Advances in Rocket Propulsion
Dr K Ramamurthi, Non-member
The state-of-the art technology in propulsion is briefly reviewed in this article. The application and future growth of rocket
propulsion for launch vehicle and spacecraft applications are also disscused. The power density of rockets is seen to be a
limiting factor and the growth with energetic materials, vortex combustion and water for propulsion is discussed. The
application of nano-technologies, non-chemical propulsion and propellantless propulsion is also discussed.
Keywords: Rocket propulsion; Launch vechicle; Spacecraft application; Chemical propulsion; Nano-technology
Dr K Ramamurthi is with Liquid Propulsion Systems Centre, ISRO,
Trivandrum 695 547.
This paper was presented and discussed at the All-India Saminar on
Aircrafts and Trans-atmospheric Vehicles : Missions, Challenges and
Perspectives held at Kolkata during May 28-29, 2004.
INTRODUCTION
Advances signify improvements and this review of Advances
in Propulsion deals mainly with methods of improving the
performance of rockets used in launch vehicles and satellites.
Improvements are mainly aimed to make the launch vehicle
and satellite less-expensive to fly and to achieve better
reliability. Additional factors, such as, safety and an eco-
friendly propulsion system are also important. The advances,
are not meant to have a sophisticated or complex system and the
pursuit is essentially to have a simple and rugged system that
propels efficiently.
The pioneers in rocket propulsion, such as, Tsialkowsky,
Goddard and Oberth dreamt of and conceived very innovative
propulsive devices for space applications in the early part of the
twentieth century. These devices have been developed in the
twentieth century and scaled-up and also applied successfully
for various space missions including planetary missions. India
has also successfully employed solid and liquid propellant
rockets for launching satellites in different orbits. Liquid-
fuelled rockets have been used for station keeping and orbit
control of satellites. Advanced propulsion involving electrical
propulsion is to be employed in some of the upcoming Indian
geostationary class of satellites.
The application of revolutionary thoughts, based on advances
in physical sciences, could assist in radical changes in the
propulsion systems and help in major innovations. Innovative
research using new concepts is to be preferred over the
conventional mundane method of improving by incremental
stretching of performance using small modifications and
improvements over the present propulsion modules. The scope
of such innovations are specifically addressed in this article.
Propulsion involves locomotion or movement. Everyone is
familiar that a less efficient system can do the job of locomotion
of a more efficient one if the less efficient one is made larger,
that is, stronger. This is a damper for innovative development in
propulsion and the objective of propelling satellites into orbit
can do a large extent be met by larger and somewhat less
efficient propulsive devices compared to advanced propulsion
systems, which are possible to be developed based on current
technologies. However, the missions using less efficient devices
become not only unduly costly but have limitations in terms
longer durations and smaller pay-load capability. For certain
high demanding missions involving interplanetary or
interstellar travel, a very high performance propulsion system
having grossly improved characteristics is required. These
aspects dictate the direction of the advances in propulsion.
CHEMICAL PROPULSION AND POWER DENSITY
OF COMBUSTION
In this section, classification of chemical propulsion, along with
the details of solid and liquid propellants liquids is discussed.
Classification of Chemical Propulsion
The heat release from the chemical reactions between a fuel and
an oxidizer has invariably been used for generating high
pressure and high temperature gases which produce the thrust
or locomotion for propulsion. The solid propellant rocket are
fed with fuel and oxidizer in a solid form, whereas if the fuel and
oxidizer are stored as liquids before being brought together for
burning in a combustion chamber, the rocket is known as a
liquid propellant rocket. Certain fuels and oxidizers (which are
in gaseous form at ambient temperatures and pressures) need to
be stored at very low temperature in order to use them as
liquids. Rockets using these low temperature liquid fuels and
oxidizers are called cryogenic propellant rockets. These low
temperature cryogenic fuels are stored in insulated containers.
Application of Solid and Liquid Propellant Rockets
A large number of rockets have been developed using solid,
liquid and cryogenic propellants. Rockets generating very large
thrust (thrust of several thousand kN) and very small thrust
(thrust about a fraction of a Newton) have been made. Rockets
having large values of thrust are used for boosters of launch
vehicles whereas very small thrust rockets are used for
spacecraft propulsion and control. New types of fuels have been
tried and very high performance cryogenic propellant rockets
using liquid hydrogen and liquid oxygen have been developed.
