed, ignited, and burned within milliseconds. While scramjet technology has been under development since the 1950s, only very recently have scramjets successfully achieved powered flight.{{sfn |Segal|2009| pp=3–11}}
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| [[File:Turbo ram scramjet comparative diagram.svg|alt=A [[comparative diagram]] of the different geometries for the compression, combustion, and expansion sections of a turbojet, a ramjet, and a scramjet. |thumb| The compression, combustion, and expansion regions of: (a) turbojet, (b) ramjet, and (c) scramjet engines.]]
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| Scramjets are designed to operate in the hypersonic flight regime, beyond the reach of turbojet engines, and, along with ramjets, fill the gap between the high efficiency of turbojets and the high speed of rocket engines. [[Turbomachinery]]-based engines, while highly efficient at subsonic speeds, become increasingly inefficient at transonic speeds, as the compressor rotors found in turbojet engines require subsonic speeds to operate. While the flow from [[transonic]] to low supersonic speeds can be decelerated to these conditions, doing so at supersonic speeds results in a tremendous increase in temperature and a loss in the total [[pressure]] of the flow. Around Mach{{nbsp}}3–4, turbomachinery is no longer useful, and ram-style compression becomes the preferred method.{{sfn |Hill|Peterson|1992| pp=21}}
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| [[Ramjet]]s use high-speed characteristics of air to literally 'ram' air through an inlet diffuser into the combustor. At transonic and supersonic flight speeds, the air upstream of the inlet is not able to move out of the way quickly enough, and is compressed within the diffuser before being diffused into the combustor. Combustion in a ramjet takes place at subsonic velocities, similar to turbojets but the combustion products are then accelerated through a [[convergent-divergent nozzle]] to supersonic speeds. As they have no mechanical means of compression, ramjets cannot start from a standstill, and generally do not achieve sufficient compression until supersonic flight. The lack of intricate turbomachinery allows ramjets to deal with the temperature rise associated with decelerating a supersonic flow to subsonic speeds. However, as speed rises, the internal energy of the flow after diffusor grows rapidly, so the relative addition of energy due to fuel combustion becomes lower, leading to decrease in efficiency of the engine. This leads to decrease in thrust generated by ramjets at higher speeds.{{sfn|Hill|Peterson|1992| pp=21}} | |
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| Thus, to generate thrust at very high velocities, the rise of the pressure and temperature of the incoming air flow must be tightly controlled. In particular, this means that deceleration of the airflow to subsonic speed cannot be allowed. Mixing the fuel and air in this situation presents a considerable engineering challenge, compounded by the need to closely manage the speed of combustion while maximizing the relative increase of internal energy within the combustion chamber. Consequently, current scramjet technology requires the use of high-energy fuels and active cooling schemes to maintain sustained operation, often using [[hydrogen]] and [[regenerative cooling (rocket)|regenerative cooling]] techniques.{{sfn |Segal|2009| pp=4}}
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| ==Theory==
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| All scramjet engines have an intake which compresses the incoming air, fuel injectors, a combustion chamber, and a divergent [[propulsive nozzle|thrust nozzle]]. Sometimes engines also include a region which acts as a [[flame holder]], although the high [[stagnation temperature]]s mean that an area of focused waves may be used, rather than a discrete engine part as seen in turbine engines. Other engines use [[pyrophoric]] fuel additives, such as [[silane]], to avoid flameout. An isolator between the inlet and combustion chamber is often included to improve the homogeneity of the flow in the combustor and to extend the operating range of the engine.
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| [[Shock wave|Shockwave]] imaging by the University of Maryland using [[Schlieren imaging]] determined that the fuel mixture controls compression by creating backpressure and shockwaves that slow and compress the air before ignition, much like the shock cone of a Ramjet. The imaging showed that the higher the fuel flow and combustion, the more shockwaves formed ahead of the combustor, which slowed and compressed the air before ignition.<ref>Analysis of Ignition Process in a Scramjet at Low and High Fueling Rates, Gareth Dunlap, Elias Fekadu, Ben Grove, Nick Gabsa, Kenneth Yu, Camilo Munoz, Jason Burr.</ref>
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| [[File:X-43A (Hyper - X) Mach 7 computational fluid dynamic (CFD).jpg|thumb|upright=1.15|[[Computational fluid dynamics]] (CFD) image of the [[NASA]] [[X-43A]] with scramjet attached to the underside at [[Mach number|Mach]] 7|alt=Computer-generated image of stress and shock-waves experienced by aerial vehicle travelling at high speed ]]
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| A scramjet is reminiscent of a [[ramjet]]. In a typical ramjet, the supersonic inflow of the engine is decelerated at the inlet to subsonic speeds and then reaccelerated through a nozzle to supersonic speeds to produce thrust. This deceleration, which is produced by a normal [[shock wave|shock]], creates a total [[pressure]] loss which limits the upper operating point of a ramjet engine.
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| For a scramjet, the kinetic energy of the freestream air entering the scramjet engine is comparable to the energy released by the reaction of the oxygen content of the air with a fuel (e.g. hydrogen). Thus the heat released from combustion at Mach{{nbsp}}2.5<!-- changed this from a clearly erroneous "Mach 25"; assumed it was just an omitted decimal point --> is around 10% of the total enthalpy of the working fluid. Depending on the fuel, the [[kinetic energy]] of the air and the potential combustion heat release will be equal at around Mach{{nbsp}}8. Thus the design of a scramjet engine is as much about minimizing drag as maximizing thrust.
