G. V. R. Rao

Last updated
G.V.R.Rao (Gadicharla V R Rao)
Born24 June 1918
Died27 May 2005(2005-05-27) (aged 86)
Known for Bell nozzle, also commonly called the Rao Nozzle [1]

Gadicharla V.R. Rao (G. V. R. Rao), D.Sc. (June 24, 1918- May 27, 2005) was an American aerospace engineer of Indian origin who worked in the jet engine and rocket propulsion fields. [2] Rao worked for General Electric in their Gas Turbine Division department and was a research scientist at Marquardt Aircraft, before working for Rocketdyne, [2] 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. [3] 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), [4] California Institute of Technology (Caltech), [5] and Georgia Institute of Technology. [1]

Contents

During his career, he also worked on aerodynamic and fluid dynamic design projects, such as chemical lasers, the space shuttle main engines [3] [6] [7] scramjet and aerospike rocket engines, and wind-powered generators. [3]

Personal life and education

On June 24, 1918, Rao was born in Rajahmundry [2] [3] [8] in the Andhra Pradesh province of southeastern India. His father was a school headmaster. Rao was born into a large Brahmin household, [3] and is related to Gadicherla Harisarvottama Rao, a well-known freedom fighter for India's independence.

Rao attended Madras Engineering College, and then came to the United States, where he received his D.Sc. in Aeronautical Engineering from New York University in 1949. [2]

He met and married Mary Fabrizio in New York, and they subsequently moved to Bangalore, India. [3] [8] Rao and Mary returned to America after their first son, Raman was born. Rao then worked at General Electric. Their second son, Krishna was born, and the family subsequently moved to Woodland Hills, California. [3] In 1976, the Raos moved to Thousand Oaks. Rao died at the age of 86 on May 27, 2005. [3]

Career

Nozzles of Saturn-V Nozzles of Saturn-V.JPG
Nozzles of Saturn-V
Nozzle of an extensible Cryogenic Engine Common Extensible Cryogenic Engine.jpg
Nozzle of an extensible Cryogenic Engine

Educator

After receiving his D.Sc., Rao taught in Bangalore, India at the Graduate Research Institute. [3]

Aerospace engineer

From 1952 to 1955, Rao worked for General Electric in their Gas Turbine Division. He was then a research scientist at Marquardt Aircraft until 1958. Rao then worked for Rocketdyne in California as a design analyst. [2] [9]

Beginning in the mid-1950s, Rao began to use mainframe computers at Rocketdyne to make computations for the design of rocket nozzles. Kramer and Wheelock state, "Rao developed a method for determining the nozzle contour that would produce the maximum thrust for any given nozzle area ratio and length... The optimum turned out to be not only more efficient but also considerably shorter by about 60% than a 15-degree conical nozzle of the same area." [10] George P. Sutton, who worked with Rao at Rocketdyne, said that "bell shape or curved exit contour is used almost universally today for nozzles designed since about 1960 for large as well as small thrust chamber nozzles" and for both solid and liquid propellants. [11] In 1963, the Advanced Propulsion Section of NASA published Computation of Plug Nozzle Contours by the Rao Optimum Thrust Method about a study that was performed to design a plug nozzle using Rao's maximum thrust theory using a FORTRAN computer program. [12] In 1983, Rao's design was modified, with a slightly different contour, to maximize performance. [13]

In 1961, Rao worked at National Engineering Science Company as associate director. [2] By 1970, he formed his own company, G. V. R. Rao and Associates, through which he contracted with NASA. [14] He worked at Rockwell International for Marshall Space Flight Center in 1988. [15] During his career, he also worked on aerodynamic and fluid dynamic design projects, such as chemical lasers, the space shuttle main engines [3] [6] [7] scramjet and aerospike rocket engines, and wind-powered generators. [3]

His patented inventions include Device for thrust spoiling and thrust reversal (1957), [16] Quiet fan with non-radial elements (1975), [17] Shock wave suppressing flow plate for pulsed lasers (1984), [18] [19] and Mixing aids for supersonic flows (1990). [19] [20]

Publications

Related Research Articles

<span class="mw-page-title-main">Jet engine</span> Aircraft engine that produces thrust by emitting a jet of gas

A jet engine is a type of reaction engine, discharging a fast-moving jet of heated gas that generates thrust by jet propulsion. While this broad definition may include rocket, water jet, and hybrid propulsion, the term jet engine typically refers to an internal combustion air-breathing jet engine such as a turbojet, turbofan, ramjet, pulse jet, or scramjet. In general, jet engines are internal combustion engines.