54 IE (I) JournalAS
Figure 1 shows the evolution of satellite launch vehicles in
India. Solid rockets were used for sounding rockets and for the
rocket stages of the Indian launch vehicles SLV-3 and ASLV.
Liquid rockets stages were used along with solid propellant
rockets in the polar satellite launch vehicle (PSLV). The liquid
rockets used earth storable propellants di-nitrogen tetroxide for
oxidizer and dimethyl hydrazine for fuel. The requirements of
larger orbital velocities for geo-synchronous missions and the
pay-load requirements demanded the higher performance of
the cryogenic propellant rockets in order to avoid a large lift off
mass and an inefficient and costly vehicle. The geo-
synchronous satellite has cryogenic propellant rocket for its
upper stage, earth storable propellant rockets for the second and
strap on stages and a high thrust solid propellant rocket for the
booster stage.
Implications of High Power Density
The high performance rockets release their chemical energy in
a small combustion volume giving very high values of power
density of the chemical energy release rates. The power density
of a rocket has gone up substantially during the last sixty years.
At present, it is some thousand times higher than it was for the
first operational liquid propellant rocket (V2) developed in the
1940s and used during World War II. Figure 2 compares the
power density of rockets with those of other propulsive devices.
A typical automobile engine such the Maruti 800 has a power
density of about 0.04 kW/cm3. The power density of a high
performance large rocket, such as, the RD170 Zenith rocket,
which produces a thrust of 7250 kN at a chamber pressure of
24.5 MPa is 103 kW/cm3. This is very near to the power density
of a detonation and is indicative of the almost explosive nature
of the heat release.
High values of power densities signify that larger amounts of
energy are released faster in a smaller volume. The
temperatures and heat transfer rates would, therefore, be
significantly higher. Better methods of cooling the rocket
chamber and use of special materials of construction become
essential to contain the high power densities. Means of
controlling the combustion also become necessary since even if
a small fraction of the high power were to excite the chamber
acoustics and vibration, it would spell disaster. If advances in
high performance rockets are required with an increase of the
power density through use of higher pressures and
temperatures, one needs to specifically address the possibilities
of combustion control and improved methods of cooling. The
subject of active combustion control is currently of topical
interest and is vigorously pursued.
Vortex Rocket
Cooling of the rocket chamber, however, invariably leads to
losses. A new concept of a Vortex rocket in which the fuel is
introduced in a rotating or vortex motion is shown in Figure 3.
The fuel cools the chamber walls before being burnt with
oxygen in the core. The centrifugal forces associated with the
higher density low temperature fuel keeps the hot gases away
from walls. The subject of vortex combustion with the
Figure 1 Solid and liquid propellant rocket applications
Vol 85, November 2004 55
Figure 2 Power densities in different propulsive devices
associated large characteristic lengths and improved flame
stability is exciting and is a promising contender for the future.
IMPROVING PERFORMANCE OF CHEMICAL
PROPULSION
The efficiency of conversion of chemical energy of fuel into
heat is of the order of 99% in the modern day rockets. If the
performance of the chemical propulsion rocket is to be
improved, then the important step is to improve the energy
content of the fuel since the conversion efficiency is already high.
Metal Addition to Improve Performance
The cryogenic propellant combination of liquid hydrogen and
liquid oxygen gives high performance since the molecular
weight of the products of combustion is low leading to low
densities and high exhaust jet vehicles. Metals have high values
of stored energies and the possibilities of adding metal powders
to rocket fuels to improve the performance have always been of
interest. With solid propellants (which have somewhat lower
performance) the metal addition leads to enhanced values of the
performance. However, the enhancement in performance of the
liquid propellant rockets is not very significant since the
amount of increase in molecular weight of the combustion
products is higher as compared to solid propellant rockets.
The changes in performance of liquid propellant rockets from
56 IE (I) JournalAS
V2 Rocket
Turbojets
IC Engine
Rockets
Gas turbine
RD 170 Zenit Rocket
Detonative Combustion
Maruti car
kW/ cm3
102 101 1 1021 0 10
3
Fuel or Oxygen
Oxygen or Fuel
Figure 3 Vortex rocket diagram
adding aluminium to kerosene and hydrogen fuel is shown in
Figure 4. The metals of interest are those of lower atomic mass,
such as, beryllium, boron, lithium, magnesium and aluminium.
