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Abstract

Cryogenic propulsion systems using liquid hydrogen and liquid oxygen propellant combination are used in satellite launch vehicles in view of the higher specific impulse (ISP). Due to extreme low temperature of cryogenic propellant and low density and explosive nature of LH2, the development of cryogenic propulsion system is very complex and time consuming. In ISRO an indigenous cryogenic upper stage powered by an engine developing a nominal thrust of 73.5 kN in vacuum with a propellant loading of 12.8 tonnes is developed and successfully flight tested for the first time in GSLV D5 flight on 5th January 2014. A mathematical model is developed for finalizing the engine start and shut off sequence, ensuring smooth and safe ignition, predicting performance of subsystems under transient phase, nominal and off nominal conditions, control systems parameter settings and for the performance estimation of engine in sea level and flight. This paper highlights the configuration and working of a cryogenic engine, mathematical modelling of the engine, applications of the model in the cryogenic engine development and comparison of predicted values with the test results.

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Abbreviations

PC :

Main engine chamber pressure

PGGE:

Gas generator chamber pressure

PFPI:

Pressure at main fuel pump inlet

PHPD:

Pressure at main fuel pump delivery

POPI:

Pressure at main oxidizer pump inlet

POPD:

Pressure at main oxidizer pump delivery

PHCHE:

Pressure of hydrogen at coolant channel exit

POME:

Pressure of LOX at the exit of mixture ratio controller

PGTE:

Pressure at the exit of main turbine

POAE:

Pressure of LOX at the exit of absolute velocity regulator

PHBTI:

Pressure at hydrogen booster turbine inlet

PHBTD:

Pressure at hydrogen booster turbine exit

PFBO:

Pressure at fuel booster pump outlet

POBTI:

Pressure at oxygen booster turbine inlet

POBO:

Pressure at oxygen booster pump outlet

TFPI:

Fluid temperature at main fuel pump inlet

TOPI:

Fluid temperature at main oxidizer pump inlet

TOPD:

Fluid temperature at main oxidizer pump delivery

THCHE:

Fluid temperature of hydrogen at coolant channel exit

THBTD:

Fluid temperature at hydrogen booster turbine exit

mlox :

LOX flow rate

mf :

Hydrogen flow rate

ME:

Main engine

GG:

Gas generator

OBT:

Oxidizer booster turbine

FBT:

Fuel booster turbine

SE:

Steering engine

MOP:

Main oxidizer pump

V, U:

Velocity

f:

Friction factor, body force

L:

Length

At :

Throat area

A:

Turbine nozzle area

C*:

Characteristic velocity

hg:

Gas side convective heat transfer coefficient

hc:

Coolant side heat transfer coefficient

qc:

Heat flux due to convection

qr:

Heat flux due to radiation

q:

Combined heat flux

k:

Conductivity of the material

t:

Shell thikness

ηf:

Fin effectiveness

H:

Total enthalpy

C:

Concentration

τ:

Shear stress

μ:

Viscocity

ρ:

Density

P:

Pressure

Q, R:

Source terms

h:

Static enthalpy

E:

Total energy

e:

Internal energy

J:

Diffusion flux

References

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Correspondence to K. S. Bijukumar.

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Narayanan, V., Suresh, M.S., Jayan, N. et al. Mathematical modelling of a cryogenic engine. Int J Adv Eng Sci Appl Math 6, 183–194 (2014). https://doi.org/10.1007/s12572-015-0117-2

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  • DOI: https://doi.org/10.1007/s12572-015-0117-2

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