gas dynamics-rocket propulsion

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GDJP Anna University Rocket P R O P U L S I O N

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Gas Dynamics and Propulsion / BY Dr.G.KUMARESAN, / PROFESSOR, / ANNA UNIVERSITY

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Page 1: Gas Dynamics-Rocket Propulsion

GDJP Anna University

Rocket

PROPULSION

Page 2: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction

GDJP Anna University

Aircraft engine application is limited to altitudes of about

100,000 ft or less. But Rocket can function outside the

atmosphere

Rocket can operate in vacuum and achieve any altitude

The thrust of the rocket engines is independent of the flight

speed

Rocket works based on Newton’s law of motion

Rockets carry own oxidizer and fuel tank

Page 3: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Newton’s First law - Applied to Rocket Liftoff

Page 4: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Rocket Engine Thrust

Page 5: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Forces on a Model Rocket

Page 6: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Flight of a Model Rocket

Page 7: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Forces at Liftoff

Page 8: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Acceleration at Liftoff

Page 9: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Forces in Powered Flight

Page 10: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Forces in Coasting Flight

The rocket uses up all its fuel, the engine goes out and the thrust goes to zero

Page 11: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Forces during Recovery

Page 12: Gas Dynamics-Rocket Propulsion

Rocket Propulsion-Introduction Cont..

GDJP Anna University

Terminal Velocity

Page 13: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Types

GDJP Anna University

Rockets can be classified by

A.Based on source of energy1. Chemical Rockets 2. Solar Rockets 3. Electrical Rockets

4. Nuclear Rockets

B.Based on propellant1. Liquid propellant 2. Solid propellant 3. Hybrid propellant

C.Based on application field1. Space rocket 2. Military rocket 3. Aircraft rocket 4. Booster rocket

D.Based on number stage 1. Single stage rocket 2. Multi stage rocket

E.Based on size and range1. Short range and small rocket 2. Long range and large rocket

Page 14: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Chemical Rocket Propellants

GDJP Anna University

Solid Propellant

Liquid Propellant

Propellant is a chemical mixture burned to produce thrust in rockets andconsists of a fuel and oxidizer

In a liquid system the fuel and oxidizer are separately stored and are sprayed under high pressure (20 to 60 bar) into the combustion chamber

In solid system, both fuel and oxidizer are contained in the propellant grain and the burning takes place on the surface of the propellant

Page 15: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Solid Propellant grains

GDJP Anna University

Well mixed fuel and oxidizer called as Propellant grain. Several grain configurations are employed to obtain burning at the desired rate.

Propellant cross section

Page 16: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Solid Propellants

GDJP Anna University

Exit velocity range1500 m/s to 3000 m/s

Star-grained solid rocket motor

Fuel : Plastic, Resin material

Oxidizer : Nitrates, Perchlorates

Page 17: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Hybrid Propellants

GDJP Anna University

Regulator

-

Liquidoxidizer

Oxidizer injector

Solid Fuel

Nozzle

Fuel : Solid type Oxidizer : Liquid type

Beryllium hydride(Be-H2 ) Fluorine(F2 )Lithium hydride (Li H) Chlorine Trifluoride(ClF3)Lithium hydride (Li H) Nitrogen tetroxide(N2O4 )Hydrocarbon(CH2)n Nitrogen tetroxide(N2O4 )

Special Type: Hypergolic propellants

Page 18: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Liquid Propellant Types

GDJP Anna University

Liquid Propellants

Monopropellant Bipropellant

Fuel and Oxidizer in a single chemical – MonopropellantsHydrogen peroxide (H2O2), Hydrazine (N2H4), Nitro methane (CH3NO2)

Fuel and Oxidizers are different in chemical - Bipropellants

Oxidizer Fuel mox/mf Combustion temperature (K)

Liquid Oxygen Gasoline, Hydrazine, UDMH, Ethanol

2.5, 0.92, 1.65, 1.8

3294, 34003600, 3422

Hydrogen Peroxide Hydrazine, UDMH

1.844.54

28172922

Nitric acid (RFNA) Aniline, Hydrazine

3.001.47

30453083

Page 19: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Propellant Properties

GDJP Anna University

Liquid Propellants1) Energy released during combustion should be high2) High density propellants are preferred3) Low freezing point propellants are preferred 4) Non-corrosive, chemically stable and should not absorb moisture5) Low values of vapor pressure and viscosity are preferred6) They should not be poisonous and hazardous7) It should be cheap and abundantly available

Solid Propellants1) Propellants should be easily available and safe to handle2) Physical and chemical properties should not change considerably during

processing as well as during time3) It should release large amount of heat energy during combustion4) They should be chemically inert before ignition5) Low molecular weight and high density of propellants are preferred6) Exhaust gases should be smokeless and colorless7) Propellants should not react with atmospheric air and moisture

Page 20: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Liquid Propellant feed system

GDJP Anna University

Page 21: Gas Dynamics-Rocket Propulsion

Liquid Propellant feed system - Cont..

GDJP Anna University

Page 22: Gas Dynamics-Rocket Propulsion

Liquid Propellant feed system - Cont..

GDJP Anna University

Pressure Fed system

Page 23: Gas Dynamics-Rocket Propulsion

Rocket Thrust

GDJP Anna University

Solid Motor

Liquid Motor

eAeceemm ..