Tri-propellant Rockets
The use of hydrogen along with fuels, such as, kerosene helps in
improving the performance of the kerosene fuels used for
booster propulsion. The rockets employing two fuels, (namely,
kerosene and hydrogen) with an oxidizer are spoken of as
tri-propellant rockets. Such rockets can start in a tri-propellant
mode for booster and transit to a high performance bi-
propellant mode (using hydrogen and oxygen). The application
of such tri-propellant rockets has been promising. However,
though a large amount of initial research on tri-propellant
rocket was witnessed a decade earlier, not much flurry of
activity is currently seen for developing tri-propellant rockets.
Increasing Energetics of Propellants
A novel method of adding energy to a fuel is by straining its
chemical bonds. When the standard angle of 108.50 in the
hexagonal bond structure in a hydrocarbon molecule is charged
to form triangles, squares and tetrahedrons, a net increase in
the energy content of the fuel results. Strain energies of
about 40 kcal/mol to 100 kcal/mol have been claimed.
However, such fuels tend to be unstable and soot readily when
burning. Further research study is required before they could
be applied in liquid propellant rockets.
Rather than use of strained fuels, the possibilities of using the
fuel in the atomic state is of interest since the energy content is
several orders of magnitude higher. Thus, if atomic hydrogens
were to be used for fuel instead of molecular hydrogen, the
energy release rate would be almost 20 times higher giving an
order of magnitude increase in the specific impulse
performance parameter. But then the storage of atomic
PP
V V
Brayton Cycle Atkinson Cycle
Figure 5 Brayton and Atkinson cycles
hydrogen is difficult and special traps with high magnetic fields
at temperatures close to zero Kelvin are necessary. Similarly,
the use of metallic hydrogen, formed when the solid hydrogen
is compressed under very high pressure at Mega bar level would
have intense locked up energy and contribute to the making of a
very high performance propulsion system. Even solid hydrogen
could be used and a proposal was put up by a German Scientist
to use it as a solid propellant.
Atkinson Cycle and Pulse Detonation Engines
The energy is added in the rocket at constant pressure, such as,
in the Brayton cycle. Energy addition at constant volume is
more efficient for a given compression. The Atkinson cycle,
which uses constant volume heat addition (Figure 5) gives an
improvement by about 18% to 25% over Brayton cycle depending
on the pressure and temperature. In the case of the constant
volume combustion rocket, the fuel and oxidizer can also be
admitted into the chamber at low pressures and the associated
feed system can be made much simpler. The burning at constant
volume marks a jump in pressure at which the burnt gas is
discharged out through the nozzle.
As an extension to the constant volume combustion, the use of
detonative combustion in a pulsed constant volume combustor
has attracted significant attention. The rockets using this
principle are known as pulse detonation engines. A number of
technologies, such as, extremely high mixing rates under
unsteady conditions, flow control, vibration attenuation and
rapid deflagration to detonation transition need to be
established to make the system viable. The products of
combustion have also to be aspirated out of the chamber after
the detonation. Pulse detonation engines have been
demonstrated with gaseous fuels for cyclic operation up to 100 Hz.
The aim of the pulse detonation engine is to have a simplified
rocket system, which can operate at low feed pressures with
lean fuels and high power densities and efficiencies.
AIR BREATHING AND REUSABILITY
In this section, air breathing and in situ production of
propellants along with reusability details are discussed.
Air Breathing and In-situ Production of Propellants
The fractional weight of the pay-load, the structure, and the fuel
and oxidizer in a typical launch vehicle are shown in Figure 6.
It is seen that the oxygen content is about 70%. If this oxygen can
Vol 85, November 2004 57
Lox/ Kerosene with Aluminium
Lox/ LH2 with Aluminium450
400
350
300
250
200
0 1 2 3 4 5 6 7 8
Mixture Ratio
P C = 100 bar
Sp
ec
ific
Im
pu
lse
, s
10 % AL
5 % AL
2 % AL
0 % AL
10 % AL
5 % AL
2 % AL
0 % AL
Figure 4 Influence of metal addition to liquid fuels
be drawn from the atmospheric air, the rocket weight and,
hence, the cost of the rocket can be brought down. The
incorporation of air-breathing propulsion for the space vehicles
with the take-off using turbojets, turbofans or ejector ramjets
followed by ramjets, scramjets and rockets has been the subject
of intense debate over the last thirty years. Combined cycle
engines transitioning from one phase of operation to the other
have been proposed. Even the possibility of collecting air,
liquefying it and then using it for a rocket mode has been
suggested. This constitutes the Liquid Air Cycle Engine
(LACE). The major issue is the difficulty of a low weight
compact-heat exchanger for the liquefaction.
