Expansion deflection nozzle

Last updated

The expansion-deflection nozzle is a rocket nozzle which achieves altitude compensation through interaction of the exhaust gas with the atmosphere, much like the plug and aerospike nozzles.

Contents

Description

This section through an ED nozzle clearly shows the pintle. In this example the outer wall appears similar to the internal contour of a bell nozzle. ED nozzle cutaway view.jpg
This section through an ED nozzle clearly shows the pintle. In this example the outer wall appears similar to the internal contour of a bell nozzle.

It appears much like a standard bell nozzle, but at the throat is a 'centrebody' or 'pintle' which deflects the flow toward the walls. The exhaust gas flows past this in a more outward direction than in standard bell nozzles while expanding before being turned toward the exit. This allows for shorter nozzles than the standard design while maintaining nozzle expansion ratios. Because of the atmospheric boundary, the atmospheric pressure affects the exit area ratio so that atmospheric compensation can be obtained up to the geometric maximum allowed by the specific nozzle.

The nozzle operates in two distinct modes: open and closed. In closed wake mode, the exhaust gas fills the entire nozzle exit area. The ambient pressure at which the wake changes from open to closed modes is called the design pressure. If the ambient pressure reduces any further, additional expansion will occur outside the nozzle much like a standard bell nozzle and no altitude compensation effect will be gained. In open wake mode, the exit area is dependent on the ambient pressure and the exhaust gas exits the nozzle as an annulus as it does not fill the entire nozzle. Because the ambient pressure controls the exit area, the area ratio should be perfectly compensating to the altitude up to the design pressure.

If the pintle is designed to move along its axis of rotation, the throat area can be varied. This would allow for effective throttling, while maintaining chamber pressure. [1]

Like the aerospike and plug nozzles, if modular combustion chambers were used in place of a single combustion chamber, then thrust vectoring would be achievable by throttling the flow to various chambers.

Developed models

The ED nozzle has been known about since the 1960s and there has been several attempts to develop it, with several reaching the level of static hot-firings. These include the 'Expansion-Deflection 50k' [2] (Rocketdyne), the 'Expansion-Deflection 10k' [3] (Rocketdyne) and the RD-0126 [4] (CADB). Rocketdyne also developed a third, smaller E-D nozzle. [5]

Rocketdyne carried out their work during an initial surge in interest in the 1960s, initially developing the E-D 50k nozzle, which had a chamber pressure of 20.7 bar (2.07 MPa) delivering a thrust of 50,000 lbf (220 kN) and was uncooled, allowing it to be tested for a couple seconds at a time. [6] The E-D 10k nozzle had a chamber pressure of 15.5 bar (1.55 MPa) delivering 10,000 lbf (44 kN), a cooled-thrust chamber and was tested in an altitude simulation facility. [7] The smaller E-D nozzle developed 9,900 lbf (44 kN) and was also used to test the altitude compensation ability. These tests confirmed a performance advantage over equivalent bell nozzles. [8]

The Chemical Automatics Design Bureau E-D nozzle was fully cooled and used for hot-fire tests in 1998. Its centrebody houses the combustion chamber (much like the Astrium design mentioned below) allowing for a reduction in length, beyond that of the improved contouring.

Wickman Spacecraft & Propulsion Company have developed and static-tested a solid motor in conjunction with an E-D. [9]

The University of Bristol, UK, has recently[ when? ] successfully tested gaseous hydrogen/air propellants as part of the STERN project. They are also involved in developing knowledge of the in-flight behaviour of the E-D nozzle using a hybrid rocket motor. [10]

Potential uses

While research into this nozzle continues, it could be used before all its advantages are developed. As an upper stage, where it would be used in a low ambient pressure/vacuum environment specifically in closed wake mode, an E-D nozzle would offer weight reductions, length reductions and a potential increase to the specific impulse over bell nozzles (depending on engine cycle) allowing increased payloads. A study suggests it could add an additional 180 kg (400 lb) to the payload of an Ariane 5 over the new Vinci engine provided it is also an expander cycle. Such a nozzle could be brought into service before its altitude compensation abilities were developed. [11]

It is also being investigated for Reaction Engines Skylon spaceplane. Employment on a single-stage-to-orbit (SSTO) rocket would use an E-D nozzle's altitude compensating abilities fully, allowing for a substantial increase in payload. Reaction Engines, Airborne Engineering and the University of Bristol are currently involved in the STERN (Static Test Expansion deflection Rocket Nozzle) project [12] to assess the abilities of the E-D nozzle, and to develop the technology. [13] [14] [15]

Related Research Articles

<span class="mw-page-title-main">Rocket</span> Vehicle propelled by a reaction gas engine

A rocket is a vehicle that uses jet propulsion to accelerate without using the surrounding air. A rocket engine produces thrust by reaction to exhaust expelled at high speed. Rocket engines work entirely from propellant carried within the vehicle; therefore a rocket can fly in the vacuum of space. Rockets work more efficiently in a vacuum and incur a loss of thrust due to the opposing pressure of the atmosphere.