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| This high speed makes the control of the flow within the combustion chamber more difficult. Since the flow is supersonic, no downstream influence propagates within the freestream of the combustion chamber. Throttling of the entrance to the thrust nozzle is not a usable control technique. In effect, a block of gas entering the combustion chamber must mix with fuel and have sufficient time for initiation and reaction, all the while traveling supersonically through the combustion chamber, before the burned gas is expanded through the thrust nozzle. This places stringent requirements on the pressure and temperature of the flow, and requires that the fuel injection and mixing be extremely efficient. Usable [[dynamic pressure]]s lie in the range {{convert|20|to|200|kPa|psi}}, where
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| :<math>q = \frac{1}{2}\rho v^2 </math>
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| where
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| :''q'' is the dynamic pressure of the gas
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| :''ρ'' ([[rho (letter)|rho]]) is the [[density]] of the gas
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| :''v'' is the [[velocity]] of the gas
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| To keep the combustion rate of the fuel constant, the pressure and temperature in the engine must also be constant. This is problematic because the airflow control systems that would facilitate this are not physically possible in a scramjet launch vehicle due to the speed and altitude range involved, meaning that it must travel at an altitude specific to its speed. Because air density reduces at higher altitudes, a scramjet must climb at a specific rate as it accelerates to maintain a constant air pressure at the intake. This optimal climb/descent profile is called a "constant dynamic pressure path". It is thought that scramjets might be operable up to an altitude of 75 km.<ref name="OrbitalVector">{{cite web |url=http://www.orbitalvector.com/Orbital%20Travel/Scramjets/Scramjets.htm |title=Scramjets |url-status=live |archive-url=https://web.archive.org/web/20160212164212/http://www.orbitalvector.com/Orbital%20Travel/Scramjets/Scramjets.htm |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| Fuel injection and management is also potentially complex. One possibility would be that the fuel be pressurized to 100 bar by a turbo pump, heated by the fuselage, sent through the turbine and accelerated to higher speeds than the air by a nozzle. The air and fuel stream are crossed in a comb-like structure, which generates a large interface. Turbulence due to the higher speed of the fuel leads to additional mixing. Complex fuels like kerosene need a long engine to complete combustion.
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| The minimum Mach number at which a scramjet can operate is limited by the fact that the compressed flow must be hot enough to burn the fuel, and have pressure high enough that the reaction be finished before the air moves out the back of the engine. Additionally, to be called a scramjet, the compressed flow must still be supersonic after combustion. Here two limits must be observed: First, since when a supersonic flow is compressed it slows down, the level of compression must be low enough (or the initial speed high enough) not to slow the gas below Mach{{nbsp}}1. If the gas within a scramjet goes below Mach{{nbsp}}1 the engine will "choke", transitioning to subsonic flow in the combustion chamber. This effect is well known amongst experimenters on scramjets since the waves caused by choking are easily observable. Additionally, the sudden increase in pressure and temperature in the engine can lead to an acceleration of the combustion, leading to the combustion chamber exploding.
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| Second, the heating of the gas by combustion causes the speed of sound in the gas to increase (and the Mach number to decrease) even though the gas is still travelling at the same speed. Forcing the speed of air flow in the combustion chamber under Mach{{nbsp}}1 in this way is called "thermal choking". It is clear that a pure scramjet can operate at Mach numbers of 6–8,<ref name="N96-11688">{{cite journal |last1=Paull |first1=A. |last2=Stalker |first2=R. J. |last3=Mee |first3=D. J. |title=Supersonic Combustion Ramjet Propulsion Experiments In a Shock Tunnel |journal=Shock Tunnel Studies of Scramjet Phenomena 1994 |publisher=[[University of Queensland]] |date=1 January 1995 |hdl=2060/19960001680 }}</ref> but in the lower limit, it depends on the definition of a scramjet. There are engine designs where a ramjet transforms into a scramjet over the Mach{{nbsp}}3–6 range, known as dual-mode scramjets.<ref name="AIAA-99-4848">{{cite conference |last1=Voland |first1=R. T. |last2=Auslender |first2=A. H. |last3=Smart |first3=M. K. |last4=Roudakov |first4=A. S. |last5=Semenov |first5=V. L. |last6=Kopchenov |first6=V. |title=CIAM/NASA Mach 6.5 Scramjet Flight and Ground Test |conference=9th International Space Planes and Hypersonic Systems and Technologies Conference |publisher=[[AIAA]] |place=[[Norfolk, Virginia]] |year=1999 |doi=10.2514/MHYTASP99 |hdl=2060/20040087160 }}</ref> In this range however, the engine is still receiving significant thrust from subsonic combustion of the ramjet type.
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| The high cost of flight testing and the unavailability of ground facilities have hindered scramjet development. A large amount of the experimental work on scramjets has been undertaken in cryogenic facilities, direct-connect tests, or burners, each of which simulates one aspect of the engine operation. Further, vitiated facilities (with the ability to control air impurities<ref name="UoV Ground Testing">{{cite web |url=http://www.mae.virginia.edu/HyV/groundtesting.htm |title=The Hy-V Program – Ground Testing |work=Research |publisher=[[University of Virginia]] |url-status=live |archive-url=https://web.archive.org/web/20160212174005/http://www.mae.virginia.edu/HyV/groundtesting.htm |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>), storage heated facilities, arc facilities and the various types of shock tunnels each have limitations which have prevented perfect simulation of scramjet operation. The [[HyShot]] flight test showed the relevance of the 1:1 simulation of conditions in the T4 and HEG shock tunnels, despite having cold models and a short test time. The [[NASA]]-CIAM tests provided similar verification for CIAM's C-16 V/K facility and the Hyper-X project is expected to provide similar verification for the Langley AHSTF,<ref>{{cite web |url=http://wte.larc.nasa.gov/facilities/hypersonic/arc-heated.cfm?field=11&id=2&fac=1 |title=Arc-Heated Scramjet Test Facility |publisher=[[NASA Langley Research Center]] |date=17 November 2005 |archive-url=https://web.archive.org/web/20101024014047/http://wte.larc.nasa.gov/facilities/hypersonic/arc-heated.cfm?field=11&id=2&fac=1 |archive-date=24 October 2010 |access-date=18 August 2009 }}</ref> CHSTF,<ref name="Langley HSTF">{{cite web |url=http://wte.larc.nasa.gov/facilities/hypersonic/combustion.cfm?field=12&id=2&fac=1 |title=Combustion-Heated Scramjet Test Facility |publisher=[[NASA Langley Research Center]] |date=17 November 2005 |archive-url=https://web.archive.org/web/20101024014107/http://wte.larc.nasa.gov/facilities/hypersonic/combustion.cfm?field=12&id=2&fac=1 |archive-date=24 October 2010 |access-date=12 February 2016 }}</ref> and {{Convert|8|ft|m|1|abbr=on}} HTT.