Page 24: Gas Dynamics-Rocket Propulsion

Rocket Nozzle

GDJP Anna University

Page 25: Gas Dynamics-Rocket Propulsion

Rocket Nozzle- Function

GDJP Anna University

The function of the nozzle is to convert the chemical-thermal energy generated in the combustion chamber into kinetic energy.

The nozzle converts the slow moving, high pressure, high temperature gas in the combustion chamber into high velocity gas of lower pressure and temperature. Since thrust is the product of mass and velocity, a very high gas velocity is desirable.

The nozzle is usually made long enough (or the exit area is great enough) such that the pressure in the combustion chamber is reduced at the nozzle exit to the pressure existing outside the nozzle.

It is under this condition, Pe=Po, where Pe is the pressure at the nozzle exit and Po is the outside ambient pressure, that thrust is maximum and thenozzle is said to be adapted, also called optimum or correct expansion.

When Pe is greater than Po, the nozzle is under-extended. When the opposite is true, it is over-extended.

Page 26: Gas Dynamics-Rocket Propulsion

Rocket Nozzle- Function

GDJP Anna University

The most efficient nozzle (1) is contoured to the exhaust stream, allowing the escaping gas to expand just enough to fill the nozzle.

A nozzle that lets the gas expand too much (2), or too little (3), wastes the energy and thrust potential of the exhaust system.

The most efficient nozzle (1) is contoured to the exhaust stream, allowing the escaping gas to expand just enough to fill the nozzle.

A nozzle that lets the gas expand too much (2), or too little (3), wastes the energy and thrust potential of the exhaust system.

C-D Nozzle

Page 27: Gas Dynamics-Rocket Propulsion

Rocket Propulsion – Combustion-Liquid Propellant

GDJP Anna University

Combustion process involves: injection, atomization, mixing, vaporization, ignition andexothermic chemical reaction between fuel and oxidizer

Propellant Injectors

Page 28: Gas Dynamics-Rocket Propulsion

Rocket Propulsion – Solid Fuel Geometry

GDJP Anna University

A solid fuel's geometry determines the area and contours of its exposed surfaces, and thus its burn pattern. There are two main types of solid fuel blocks used in the space industry. These are cylindrical blocks, with combustion at a front, or surface, and cylindrical blocks with internal combustion.

In the first case, the front of the flame travels in layers from the nozzle end of the block towards the top of the casing. This so-called end burner produces constant thrust throughout the burn.

In the second, more usual case, the combustion surface develops along the length of a central channel. Sometimes the channel has a star shaped, or other, geometry to moderate the growth of this surface.

Page 29: Gas Dynamics-Rocket Propulsion

Rocket Propulsion – Solid Fuel Geometry- Thrust profile

GDJP Anna University

Cylindrical Channel – Progressive burning

Cylindrical Channel with central cylinder- Neutral burning

Star Profile Cruciform Profile – Regressive burning

Page 30: Gas Dynamics-Rocket Propulsion

Rocket Propulsion – Solid Fuel Geometry- Thrust profile

GDJP Anna University

Double anchor profile

Cog profile

Page 31: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Solid motor- Combustion

GDJP Anna University

Linear burning rateThe burning rate of the propellant grain depends on the initial temperature of the grain before combustion, equilibrium combustion pressure and the ratio of grain surface area and the nozzle throat area.

The burning surface of a rocket propellant grain recedes in a direction perpendicular to this burning surface. The rate of regression, typically measured in millimeters per second (or inches per second), is termed burn rate.

The linear burning rate is given by, Saint-Roberts law (regression law)where r- burn rate ; a-burn rate coefficient ; Pc - combustor pressure

n-pressure exponent (range 0.2 to 0.8)a =f (chemical composition, initial temperature of the propellant grain )n =f( combustor pressure)

ncaPr

Combustion limitSolid propellant grain requires certain minimum value of the combustion pressure for stable combustion. This minimum value of the pressure is known as the combustion limit ( it depends on type of propellant employed)

Usually it lies between the range of 5 and 55 bar

Page 32: Gas Dynamics-Rocket Propulsion

Rocket Propulsion- Solid motor- Combustion

GDJP Anna University

Propellant consumption rate, cAncPacrAcm

.

.

Propellant flow rate, (1))(cm Vdt

dpm

. .

mass of gas in bore

mp

.

Equilibrium Combustion Pressure

Page 33: Gas Dynamics-Rocket Propulsion

Solid motor- Combustion Cont..

GDJP Anna University

Propellant area ratio

The ratio of the surface area available for burning of a propellant grain and the throat area of the exhaust nozzle is known as the propellant area ratio ( Kp)

*A

cApK r and Kp increase with the combustion pressure

Page 34: Gas Dynamics-Rocket Propulsion

Rocket Nozzle- Function

GDJP Anna University

The function of the nozzle is to convert the chemical-thermal energy generated in the combustion chamber into kinetic energy.

The nozzle converts the slow moving, high pressure, high temperature gas in the combustion chamber into high velocity gas of lower pressure and temperature. Since thrust is the product of mass and velocity, a very high gas velocity is desirable.

The nozzle is usually made long enough (or the exit area is great enough) such that the pressure in the combustion chamber is reduced at the nozzle exit to the pressure existing outside the nozzle.

It is under this condition, Pe=Po, where Pe is the pressure at the nozzle exit and Po is the outside ambient pressure, that thrust is maximum and thenozzle is said to be adapted, also called optimum or correct expansion.

When Pe is greater than Po, the nozzle is under-extended. When the opposite is true, it is over-extended.