An arcjet rocket or arcjet thruster is a form of electrically powered spacecraft propulsion, in which an electrical discharge (arc) is created in a flow of propellant. This imparts additional energy to the propellant, so that one can extract more work out of each kilogram of propellant, at the expense of increased power consumption and (usually) higher cost. Also, the thrust levels available from typically used arcjet engines are very low compared with chemical engines.

<span class="mw-page-title-main">Scramjet</span> Jet engine where combustion takes place in supersonic airflow

A scramjet is a variant of a ramjet airbreathing jet engine in which combustion takes place in supersonic airflow. As in ramjets, a scramjet relies on high vehicle speed to compress the incoming air forcefully before combustion, but where as a ramjet decelerates the air to subsonic velocities before combustion using shock cones, a scramjet has no shock cone and slows the airflow using shockwaves produced by its ignition source in place of a shock cone. This allows the scramjet to operate efficiently at extremely high speeds.

<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 used by ballistic missiles and 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">Rocketdyne J-2</span> Rocket engine

The J-2, commonly known as Rocketdyne J-2, was a liquid-fuel cryogenic rocket engine used on NASA's Saturn IB and Saturn V launch vehicles. Built in the United States 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-68</span> A large hydrogen-oxygen rocket engine that powers the Delta IV rocket

The Aerojet Rocketdyne RS-68 was a liquid-fuel rocket engine that used liquid hydrogen (LH2) and liquid oxygen (LOX) as propellants in a gas-generator power cycle. It was the largest hydrogen-fueled rocket engine ever flown.

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

The staged combustion cycle is a power cycle of a bipropellant rocket engine. In the staged combustion cycle, propellant flows through multiple combustion chambers, and is thus combusted in stages. The main advantage relative to other rocket engine power cycles is high fuel efficiency, measured through specific impulse, while its main disadvantage is engineering complexity.

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

The gas-generator cycle, also called open cycle, is one of the most commonly used power cycles in bipropellant liquid rocket engines. Part of the unburned propellant is burned in a gas generator and the resulting hot gas is used to power the propellant pumps before being exhausted overboard, and lost. Because of this loss, this type of engine is termed open cycle.

Regenerative cooling, in the context of rocket engine design, is a configuration in which some or all of the propellant is passed through tubes, channels, or in a jacket around the combustion chamber or nozzle to cool the engine. This is effective because the propellants are often cryogenic. The heated propellant is then fed into a special gas-generator or injected directly into the main combustion chamber.

<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.

<span class="mw-page-title-main">Spacecraft electric propulsion</span> Type of space propulsion using electrostatic and electromagnetic fields for acceleration

Spacecraft electric propulsion is a type of spacecraft propulsion technique that uses electrostatic or electromagnetic fields to accelerate mass to high speed and thus generating thrust to modify the velocity of a spacecraft in orbit. The propulsion system is controlled by power electronics.

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

The bell-shaped or contour nozzle is probably the most commonly used shaped rocket engine nozzle. It has a high angle expansion section right behind the nozzle throat; this is followed by a gradual reversal of nozzle contour slope so that at the nozzle exit the divergence angle is small, usually less than a 10 degree half angle.

<span class="mw-page-title-main">Pintle injector</span> Propellant injection device for a rocket engine.

The pintle injector is a type of propellant injector for a bipropellant rocket engine. Like any other injector, its purpose is to ensure appropriate flow rate and intermixing of the propellants as they are forcibly injected under high pressure into the combustion chamber, so that an efficient and controlled combustion process can happen.

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.

The descent propulsion system or lunar module descent engine (LMDE), internal designation VTR-10, is a variable-throttle hypergolic rocket engine invented by Gerard W. Elverum Jr. and developed by Space Technology Laboratories (TRW) for use in the Apollo Lunar Module descent stage. It used Aerozine 50 fuel and dinitrogen tetroxide oxidizer. This engine used a pintle injector, which paved the way for other engines to use similar designs.