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| [[Computational fluid dynamics]] has only recently{{hsp}}{{When|date=September 2011}} reached a position to make reasonable computations in solving scramjet operation problems. Boundary layer modeling, turbulent mixing, two-phase flow, flow separation, and real-gas aerothermodynamics continue to be problems on the cutting edge of CFD. Additionally, the modeling of kinetic-limited combustion with very fast-reacting species such as hydrogen makes severe demands on computing resources.<ref>{{Cite journal |last1=Guan |first1=Xingyi |last2=Das |first2=Akshaya |last3=Stein |first3=Christopher J. |last4=Heidar-Zadeh |first4=Farnaz |last5=Bertels |first5=Luke |last6=Liu |first6=Meili |last7=Haghighatlari |first7=Mojtaba |last8=Li |first8=Jie |last9=Zhang |first9=Oufan |last10=Hao |first10=Hongxia |last11=Leven |first11=Itai |last12=Head-Gordon |first12=Martin |last13=Head-Gordon |first13=Teresa |date=2022-05-17 |title=A benchmark dataset for Hydrogen Combustion |journal=Scientific Data |language=en |volume=9 |issue=1 |page=215 |doi=10.1038/s41597-022-01330-5 |pmid=35581204 |pmc=9114378 |bibcode=2022NatSD...9..215G |issn=2052-4463}}</ref>
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| Reaction schemes are [[Stiff equation|numerically stiff]] requiring reduced reaction schemes.{{Clarify|date=September 2011}}
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| Much of scramjet experimentation remains [[Classified information|classified]]. Several groups, including the [[United States Navy|US Navy]] with the SCRAM engine between 1968 and 1974, and the [[Hyper-X]] program with the [[NASA X-43|X-43A]], have claimed successful demonstrations of scramjet technology. Since these results have not been published openly, they remain unverified and a final design method of scramjet engines still does not exist.
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| The final application of a scramjet engine is likely to be in conjunction with engines which can operate outside the scramjet's operating range.{{Citation needed|date=September 2011}}
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| Dual-mode scramjets combine [[Speed of sound|subsonic]] combustion with [[supersonic]] combustion for operation at lower speeds, and [[rocket]]-based combined cycle (RBCC) engines supplement a traditional rocket's propulsion with a scramjet, allowing for additional [[oxidizer]] to be added to the scramjet flow. RBCCs offer a possibility to extend a scramjet's operating range to higher speeds or lower intake dynamic pressures than would otherwise be possible.
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| == Characteristics ==
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| === Aircraft ===
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| # Does not have to carry oxygen
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| # No rotating parts makes it easier to manufacture than a turbojet
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| # Has a higher [[specific impulse]] (change in momentum per unit of propellant) than a rocket engine; could provide between 1000 and 4000 seconds, while a rocket typically provides around 450 seconds or less.<ref>{{cite web|url=http://www.braeunig.us/space/specs/delta.htm|title=Space Launchers – Delta|website=www.braeunig.us}}</ref>
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| # Higher speed could mean cheaper access to outer space in the future
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| # Difficult / expensive testing and development
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| # Very high initial propulsion requirements
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| Unlike a rocket that quickly passes mostly vertically through the atmosphere or a turbojet or ramjet that flies at much lower speeds, a hypersonic airbreathing vehicle optimally flies a "depressed trajectory", staying within the atmosphere at hypersonic speeds. Because scramjets have only mediocre thrust-to-weight ratios,<ref>{{cite book |last1=Rathore |first1=Mahesh M. |url=https://books.google.com/books?id=hBl2IIcbLy0C&pg=PA966 |title=Thermal Engineering |chapter=Jet and Rocket Propulsions |chapter-url=https://books.google.com/books?id=hBl2IIcbLy0C&pg=PA963 |location=New Delhi, India |publisher=[[Tata McGraw-Hill Education]] |year=2010 |page=966 |isbn=978-0-07-068113-2 |access-date=12 February 2016 |quote=A scramjet has very poor thrust to weight ratio (~2). }}</ref> acceleration would be limited. Therefore, time in the atmosphere at supersonic speed would be considerable, possibly 15–30 minutes. Similar to a [[Atmospheric reentry|reentering]] space vehicle, heat insulation would be a formidable task, with protection required for a duration longer than that of a typical [[space capsule]], although less than the [[Space Shuttle]].
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| New materials offer good insulation at high temperature, but they often [[Ablation|sacrifice]] themselves in the process. Therefore, studies often plan on "active cooling", where coolant circulating throughout the vehicle skin prevents it from disintegrating. Often the coolant is the fuel itself, in much the same way that modern rockets use their own fuel and oxidizer as coolant for their engines. All cooling systems add weight and complexity to a launch system. The cooling of scramjets in this way may result in greater efficiency, as heat is added to the fuel prior to entry into the engine, but results in increased complexity and weight which ultimately could outweigh any performance gains.