Specific impulse is a measure of how efficiently a reaction mass engine creates thrust. For engines whose reaction mass is only the fuel they carry, specific impulse is exactly proportional to the effective exhaust gas velocity.

A tripropellant rocket is a rocket that uses three propellants, as opposed to the more common bipropellant rocket or monopropellant rocket designs, which use two or one propellants, respectively. Tripropellant systems can be designed to have high specific impulse and have been investigated for single-stage-to-orbit designs. While tripropellant engines have been tested by Rocketdyne and Energomash, no tripropellant rocket has been flown.

<span class="mw-page-title-main">Aerospike engine</span> Type of rocket engine that maintains its aerodynamic efficiency across a wide range of altitudes

The aerospike engine is a type of rocket engine that maintains its aerodynamic efficiency across a wide range of altitudes. It belongs to the class of altitude compensating nozzle engines. Aerospike engines have been studied for several years and are the baseline engines for many single-stage-to-orbit (SSTO) designs and were also a strong contender for the Space Shuttle main engine. However, no such engine is in commercial production, although some large-scale aerospikes are in testing phases.

The plug nozzle is a type of nozzle which includes a centerbody or plug around which the working fluid flows. Plug nozzles have applications in aircraft, rockets, and numerous other fluid flow devices.

<span class="mw-page-title-main">Expanding nozzle</span>

The expanding nozzle is a type of rocket nozzle that, unlike traditional designs, maintains its efficiency at a wide range of altitudes. It is a member of the class of altitude compensating nozzles, a class that also includes the plug nozzle and aerospike. While the expanding nozzle is the least technically advanced and simplest to understand from a modeling point of view, it also appears to be the most difficult design to build.

<span class="mw-page-title-main">Rocket engine</span> Non-air breathing jet engine used to propel a missile or vehicle

A rocket engine uses stored rocket propellants as the reaction mass for forming a high-speed propulsive jet of fluid, usually high-temperature gas. Rocket engines are reaction engines, producing thrust by ejecting mass rearward, in accordance with Newton's third law. Most rocket engines use the combustion of reactive chemicals to supply the necessary energy, but non-combusting forms such as cold gas thrusters and nuclear thermal rockets also exist. Vehicles propelled by rocket engines are commonly called rockets. Rocket vehicles carry their own oxidiser, unlike most combustion engines, so rocket engines can be used in a vacuum to propel spacecraft and ballistic missiles.

<span class="mw-page-title-main">Expander cycle</span> Rocket engine operation method

The expander cycle is a power cycle of a bipropellant rocket engine. In this cycle, the fuel is used to cool the engine's combustion chamber, picking up heat and changing phase. The now heated and gaseous fuel then powers the turbine that drives the engine's fuel and oxidizer pumps before being injected into the combustion chamber and burned.

<span class="mw-page-title-main">RS-25</span> Space Shuttle and SLS main engine

The Aerojet Rocketdyne RS-25, also known as the Space Shuttle Main Engine (SSME), is a liquid-fuel cryogenic rocket engine that was used on NASA's Space Shuttle and is currently used on the Space Launch System (SLS).

<span class="mw-page-title-main">Rocketdyne F-1</span> Rocket engine used on the Saturn V rocket

The F-1, commonly known as Rocketdyne F1, was a rocket engine developed by Rocketdyne. This engine uses a gas-generator cycle developed in the United States in the late 1950s and was used in the Saturn V rocket in the 1960s and early 1970s. Five F-1 engines were used in the S-IC first stage of each Saturn V, which served as the main launch vehicle of the Apollo program. The F-1 remains the most powerful single combustion chamber liquid-propellant rocket engine ever developed.

<span class="mw-page-title-main">Rocketdyne J-2</span> Rocket engine

The J-2 is a liquid-fuel cryogenic rocket engine used on NASA's Saturn IB and Saturn V launch vehicles. Built in the U.S. by Rocketdyne, the J-2 burned cryogenic liquid hydrogen (LH2) and liquid oxygen (LOX) propellants, with each engine producing 1,033.1 kN (232,250 lbf) of thrust in vacuum. The engine's preliminary design dates back to recommendations of the 1959 Silverstein Committee. Rocketdyne won approval to develop the J-2 in June 1960 and the first flight, AS-201, occurred on 26 February 1966. The J-2 underwent several minor upgrades over its operational history to improve the engine's performance, with two major upgrade programs, the de Laval nozzle-type J-2S and aerospike-type J-2T, which were cancelled after the conclusion of the Apollo program.

<span class="mw-page-title-main">RL10</span> Liquid fuel cryogenic rocket engine, typically used on rocket upper stages

The RL10 is a liquid-fuel cryogenic rocket engine built in the United States by Aerojet Rocketdyne that burns cryogenic liquid hydrogen and liquid oxygen propellants. Modern versions produce up to 110 kN (24,729 lbf) of thrust per engine in vacuum. Three RL10 versions are in production for the Centaur upper stage of the Atlas V and the DCSS of the Delta IV. Three more versions are in development for the Exploration Upper Stage of the Space Launch System and the Centaur V of the Vulcan rocket.