<span class="mw-page-title-main">Joseph Majdalani</span> Lebanese-American professor

Joseph Majdalani is a Lebanese-American professor of Mechanical and Aerospace Engineering. He began his career at Marquette University, before serving as both the Jack D. Whitfield Professor of High Speed Flows and Arnold Chair of Excellence at the University of Tennessee Space Institute. He then served as the Auburn Alumni Engineering Council Endowed Professor and Chair, and is currently the Hugh and Loeda Francis Chair of Excellence in Aerospace Engineering at Auburn University.

<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. 1 2 "Bell/Contoured Nozzles" (PDF). GA Tech. Retrieved November 27, 2016.
  2. 1 2 3 4 5 6 G. V. R. RAO (November 1961). "Recent Developments in Rocket Nozzle Configurations" (PDF). ARS Journal. 31 (11): 1488–1494. doi:10.2514/8.5837 . Retrieved November 27, 2016.
  3. 1 2 3 4 5 6 7 8 9 10 11 "Gadicherla V R Rao". Ventura Star Newspaper. May 28, 2005. Retrieved November 27, 2016. It was posted soon after his death, the exact date is unclear
  4. "Types of Nozzles; Connection of flow to nozzle shape. MIT OpenCourseWare: Lecture 8" (PDF). MIT. p. 6. Retrieved July 30, 2016.
  5. S. R. Kulkarni. "Nozzles". Caltech. p. 8. Retrieved November 27, 2016.
  6. 1 2 Lepore, Frank A. (June 1991). "Flow Induced Vibration in SSME Injection heads" (PDF). Rocketdyne Division, Rockwell International. Retrieved November 27, 2016 via NASA.{{cite journal}}: Cite journal requires |journal= (help)
  7. 1 2 D.G. Pelaccio; F.F. Lepore; G.M. O'Connor; G.V.R. Rao; G.H. Ratekin; S.T. Vogt (June 1984), Experimental Evaluation of an Advanced Space Shuttle Main Engine Hot Gas Manifold Design Concept, American Institute of Aeronautics and Astronautics (AIAA)
  8. 1 2 Who's who in World Aviation and Astronautics. American Aviation Publications, Inc. 1958. p. 362.
  9. Missiles and Rockets. American Aviation Publications. January 1958. p. 175.
  10. Kraemer, Robert S.; Wheelock, Vince (2006). Rocketdyne: Powering Humans Into Space. AIAA. p. 83. ISBN   978-1-56347-754-6.
  11. Sutton, George Paul (2006). History of Liquid Propellant Rocket Engines. AIAA. p. 92. ISBN   978-1-56347-649-5.
  12. "Computation of Plug Nozzle Contours by the Rao Optimum Thrust Method. NASA Technical Document". July 1, 1963. Retrieved November 27, 2016.
  13. J. L, Tuttle; D. H. Blount (May 1983). "Perfect Bell Nozzle Parametric and Optimization Curves - NASA Reference Publication 1104" (PDF). NASA: 7–8. Retrieved July 30, 2016.{{cite journal}}: Cite journal requires |journal= (help)
  14. "G.+V.+R.+"+OR+"G.V.R."+Rao NASA Tech Brief. NASA. 1970.
  15. Tech Notes. U.S. Department of Commerce, National Technical Information Service, Center for the Utilization of Federal Technology. 1988. p. 26.
  16. "Device for thrust spoiling and thrust reversal - US Patent 2,791,088 A". May 7, 1957. Archived from the original on August 11, 2014.
  17. "Quiet fan with non-radial elements - United States Patent: 3,883,264". United States Patent and Trademark Office. May 13, 1975. Retrieved November 27, 2016.
  18. "Shock wave suppressing flow plate for pulsed laser - US patent: 4,457,000". United States Patent and Trademark Office. June 1984. Retrieved November 27, 2016.
  19. 1 2 "Patents by Inventor Gadicherla V. R. Rao". Justia. Retrieved November 27, 2016.
  20. "Mixing aids for supersonic flows - United States Patent 4,899,772". United States Patent and Trademark Office. February 13, 1990. Retrieved November 27, 2016.

Further reading