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| {{Unreferenced section|date=April 2010}}
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| [[File:Specific-impulse-kk-20090105.png|thumb|upright=1.75|The specific impulse of various engines]]
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| The performance of a [[Launch vehicle|launch system]] is complex and depends greatly on its weight. Normally craft are designed to maximise range (<math>R</math>), orbital radius (<math>R</math>) or payload mass fraction (<math>\Gamma</math>) for a given engine and fuel. This results in tradeoffs between the efficiency of the engine (takeoff fuel weight) and the complexity of the engine (takeoff dry weight), which can be expressed by the following:
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| :<math>\Pi_\text{e} + \Pi_\text{f} + \frac{1}{\Gamma} = 1</math>
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| Where :
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| *<math>\Pi_\text{e} = \frac{m_\text{empty}}{m_\text{initial}}</math> is the empty mass fraction, and represents the weight of the superstructure, tankage and engine. | |
| *<math>\Pi_\text{f} = \frac{m_\text{fuel}}{m_\text{initial}}</math> is the fuel mass fraction, and represents the weight of fuel, oxidiser and any other materials which are consumed during the launch.
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| *<math>\Gamma = \frac{m_\text{initial}}{m_\text{payload}}</math> is initial mass ratio, and is the inverse of the payload mass fraction. This represents how much payload the vehicle can deliver to a destination.
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| A scramjet increases the mass of the motor <math>\Pi_\text{e}</math> over a rocket, and decreases the mass of the fuel <math>\Pi_\text{f}</math>. It can be difficult to decide whether this will result in an increased <math>\Gamma</math> (which would be an increased payload delivered to a destination for a constant vehicle takeoff weight). The logic behind efforts driving a scramjet is (for example) that the reduction in fuel decreases the total mass by 30%, while the increased engine weight adds 10% to the vehicle total mass. Unfortunately the uncertainty in the calculation of any mass or efficiency changes in a vehicle is so great that slightly different assumptions for engine efficiency or mass can provide equally good arguments for or against scramjet powered vehicles.
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| Additionally, the drag of the new configuration must be considered. The drag of the total configuration can be considered as the sum of the vehicle drag (<math>D</math>) and the engine installation drag (<math>D_\text{e}</math>). The installation drag traditionally results from the pylons and the coupled flow due to the engine jet, and is a function of the throttle setting. Thus it is often written as:
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| :<math>D_\text{e} = \phi_\text{e} F</math>
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| Where:
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| *<math>\phi_\text{e}</math> is the loss coefficient
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| *<math>F</math> is the thrust of the engine
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| For an engine strongly integrated into the aerodynamic body, it may be more convenient to think of (<math>D_\text{e}</math>) as the difference in drag from a known base configuration.
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| The overall [[engine efficiency]] can be represented as a value between 0 and 1 (<math>\eta_0</math>), in terms of the [[specific impulse]] of the engine:
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| :<math>\eta_0 = \frac{g_0 V_0}{h_\text{PR}} I_\text{sp} = \frac{\mbox{Thrust power}}{\mbox{Chemical energy rate}}</math>
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| Where:
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| *<math>g_0</math> is the acceleration due to gravity at ground level
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| *<math>V_0</math> is the vehicle speed
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| *<math>I_\text{sp}</math> is the [[specific impulse]]
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| *<math>h_\text{PR}</math> is fuel [[heat of reaction]]
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| Specific impulse is often used as the unit of efficiency for rockets, since in the case of the rocket, there is a direct relation between specific impulse, [[specific fuel consumption (thrust)|specific fuel consumption]] and exhaust velocity. This direct relation is not generally present for airbreathing engines, and so specific impulse is less used in the literature. Note that for an airbreathing engine, both <math>\eta_0</math> and <math>I_\text{sp}</math> are a function of velocity.
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| The specific impulse of a [[rocket]] engine is independent of velocity, and common values are between 200 and 600 seconds (450{{nbsp}}s for the space shuttle main engines). The specific impulse of a scramjet varies with velocity, reducing at higher speeds, starting at about 1200{{nbsp}}s,{{Citation needed|date=September 2011}} although values in the literature vary.{{Citation needed|date=September 2011}}
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| For the simple case of a single stage vehicle, the fuel mass fraction can be expressed as:
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| :<math>\Pi_\text{f} = 1 - \exp\left[-\frac{\left(\frac{V_\text{initial}^2}{2} - \frac{V_i^2}{2}\right) + \int{g}\,dr}{\eta_0 h_\text{PR}\left(1 - \frac{D + D_\text{e}}{F}\right)}\right]</math>
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| Where this can be expressed for [[single-stage-to-orbit|single stage transfer to orbit]] as:
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| :<math>\Pi_\text{f} = 1 - \exp\left[-\frac{g_0 r_0\left(1 - \frac{1}{2}\frac{r_0}{r}\right)}{\eta_0 h_\text{PR}\left(1 - \frac{D + D_\text{e}}{F}\right)}\right]</math>
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| or for level atmospheric flight from [[air launch]] ([[missile]] flight):
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| :<math>\Pi_\text{f} = 1 - \exp\left[-\frac{g_0 R}{\eta_0 h_\text{PR}\left(1 - \phi_\text{e}\right)\frac{C_\text{L}}{C_\text{D}}}\right]</math>
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| Where <math>R</math> is the [[Range (aircraft)|range]], and the calculation can be expressed in the form of the [[Louis Charles Breguet|Breguet]] range formula:
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| :<math>\begin{align}
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| \Pi_\text{f} &= 1 - e^{-BR} \\
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| B &= \frac{g_0}{\eta_0 h_{PR}\left(1 - \phi_e\right)\frac{C_\text{L}}{C_\text{D}}}
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| \end{align}</math>
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| Where:
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| *<math>C_\text{L}</math> is the [[lift coefficient]] | |
| *<math>C_\text{D}</math> is the [[drag coefficient]]
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| This extremely simple formulation, used for the purposes of discussion assumes:
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| * [[Single-stage-to-orbit|Single stage]] vehicle
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| * No aerodynamic lift for the transatmospheric lifter
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| However they are true generally for all engines.
