mae 5391: rocket propulsion overview of propulsion systems

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MAE 5391: Rocket Propulsio Overview of Propulsion Sys

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Page 1: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

MAE 5391: Rocket PropulsionOverview of Propulsion Systems

Page 3: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Propulsion Technology Options

Thermodynamic Systems (TE KE) Cold Gas Thrusters Liquids

• Monopropellants• Bipropellants

Solids Hybrids

Nuclear (NE TE KE) Electric Systems

Electrothermal (Resistance Heating) Electrostatic (Ion with E field F=qE) Electromagnetic (plasma with B field F=JxB)

With the exception of electrostatic and electromagnetic, all use concept of gas at some temp flowing though a converging/diverging nozzle!

Page 4: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Chemical Limitations

Why we have thermo!

])(1[)1(

2 /1

0

0

p

p

M

TRV

euexit

Vexit= nozzle exit velocity (m/s)

Ru= universal gas constant (8314.41 J/kmol*K)

T0= chamber temperature (K)

Pe= exit pressure (Pa)

P0= chamber pressure (Pa)

M= molecular mass of gas (kg/kmol)g= ratio of specific heats (no dimensions)

Page 5: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Cold Gas

Gas MolecularWeight

SpecificImpulse (sec)

Air 28.9 74

Argon 39.9 57

CO2 44.0 67

Helium 4.0 179

Hydrogen 2.0 296

Nitrogen 28.0 80

Methane 16.0 114

1.5 litre X 600 barNitrogen tanks

Fill/drain valve

Two stage regulator (feed pressure ~ 4bar)

Thruster (0.01N,1.3 *10-5 kg/s,throat diameter0.0133 cm)

Stop valve

Microsat cold gaspropulsion systemlayout proposal

Cold Gas: Expand a pressurized gas through a nozzle

Page 6: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Liquid Monopropellant

Parameter Value

Catalyst LCH 227/202

Steady-state thrust (N) 11.1 - 31.2

Isp (sec) 228 - 235

Propellant specific gravity 1.023

Average Density Isp ( sec) 236.8

Rated total impulse (Nsec) 124,700

Total pulses 12,405

Minimum impulse bit (Nsec) 0.56

Feed pressure (bar) 6.7 - 24.1

Chamber pressure (bar) 4.5 - 12.4

Nozzle expansion ratio 61:1

Mass flow rate (gm/sec) 5.0 - 13.1

Valve power 27 W max @ 28 VDC

Thruster mass (kg) 0.52

3 N2H4 4 NH3 + N2 + 336,280 joules

MonoProp: Decompose a single propellant and expand the exhaust through a nozzle

Page 7: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Liquid Bi-Propellant

Storable Isp 250-320 sec

finert=0.03-.13

Cryogenic Isp 320 – 452 sec

finert=0.09-0.2

BiProp: Combust (burn) two propellants (fuel + oxidizer) in a combustion chamber and expand exhaust through a nozzle

Finert = 0.04-0.2 Finert=0.11-0.31

Page 8: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Solids

Composite propellant, consisting of an oxidizing agent, such as ammonium nitrate or ammonium perchlorate intimately mixed with an organic or metallic fuel and binder.

Thrust function of burn area, Isp = 250-300 sec

Finert=0.06-0.38, 2/3 of motors have fiinert below 0.2

AdvantagesSimpleReliableHigh density IspNo chamber cooling

DisadvantagesCracks=disasterCan’t restartHard to stopModest Isp

Page 9: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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When solids go bad!

Page 10: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Hybrids

Isp= 290-350 sec

Finert=0.2

Hybrid: Bipropellant system with liquid oxidizer (usually) and a solid fuel

Catalyst Pack

Combustion Chamber

Nozzle

Test Stand

Load Cell

Fuel Element

H2O2/PE Hybrid Test Set-Up

Polyethylene fuel rod

Page 11: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Nuclear Thermal Propulsion

NERVA Program Thrust = 890,000N Isp = 838 sec Working fluid = Hydrogen Test time = 30 minutes Stopped in 1972 Finert=0.5-0.7 (shielding)

Page 12: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Electrothermal-Resistojets

Nozzle

Thermocouple tapping

Stainless steel outer1225W Cartridge heater

Water inlet

Heater thermocouple

Power inputSintered stainlesswater distribution ring

Sintered stainless filterPressure tapping

SiC Heat transfer medium

Cutaway of Mark- III Resistojet

Working Fluid

Thrust (mN) Isp (sec) Power (W) Cp (kJ/kg K) Tc (K)

hydrogen 37 546 100 14.32 1000

water 93 219 100 2.3 1000

nitrous oxide 141 144 100 1.0 1000

Electrothermal-- electrical energy is used to directly heat a working fluid. The resulting hot gas is then expanded through a converging-diverging nozzle to achieve high exhaust

velocities. These systems convert thermal energy to kinetic energy

Page 13: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Electrothermal-Arcjets

In an arcjet, the working gas is injected in a chamber through which an electric arc is struck. The gas is heated to very high temperature (3000 – 4000 K), Arc temp =10,000K on average, and much greater in certain regions in the arc.

Power = 1.8 kW, Isp = 502, Thrust = 0.2N, Propellant = hydrazine

Page 14: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Electrostatic-Ion Propulsion

Electrostatic-- electrical energy is directly converted into kinetic energy. Electrostatic forces are applied to charged particles to accelerate the propellant.

Deep Space 1 = 4.2 kW, Thrust = 165 mN, Isp = 3800 sec

7000 hours of operation is becoming the standard!

Page 15: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Electromagnetic-MPD Thruster

Electromagnetic-- electromagnetic forces directly accelerate the reaction mass. This is done by the interaction of electric and magnetic fields on a highly ionised propellant plasma.

NH3 MPD, F=23 mN, Isp= 600 sec, P=430 W

Stuttgart, Isp=5000sec, F=100N, P=6 MW, hydrogen

Page 16: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Pulsed Plasma Thrusters

Ctrigger

CMain

Rtrigger

CenterElectrode

IntermediateElectrode

OuterElectrode

Teflon Annulus

PPUSpacecraft

Ground

Isp = 500-1500 sec

P = 1 – 100 W

Thrust = 5mN/W

Page 17: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Hall Effect Thruster

Power = 50W – 25kW

Isp = 500 – 3000 sec

Thrust = 5 mN- 1N

Page 18: MAE 5391: Rocket Propulsion Overview of Propulsion Systems

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Propulsion System “Cost”

Performance issues Mass Volume Time (thrust) Power Safety Logistics Integration Technical Risk

The “best” (lowest “cost”) option optimizes these issues for a given set of mission requirements