<span class="mw-page-title-main">RS-27A</span>

The RS-27A is a liquid-fuel rocket engine developed in 1980s by Rocketdyne for use on the first stage of the Delta II and Delta III launch vehicles. It provides 1.05 meganewtons (240,000 lbf) of thrust burning RP-1 and LOX in a gas-generator cycle. The engine is a modified version of its predecessor, the RS-27; its thrust nozzle has been extended to increase its area ratio from 8:1 to 12:1, which provides greater efficiency at altitude.

<span class="mw-page-title-main">Rocket engine nozzle</span> Type of propelling nozzle

A rocket engine nozzle is a propelling nozzle used in a rocket engine to expand and accelerate combustion products to high supersonic velocities.

An altitude compensating nozzle is a class of rocket engine nozzles that are designed to operate efficiently across a wide range of altitudes.

The RL60 was a planned liquid-fuel cryogenic rocket engine designed in the United States by Pratt & Whitney, burning cryogenic liquid hydrogen and liquid oxygen propellants. The engine runs on an expander cycle, running the turbopumps with waste heat absorbed from the main combustion process. This high-efficiency, waste heat based combustion cycle combined with the high-performance liquid hydrogen fuel enables the engine to reach a very high specific impulse of up to 465 seconds in a vacuum. The engine was planned to be a more capable successor to the Aerojet Rocketdyne RL10, providing improved performance and efficiency while maintaining the installation envelope of the RL10.

<span class="mw-page-title-main">Aerojet LR87</span> American rocket engine family used on Titan missile first stages

The LR87 was an American liquid-propellant rocket engine used on the first stages of Titan intercontinental ballistic missiles and launch vehicles. Composed of twin motors with separate combustion chambers and turbopump machinery, it is considered a single unit and was never flown as a single combustion chamber engine or designed for this. The LR87 first flew in 1959.

Gadicharla V.R. Rao , D.Sc. was an American aerospace engineer of Indian origin who worked in the jet engine and rocket propulsion fields. Rao worked for General Electric in their Gas Turbine Division department and was a research scientist at Marquardt Aircraft, before working for Rocketdyne, where he designed the optimum thrust nozzle. Often referred to as the "Rao's nozzle", it is part of the standard design for rocket engines. The Rao Nozzle is used currently in rocket, missile, and satellite control systems worldwide. It is taught in universities that offer Aerospace Engineering, including Massachusetts Institute of Technology (MIT), California Institute of Technology (Caltech), and Georgia Institute of Technology.

<span class="mw-page-title-main">Rocketdyne XRS-2200</span> Aerospike rocket engine by Rocketdyne

The Rocketdyne XRS-2200 was an experimental linear aerospike engine developed in the mid-1990s for the Lockheed Martin X-33 program. The design was based on the J-2S, the upgraded version of the Apollo era J-2 engine developed in the 1960s. The XRS-2200 used the J-2's combustion cycle and propellant choice.

The MARC-60, also known as MB-60, MB-XX, and RS-73, is a liquid-fuel cryogenic rocket engine designed as a collaborative effort by Japan's Mitsubishi Heavy Industries and US' Aerojet Rocketdyne. The engine burns cryogenic liquid oxygen and liquid hydrogen in an open expander cycle, driving the turbopumps with waste heat from the main combustion process.

References

  1. Constant Chamber Pressure Throttling of an Expansion-Deflection Nozzle [ permanent dead link ] by Charles Schorr, Journal of Spacecraft and Rockets 1970 vol.7 no.7 (pg843-847)
  2. Astronautix Expansion-Deflection 50k
  3. Astronautix Expansion-Deflection 10k
  4. Astronautix RD-0126
  5. History of Liquid Propulsion Rocket Engines, 2006, American Institute of Astronautics and Aeronautics. George P. Sutton
  6. History of Liquid Propulsion Rocket Engines, 2006, American Institute of Astronautics and Aeronautics. George P. Sutton
  7. History of Liquid Propulsion Rocket Engines, 2006, American Institute of Aeronautics and Astronautics. George P. Sutton
  8. History of Liquid Propulsion Rocket Engines, 2006, American Institute of Astronautics and Aeronautics. George P. Sutton
  9. "Small Launch Vehicle (SLV) - Wickman Spacecraft & Propulsion Company". Archived from the original on 2009-09-06. Retrieved 2010-06-10.
  10. The world's first E-D nozzle hybrid tested
  11. Advanced Upper Stage Propulsion Concept - The Expansion-Deflection Upper Stage [ permanent dead link ] by Andreas Goetz, Gerald Hagemann, Joachim Kretschmer and Richard Schwane, 31st AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit, July 10–12, 1995, San Diego CA
  12. Project STERN website Archived 2009-01-31 at the Wayback Machine
  13. Reaction Engines
  14. Bristol University News
  15. Airborne Engineering Archived 2008-12-18 at the Wayback Machine

Further reading