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| A scramjet cannot produce efficient thrust unless boosted to high speed, around Mach{{nbsp}}5, although depending on the design it could act as a ramjet at low speeds. A horizontal take-off aircraft would need conventional [[turbofan]], [[turbojet]], or rocket engines to take off, sufficiently large to move a heavy craft. Also needed would be fuel for those engines, plus all engine-associated mounting structure and control systems. Turbofan and turbojet engines are heavy and cannot easily exceed about Mach{{nbsp}}2–3, so another propulsion method would be needed to reach scramjet operating speed. That could be [[ramjet]]s or [[rocket]]s. Those would also need their own separate fuel supply, structure, and systems. A number of proposals instead call for a first stage of droppable [[solid rocket booster]]s, which greatly simplifies the design.
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| [[File:SJX61 1EngineTest20070221 TransitionToJP7.jpg|thumb|Test of [[Pratt & Whitney Rocketdyne]] [[SJY61]] scramjet engine for the [[Boeing X-51]]]]
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| Unlike jet or rocket propulsion systems facilities which can be tested on the ground, testing scramjet designs uses extremely expensive hypersonic test chambers or expensive launch vehicles, both of which lead to high instrumentation costs. Tests using launched test vehicles very typically end with destruction of the test item and instrumentation.
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| === Orbital vehicles ===
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| An advantage of a hypersonic airbreathing (typically scramjet) vehicle like the [[X-30]] is avoiding or at least reducing the need for carrying oxidizer. For example, the [[Space Shuttle external tank]] held 616,432.2 kg of [[liquid oxygen]] (LOX) and 103,000 kg of [[liquid hydrogen]] (LH{{sub|2}}) while having an empty weight of 30,000 kg. The [[Space Shuttle Orbiter|orbiter]] gross weight was 109,000 kg with a maximum payload of about 25,000 kg and to get the assembly off the launch pad the shuttle used two very powerful [[Space Shuttle Solid Rocket Booster|solid rocket boosters]] with a weight of 590,000 kg each. If the oxygen could be eliminated, the vehicle could be lighter at liftoff and possibly carry more payload.
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| On the other hand, scramjets spend more time in the atmosphere and require more hydrogen fuel to deal with aerodynamic drag. Whereas liquid oxygen is quite a dense fluid (1141 kg/m<sup>3</sup>), liquid hydrogen has much lower density (70.85 kg/m<sup>3</sup>) and takes up more volume. This means that the vehicle using this fuel becomes much bigger and gives more drag.<ref>{{cite book |last1=Johns |first1=Lionel S. |last2=Shaw |first2=Alan |last3=Sharfman |first3=Peter |last4=Williamson |first4=Ray A. |last5=DalBello |first5=Richard |url=https://books.google.com/books?id=Smtn0fbL-EAC&pg=PA78 |title=Round Trip to Orbit: Human Spaceflight Alternatives |chapter=The National Aero-Space Plane |chapter-url=https://books.google.com/books?id=Smtn0fbL-EAC&pg=PA65 |location=Washington, D.C. |publisher=[[Congress of the United States]] |year=1989 |page=78 |isbn=978-1-4289-2233-4 |access-date=12 February 2016 }}</ref> Other fuels have more comparable density, such as [[RP-1]] (810 kg/m<sup>3</sup>) [[JP-7]] (density at 15 °C 779–806 kg/m<sup>3</sup>) and [[unsymmetrical dimethylhydrazine]] (UDMH) (793.00 kg/m<sup>3</sup>).
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| One issue is that scramjet engines are predicted to have exceptionally poor [[thrust-to-weight ratio]] of around 2, when installed in a launch vehicle.<ref name="JBIS">{{cite journal|title=A Comparison of Propulsion Concepts for SSTO Reusable Launchers |journal=Journal of the British Interplanetary Society |year=2003 |last1=Varvill |first1=Richard |last2=Bond |first2=Alan |volume=56 |pages=108–117 |issn=0007-084X |url=http://www.reactionengines.co.uk/downloads/JBIS_v56_108-117.pdf |access-date=12 February 2016 |archive-url=https://web.archive.org/web/20120628231043/http://www.reactionengines.co.uk/downloads/JBIS_v56_108-117.pdf |archive-date=28 June 2012 |bibcode=2003JBIS...56..108V }}</ref> A rocket has the advantage that its engines have ''very'' high thrust-weight ratios (~100:1), while the tank to hold the liquid oxygen approaches a volume ratio of ~100:1 also. Thus a rocket can achieve a very high [[Propellant mass fraction|mass fraction]], which improves performance. By way of contrast the projected thrust/weight ratio of scramjet engines of about 2 mean a much larger percentage of the takeoff mass is engine (ignoring that this fraction increases anyway by a factor of about four due to the lack of onboard oxidiser). In addition the vehicle's lower thrust does not necessarily avoid the need for the expensive, bulky, and failure-prone high performance turbopumps found in conventional liquid-fuelled rocket engines, since most scramjet designs seem to be incapable of orbital speeds in airbreathing mode, and hence extra rocket engines are needed.{{Citation needed|date=May 2010}}
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| Scramjets might be able to accelerate from approximately Mach{{nbsp}}5–7 to around somewhere between half of [[orbital speed]] and orbital speed (X-30 research suggested that Mach{{nbsp}}17 might be the limit compared to an orbital speed of Mach{{nbsp}}25, and other studies put the upper speed limit for a pure scramjet engine between Mach{{nbsp}}10 and 25, depending on the assumptions made). Generally, another propulsion system (very typically, a rocket is proposed) is expected to be needed for the final acceleration into orbit. Since the delta-V is moderate and the payload fraction of scramjets high, lower performance rockets such as solids, hypergolics, or simple liquid fueled boosters might be acceptable.
