Time Travel Research Center
© 2005
Cetin BAL - GSM:+90 05366063183 - Turkey/Denizli
Engine List
The RS 10 from Star Born by Andre Norton, 1957
Judging from the size of the people, the ship is approximately 70
meters high (240 feet)
You can spend lots of time researching spacecraft propulsion systems.
But you are in luck, I've got some data for you. Most of this is from
Philip Eklund's invaluable boardgame
ROCKET
FLIGHT. (order
here),
the impressive Spaceship
Handbook, and the indispensable
Space
Propulsion Analysis and Design. The rest is from various places I
found around the internet, and no, I didn't keep track of where I got
them from. Use at your own risk.
If you don't like the values in the table, do some research to see if
you can discover values you like better. Also note that the designs in
the list are probably optimized for high exhaust velocities at the
expense of thrust. There is a chance that some can be altered to give
enough thrust for lift-off at the expense of exhaust velocity.
Some engines require electricity in order to operate. These have
their megawatt requirements listed under "Power Requirements". With
these engines, the Engine Mass value includes the mass of the power
plant (unless the value includes "+pp", which means the mass value
does NOT include the mass of the power plant). The
power plant mass can be omitted if the spacecraft relies on beamed power
from a remote power station. Alas, I could find no figures on the mass
of the power plant. If the plant is nuclear, it probably has a mass of
around 0.5 to 10 tons per megawatt. I agree, that isn't much help. Sorry.
Efficiency is the percentage of the power requirements megawatts that
are actually turned into thrust. The rest becomes waste heat and has to
be removed with heat radiators.
T/W >1.0 = Thrust to Weight ratio greater than zero?
This boils down to: can this be engine be used to take off from the
Earth's surface? If the answer is "no" use it only for orbit to orbit
maneuvers. It is calculated by figuring if the given thrust can
accelerate the engine mass greater than one gee of acceleration.
Most propulsion systems fall into two categories: SUV and economy.
SUV propulsion is like an SUV automobile: big and muscular, but the
blasted thing gets a pathetic three miles to the gallon. Economy
propulsion has fantastic fuel economy, but has trouble climbing low
hills. In the world of rockets, good fuel economy means a high "specific
impulse" (Isp) and high exhaust velocity. And muscle
means a high thrust.
The only vaguely possible propulsion system that has both high
exhaust velocity and high thrust is the Nuclear Salt Water Rocket, and
not a few scientist have questions about its feasibility. Well, actually
there also is Project Orion, but that has other problems (see below).
In science fiction, one often encounters the legendary "fusion drive",
which is a high exhaust velocity + high thrust propulsion system that
modern science isn't sure is even possible.
From my limited understanding, the basic problem is how to keep the
engine from vaporizing.
Fp = (F * Ve ) / 2
where
Fp = thrust power (watts)
F = thrust (newtons)
Ve = exhaust velocity (m/s)
The problem is that at high enough values for exhaust velocity and
thrust, the amount of watts in the jet is too much. "Too much" is
defined as: if only a fractional percentage of those watts are lost as
waste heat, the spacecraft glows blue-white and evaporates. The size of
the dangerous fractional percent depends on heat protection technology.
There is a limit to how much heat that current technology can deal with,
without a technological break-through.
chart from "The Atomic Rocket" by L. R. Shepherd,
Ph.D., B.Sc., A.Inst.P., & A. V. Cleaver, F.R.Ae.S., 1948. Collected
in Realities of Space Travel
Jerry Pournelle says (in his classic A STEP FARTHER OUT)
that an exhaust velocity of 28,800,000 cm/s corresponds to a temperature
of 5 million degrees Kelvin.
As an exceedingly rough approximation:
Ae = (0.5 * Am * Av2)
/ B
where
Ae = particle energy (degrees Kelvin)
Am = mass of particle (g) (1.6733e-24
grams for monatomic hydrogen)
Av = exhaust velocity (cm/s)
B = Boltzmann's constant: 1.38e-16 (erg K-1)
(note that the above equation is using centimeters per second, not
meters per second)
A slightly less rough approximation:
Qe = (Ve / (Z * 129))2 * Pw
where
Qe = engine reaction chamber temperature (degrees Kelvin)
Ve = exhaust velocity (m/s)
Z = heat-pressure factor, varies by engine design, roughly from 1.4 to
2.4 or so.
Pw = mean molecular weight of propellant, 1 for atomic
hydrogen, 2 for molecular hydrogen
The interior of stars are 5 million degrees Kelvin, but few other
things are. How do you contain temperatures of that magnitude?
If the gadget is something that can be mounted on a ship smaller than
the Queen Mary, it has other implications. It is an obvious defense
against hydrogen bombs, for starters.
Larry Niven postulates something like this in his "Known Space"
series, the crystal-zinc tube makes a magic force field which reflects
all energy. Niven does not explore the implications of this. However,
Niven and Pournelle do explore the implications in THE MOTE IN
GOD'S EYE. The Langson Field is used in the ship's drive, and as a force
screen defense. The Langson field absorbs energy, and can re-radiate it.
As a defense it sucks up hostile laser beams and nuclear detonations. As
a drive, it sucks up and contains the energy of a fusion reaction, and
re-radiates the energy as the equivalent of a photon drive exhaust.
(And please remember the difference between "temperature" and "heat".