The principle of collecting oxygen has been extended to in-situ
propellant production for vehicle returning from planet Mars.
The liquid hydrogen taken by the vehicle is used for reacting
with the carbon dioxide gas atmosphere over Mars. The
methane and oxygen so formed are liquefied and stored in
insulated tanks for the Mars Ascent Vehicle (MAV).
Reusability
Figure 7 shows the approximate cost distribution in a launch
vehicle. The major cost is towards the hardware (about 70%)
while the balance is the cost of propellants and pay-load. A
major saving in the cost is, therefore, possible if the hardwares
are to be repeatedly reused. The space shuttle of the USA and
Buran of Russia represented the first efforts to partially reuse
the hardwares. Subsequently, a large number of experimental
configurations like the use of throttleable liquid rockets air-
launched from an aircraft, and use of ramjets and scramjets have
been toyed with during the last twenty years. These comprise of
a reusable vehicle with cryogenic rockets for vertical take-off
and landing known as Delta Clipper, the take-off as a rocket and
landing as an helicopter (as in Roton) and the more
conventional two stage-to-orbit propulsion vehicle comprising
a hypersonic aircraft with ramjet and a rocket powered upper
stage (Sanger). Several such configurations have been discussed
and the use of adapted nozzles, such as, plug nozzle, aerospike
nozzle and linear aerospike nozzles has been experimented.
The single stage to orbit does not appear to be a promising
reusable vehicle. The use of air-launch, which not only gives an
initial velocity to the vehicle, but also operates it in a reduced
drag environment seems to be a promising option.
WATER FOR PROPULSION
The possibilities of using water as a source of chemical energy
was first put forward by the science fiction author Jules Verne
in 1870 in the book The Mysterious Island. The author wrote
I believe that water will one day be employed as fuel, that
hydrogen and oxygen which constitute it, used singly or
together, will furnish an inexhaustible source of heat and light
.... Studies on efficiently splitting water into hydrogen and
oxygen using different methods, such as, bond-breaking,
electrolysis, thermo-chemical and hybrid processes are in
progress. Certain semi-conductors, when illuminated, break-up
water by photolysis. The hydrogen and oxygen, thus generated
from the water, can be combined chemically to give thrust as in
chemical propulsion.
The use of fuel cells that store the solar energy during the day by
electrolyzing water into hydrogen and oxygen and then
converting the gases back into water to generate electricity is
being demonstrated. Regenerative fuel cells with capacities of
600 W-h/kg are developed. Considerable developments are also
made in the polymer electrolyte membrane and it should be
possible to use such cells in the next generation of geo-
synchronous satellites. The hydrogen and oxygen from the
water can, therefore, be also used for propulsion control of
satellites.
PROPULSION SYSTEMS FOR SATELLITE
In this section, propulsion control for both the large satellites
and the small satellites are discussed.
Propulsion Control for Large Satellite
Chemical rockets (both mono-propellant and bi-propellant) for
the Indian Remote Sensing (IRS) and Indian National Satellites
(INSAT) are being used at present. The electrical propulsion
58 IE (I) JournalAS
Structure (13 %)
Hydrogen (15 %)
Pay-load (2 %)
Oxygen (70 %)
Figure 6 Typical weight distribution in a launch vehicle
Figure 7 Typical cost distribution of a launch vehicle
Propellant (15%–20%)Pay-load (15% – 18%)
Hardware
(70 %)
system, namely, the stationary plasma thruster within two
years in Geostationary Satellites (GSAT) can be attempted for
this purpose. If one looks at the future aspects of satellites, the
continution of using heavy satellites for geosynchronous and
polar missions can be tried in future too. For these large
satellites, the propulsion would probably continue to be with
electrical and chemical nature with improvement in performance
for a prolonged lifetime of the satellites. The thrust levels
available with the chemical propulsion make them attractive
for the heavy satellites. The use of water for propulsion is
attractive since the fuel cells can use water and the hydrogen
and oxygen from the water can be used for propulsion.
Propulsion for Small Satellit