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| Theoretical projections place the top speed of a scramjet between {{convert|12|Mach|altitude_ft=200,000|sigfig=2}} and {{convert|24|Mach|altitude_ft=240,000|sigfig=2}}.<ref name="UnPoCa Tech Report">{{cite web |url=http://upcommons.upc.edu/bitstream/handle/2099.1/20295/Technical%20Report.pdf |title=Study of an Air-Breathing Engine for Hypersonic Flight |last=Mateu |first=Marta Marimon |publisher=[[Universitat Politècnica de Catalunya]] |date=2013 |url-status=live |archive-url=https://web.archive.org/web/20160212184839/http://upcommons.upc.edu/bitstream/handle/2099.1/20295/Technical%20Report.pdf |archive-date=12 February 2016 |access-date=12 February 2016 |quote=Figure 9-10, Page 20 }}</ref> For comparison, the orbital speed at {{convert|200|km|mi}} [[low Earth orbit]] is {{convert|7.79|km/s|km/h mph}}.<ref name="ASaca">{{cite web |url=http://www.spaceacademy.net.au/watch/track/leopars.htm |title=Orbital Parameters – Low Earth Circular Orbits |work=Space Surveillance |publisher=Australian Space Academy |url-status=live |archive-url=https://web.archive.org/web/20160211202014/http://www.spaceacademy.net.au/watch/track/leopars.htm |archive-date=11 February 2016 |access-date=11 February 2016 }}</ref>
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| The scramjet's heat-resistant underside potentially doubles as its reentry system if a single-stage-to-orbit vehicle using non-ablative, non-active cooling is visualised. If an ablative shielding is used on the engine it will probably not be usable after ascent to orbit. If active cooling is used with the fuel as coolant, the loss of all fuel during the burn to orbit will also mean the loss of all cooling for the thermal protection system.
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| Reducing the amount of fuel and oxidizer does not necessarily improve costs as rocket propellants are comparatively very cheap. Indeed, the unit cost of the vehicle can be expected to end up far higher, since aerospace hardware cost is about two orders of magnitude higher than liquid oxygen, fuel and tankage, and scramjet hardware seems to be much heavier than rockets for any given payload. Still, if scramjets enable reusable vehicles, this could theoretically be a cost benefit. Whether equipment subject to the extreme conditions of a scramjet can be reused sufficiently multiple times is unclear; all flown scramjet tests only survive for short periods and have never been designed to survive a flight to date. The eventual cost of such a vehicle is the subject of intense debate{{By whom|date=May 2010}} since even the best estimates disagree whether a scramjet vehicle would be advantageous. It is likely that a scramjet vehicle would need to lift more load than a rocket of equal takeoff weight to be equally as cost efficient (if the scramjet is a non-reusable vehicle).{{Citation needed|date=May 2010}}
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| Space launch vehicles may or may not benefit from having a scramjet stage. A scramjet stage of a launch vehicle theoretically provides a [[specific impulse]] of 1000 to 4000{{nbsp}}s whereas a rocket provides less than 450{{nbsp}}s while in the atmosphere.<ref name="JBIS" /><ref name="AIAA 10.2514">{{cite conference |last=Kors |first=David L. |title=Experimental investigation of a 2-D dual mode scramjet with hydrogenfuel at Mach 4–6 |url=http://arc.aiaa.org/doi/abs/10.2514/6.1990-5216 |conference=2nd International Aerospace Planes Conference |conference-url=http://arc.aiaa.org/doi/book/10.2514/MIAPC90 |publisher=[[AIAA]] |place=[[Orlando, Florida]] |year=1990 |doi=10.2514/MIAPC90 }}</ref> A scramjet's specific impulse decreases rapidly with speed, however, and the vehicle would suffer from a relatively low [[lift to drag ratio]].
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| The installed thrust to weight ratio of scramjets compares very unfavorably with the 50–100 of a typical rocket engine. This is compensated for in scramjets partly because the weight of the vehicle would be carried by aerodynamic lift rather than pure rocket power (giving reduced '[[gravity drag|gravity losses]]'),{{Citation needed|date=March 2008}} but scramjets would take much longer to get to orbit due to lower thrust which greatly offsets the advantage. The takeoff weight of a scramjet vehicle is significantly reduced over that of a rocket, due to the lack of onboard oxidiser, but increased by the structural requirements of the larger and heavier engines.
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| Whether this vehicle could be reusable or not is still a subject of debate and research.
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| ==Proposed applications==
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| An aircraft using this type of jet engine could dramatically reduce the time it takes to travel from one place to another, potentially putting any place on Earth within a 90-minute flight. However, there are questions about whether such a vehicle could carry enough fuel to make useful length trips. In addition, some countries ban or penalize airliners and other civil aircraft that create [[sonic boom]]s. (For example, in the United States, FAA regulations prohibit supersonic flights over land, by civil aircraft.<ref name="FAA-SBoom">{{cite web |url=http://elr.info/news-analysis/3/10067/faa-promulgates-strict-new-sonic-boom-regulation |title=FAA Promulgates Strict New Sonic Boom Regulation |work=The Environmental Law Reporter |publisher=[[Environmental Law Institute]] |date=1973 |url-status=live |archive-url=https://web.archive.org/web/20160212190841/http://elr.info/news-analysis/3/10067/faa-promulgates-strict-new-sonic-boom-regulation |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref><ref name="RisingUp">{{cite web |url=http://www.risingup.com/fars/info/part91-817-FAR.shtml |title=Sec. 91.817 — Civil aircraft sonic boom. |work=FAA Regulations |publisher=RisingUp Aviation |url-status=live |archive-url=https://web.archive.org/web/20160212191141/http://www.risingup.com/fars/info/part91-817-FAR.shtml |archive-date=12 February 2016 |access-date=12 February 2016 }}</ref>
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| <ref name="FAA-ShaBoom">{{cite web |url=https://www.random.org/geographic-coordinates/ |title=Random Location |website=www.random.org |date=2019 }}</ref>)
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| Scramjet vehicle has been proposed for a [[single stage to tether]] vehicle, where a Mach{{nbsp}}12 spinning [[space tether|orbital tether]] would pick up a payload from a vehicle at around 100 km and carry it to orbit.<ref name="NIAC">{{cite conference |last1=Bogar |first1=Thomas J. |last2=Forward |first2=Robert L. |last3=Bangham |first3=Michal E. |last4=Lewis |first4=Mark J. |title=Hypersonic Airplane Space Tether Orbital Launch (HASTOL) System |url=http://www.niac.usra.edu/files/library/meetings/fellows/nov99/355Bogar.pdf |conference=NIAC Fellows Meeting |publisher=[[NASA Institute for Advanced Concepts]] |place=[[Atlanta]], Georgia |date=9 November 1999 |url-status=live |archive-url=https://web.archive.org/web/20160212191315/http://www.niac.usra.edu/files/library/meetings/fellows/nov99/355Bogar.pdf |archive-date=12 February 2016 }}</ref>
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| ==See also==
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| {{Portal|Aviation}}
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| *[[Avangard (hypersonic glide vehicle)]] | |
| *[[Precooled jet engine]]
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| *[[Ram accelerator]]
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| *[[Shcramjet]]
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| *[[SABRE (rocket engine)]]
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|
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|
| == References == | | == References == |
| | | {{Reflist}} |
| === Citations ===
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| {{reflist}} | |
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| === Bibliography ===
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| {{refbegin|30em}}
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| * [http://www.up-ship.com/eAPR/ev2n5.htm ''Aerospaceplane – 1961''. Aerospace Projects Review, Volume 2, No 5.]
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| * [http://www.flightglobal.com/pdfarchive/view/1964/1964%20-%200041.html ''Aspects of the Aerospace Plane''. Flight International, 2 January 1964, pages 36–37.]
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| * {{cite book |last1=Segal |first1=Corin |url=https://books.google.com/books?id=lWXGuyj8FwoC |title=The Scramjet Engine: Processes and Characteristics |work=Cambridge Aerospace Series |location=New York City |publisher=[[Cambridge University Press]] |year=2009 |isbn=978-0-521-83815-3 |access-date=13 February 2016 }}
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| * {{cite book |last1=Hill |first1=Philip Graham |last2=Peterson |first2=Carl R. |url=https://books.google.com/books?id=8ihcPgAACAAJ |title=Mechanics and Thermodynamics of Propulsion |edition=2 |location=[[Reading, Massachusetts]] |publisher=[[Addison-Wesley Publishing Company]] |year=1992 |isbn=978-0-201-14659-2 |access-date=13 February 2016 }}
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| * {{cite conference |last=Billig |first=Frederick S. |author-link=Frederick S. Billig |title=SCRAM - A Supersonic Combustion Ramjet Missile |url=http://arc.aiaa.org/doi/abs/10.2514/6.1993-2329 |conference=29th Joint Propulsion Conference and Exhibit |conference-url=http://arc.aiaa.org/doi/book/10.2514/MJPC93 |publisher=[[AIAA]] |place=[[Monterey, California]] |year=1993 |doi=10.2514/MJPC93 }}
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| * {{cite journal |title=Physics and Regimes of Supersonic Combustion |journal=[[AIAA Journal]] |year=2010 |last1=Ingenito |first1=Antonella |last2=Bruno |first2=Claudio |volume=48 |issue=3 |pages=515–525 |issn=0001-1452 |doi=10.2514/1.43652 |bibcode=2010AIAAJ..48..515I |hdl=11573/335488 }}
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| * {{cite web |url=http://www.abc.net.au/science/slab/hyshot/default.htm |title=On the trail of the Scramjet |work=The Lab |publisher=[[Australian Broadcasting Corporation|ABC]] |date=17 October 2002 |url-status=live |archive-url=https://web.archive.org/web/20160213155513/http://www.abc.net.au/science/slab/hyshot/default.htm |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite news |url=http://news.bbc.co.uk/2/hi/science/nature/4832254.stm |title=Revolutionary jet engine tested |work=[[BBC News]] |publisher=[[BBC]] |date=25 March 2006 |url-status=live |archive-url=https://web.archive.org/web/20160213155717/http://news.bbc.co.uk/2/hi/science/nature/4832254.stm |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite web |url=http://skunk-works-digest.netwrx1.org/v02-n027.txt |title=French Support Russian SCRAMJET Tests |work=Skunk Works Digest |date=12 December 1992 |url-status=live |archive-url=https://web.archive.org/web/20160213160345/http://skunk-works-digest.netwrx1.org/v02-n027.txt |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite journal |title=A Burning Question |journal=American Scientist |year=2002 |last=Schneider |first=David |volume=90 |issue=6 |page=1 |url=http://www.americanscientist.org/issues/pub/a-burning-question |access-date=13 February 2016 |archive-url=https://web.archive.org/web/20160213160719/http://www.americanscientist.org/issues/pub/a-burning-question |archive-date=13 February 2016 }}
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| * {{cite news |url=http://www.spacedaily.com/news/scramjet-01a.html |title=Hypersonic Scramjet Projectile Flys In Missile Test |work=SpaceDaily |location=[[Ronkonkoma, New York]] |publisher=Space Media Network |date=4 September 2001 |access-date=13 February 2016 }}
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| * {{cite web |url=http://hapb-www.larc.nasa.gov/Public/Projects/national_hypersonics_plan.html |title=National Hypersonics Plan |publisher=[[NASA Langley Research Center]] |archive-url=https://web.archive.org/web/20050807023831/http://hapb-www.larc.nasa.gov/Public/Projects/national_hypersonics_plan.html |archive-date=7 August 2005 |date=13 August 2003 }}
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| * {{cite web |url=http://www.nasa.gov/missions/research/x43-main.html |title=X-43A |last=Smith |first=Yvette |work=Missions |publisher=[[NASA]] |date=2 October 2010 |url-status=live |archive-url=https://web.archive.org/web/20160213162216/http://www.nasa.gov/missions/research/x43-main.html |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite web |url=http://hypersonics.mechmining.uq.edu.au/hyshot |title=HyShot |work=Centre for Hypersonics |publisher=[[University of Queensland]] |url-status=live |archive-url=https://web.archive.org/web/20160213162533/http://hypersonics.mechmining.uq.edu.au/hyshot |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite book |last1=Swinerd |first1=Graham |url=https://books.google.com/books?id=FU0zWjX1CAUC |title=How spacecraft fly: spaceflight without formulae |publisher=[[Copernicus Books]] |year=2010 |isbn=978-1-4419-2629-6 }}
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| {{refend}}
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| == External links ==
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| {{commons category|Scramjets}}
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| * {{cite news |last=Covault |first=Craig |url=http://www.space.com/businesstechnology/x-51-scramjet-military-test-flights-ahead-sfn-100517.html |title=Hypersonic X-51 Scramjet to Launch Test Flight in May |work=[[Space.com]] |publisher=[[Purch]] |date=17 May 2010 |archive-url=https://web.archive.org/web/20101125081516/http://www.space.com/businesstechnology/x-51-scramjet-military-test-flights-ahead-sfn-100517.html |archive-date=25 November 2010 }}
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| * {{cite web |url=http://patft.uspto.gov/netacgi/nph-Parser?patentnumber=6883330 |title=United States Patent: 6883330: Variable geometry inlet design for scram jet engine |last1=Guinan |first1=Daniel P. |last2=Drake |first2=Alan |last3=Andreadis |first3=Dean |last4=Beckel |first4=Stephen A. |publisher=[[USPTO]] |date=26 April 2005 |access-date=13 February 2016 |archive-date=17 October 2015 |archive-url=https://web.archive.org/web/20151017125746/http://patft.uspto.gov/netacgi/nph-Parser?patentnumber=6883330 |url-status=dead }}
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| * {{cite web |url=http://www.islandone.org/Propulsion/SCRAM-Spencer1.html |title=Liquid Air Cycle Rocket Equation |last=Spencer |first=Henry |publisher=Island One Society |url-status=live |archive-url=https://web.archive.org/web/20160213164103/http://www.islandone.org/Propulsion/SCRAM-Spencer1.html |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite news |last=Leonard |first=David |url=http://www.space.com/missionlaunches/hyshot_020816.html |title=Results Just In: HyShot Scramjet Test a Success |work=[[Space.com]] |date=16 August 2002 |archive-url=https://web.archive.org/web/20090926181753/http://www.space.com/missionlaunches/hyshot_020816.html |archive-date=26 September 2009 }}
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| * {{cite news |last=Wickham |first=Chris |url=https://www.reuters.com/article/us-science-spaceplane-idUSBRE8AR0V220121128 |title=British company claims biggest engine advance since the jet |work=[[Reuters]] |publisher=[[Thomson Reuters Corporation]] |date=28 November 2012 |url-status=live |archive-url=https://web.archive.org/web/20160213164842/https://www.reuters.com/article/us-science-spaceplane-idUSBRE8AR0V220121128 |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite web |url=http://www.combustioninstitute-indiansection.com/pdf/SCRAMJET%20COMBUSTOR%20DEVELOPMENT.pdf |title=Scramjet Combustor Development |last= Satish |first=Kumar |publisher=Combustion Institute (Indian Section) |url-status=live |archive-url=https://web.archive.org/web/20160213165114/http://www.combustioninstitute-indiansection.com/pdf/SCRAMJET%20COMBUSTOR%20DEVELOPMENT.pdf |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| * {{cite web |url=http://nextbigfuture.com/2011/06/aerojet-has-new-mach-7-plus-reusable.html |title=Aerojet has new Mach 7 plus reusable hypersonic vehicle plans |last=Wang |first=Brian |publisher=New Big Future |date=10 June 2011 |url-status=live |archive-url=https://web.archive.org/web/20160213165327/http://nextbigfuture.com/2011/06/aerojet-has-new-mach-7-plus-reusable.html |archive-date=13 February 2016 |access-date=13 February 2016 }}
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| {{Emerging technologies|transport=yes}}
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| {{Aircraft gas turbine engine components}}
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| [[Category:Aircraft engines]] | | [[Category:Aircraft engines]] |
| [[Category:Jet engines]] | | [[Category:Hypersonic propulsion]] |
| [[Category:Ramjet engines| ]] | | [[Category:Airbreathing jet engines]] |
| [[Category:Spacecraft propulsion]]
| | [[Category:AviationSafetyX Glossary]] |
| [[Category:Single-stage-to-orbit]]
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| [[Category:Space access]]
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| [[Category:Non-rocket spacelaunch]]
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| [[Category:Australian inventions]] | |
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| [[de:Staustrahltriebwerk#Überschallverbrennung im Scramjet]]
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_Mach_7_computational_fluid_dynamic_(CFD).jpg)