A spark from the fire has a much higher temperature than a pot of
boiling water, yet a spark won't hurt your hand at all while the boiling
water can give you second degree burns. The spark has less heat, which
in this context is the thrust power in watts.)
In his Known Space novels, Larry Niven invented The Kzinti Lession.
It states that the more efficient a reaction drive is, the better a
weapon it makes. The warlike Kzinti invaded the solar system, figuring
that humanity would be a pushover since the pacifist humans of the time
had no weapons. Humans showed the Kzin the error of their ways by
annihilating Kzinti warships with laser arrays used for solar sails,
multi-million degree fusion exhausts, and photon drives that were
basically titanic lasers. So keep in mind that the higher the exhaust
velocity of the rocket engine, the more damage it will do to anything
unfortunate enough to be in the path of the exhaust.
All drives listed in the table who's names end in "MAX" require some
sort of technological breakthrough to to prevent the engine from
vaporizing.
If these figures result in disappointing rocket performance, in the
name of science fiction you can tweak some of them and claim it was due
to a technological advance. You are allowed to tweak anything who's name
does not end in "MAX". You can alter the Thrust, Engine
Mass, and/or the Eff, but no other values. If there is a corresponding "MAX"
entry for the engine you are tweaking, you cannot alter any of the
values above the "MAX" entry (i.e., you are not allowed to tweak NTR-SOLID-DUMBO's
thrust above 7,000,000, which is the value in the NTR-SOLID MAX entry).
The engines are sorted by thrust power, since that depends on both
exhaust velocity and thrust. So engines that high in both of those
parameters will be towards the end of the list. This is useful for
designers trying to make spacecraft that can both blast-off from a
planet's surface and do efficient orbital transfers.
If one was trying to design a more reasonable strictly orbit-to-orbit
spacecraft one would want the engine list sorted by exhaust velocity.
And surface-to-orbit designers would want the list sorted by thrust.
Propulsion System |
Thrust
Power
(GWatts) |
Exhaust
velocity
(m/s) |
Thrust
(newtons) |
Engine
mass
(tons) |
T/W
>1.0 |
Power
req
(MWatts) |
Eff |
VASIMR (high gear) |
0.00005 |
500 |
200 |
10+pp |
no |
10 |
? |
VASIMR (med gear) |
0.00007 |
1,500 |
100 |
10+pp |
no |
10 |
? |
VASIMR (low gear) |
0.00006 |
3,000 |
40 |
10+pp |
no |
10 |
? |
ArcJet |
0.011 |
22,000 |
1000 |
15 |
no |
30 |
48% |
AIM |
0.016 |
598,000 |
55 |
? |
no |
|
|
Solar Moth |
0.018 |
9,000 |
4,000 |
0.1 |
no |
Sunlight |
63% |
Colloid Electrostatic |
0.17 |
43,000 |
8000 |
20 |
no |
200 |
85% |
J x B Electric |
0.19 |
74,000 |
5,000 |
110 |
no |
211 |
80% |
NTR-SOLID (H2) |
|
8,093 |
|
|
|
|
|
NTR-SOLID (CH4) |
|
6,318 |
|
|
|
|
|
NTR-SOLID (NH3) |
|
5,101 |
|
|
|
|
|
NTR-SOLID (H2O) |
|
4,042 |
|
|
|
|
|
NTR-SOLID (CO2) |
|
3,306 |
|
|
|
|
|
NTR-SOLID (CO or N2) |
|
2,649 |
|
|
|
|
|
NTR-SOLID-NERVA |
0.198-
0.065 |
see above |
49,000 |
10 |
no |
|
|
Laser Thermal |
0.065 |
40,000 |
13,000 |
20 |
no |
920 laser |
30% |
Mass Driver |
0.3 |
30,000 |
20,000 |
150 |
no |
350 |
90% |
LANTR (Nerva mode) |
0.309 |
9,221 |
67,000 |
? |
yes |
|
|
LANTR (LOX mode) |
0.584 |
6,347 |
184,000 |
? |
yes |
|
|
Ion |
0.785 |
157,000 |
10,000 |
400 |
no |
800 |
96% |
NTR-SOLID-PBed (H2) |
1.1 |
9,810 |
230,000 |
4.2 |
yes |
|
|
D-T Fusion |
1.2 |
22,000 |
108,000 |
10 |
yes |
|
|
Metahelium He* |
1.4 |
43,000 |
64,000 |
10 |
no |
|
|
AM-SOLID max |
2.4 |
10,791 |
440,000 |
? |
yes |
|
|
MPD |
3.1 |
314,000 |
20,000 |
1540 |
no |
4000 |
79% |
Chemical MAX |
3.8 |
4,500 |
1,669,000 |
2 |
yes |
|
|
Metahelium He IV-A |
? |
21,600 |
? |
10 |
? |
|
|
AM-Gas max |
? |
24,500 |
? |
? |
? |
|
|
NTR-GAS-Closed (H2) |
4.5 |
20,405 |
445,000 |
56.8 |
no |
|
|
ORION Fission |
5.7 |
43,000 |
263,000 |
200 |
no |
|
|
ACMF |
6.6 |
132,300 |
100,000 |
? |
no |
|
|
ORION Fusion |
10.7 |
73,000 |
292,000 |
200 |
no |
|
|
NTR-SOLID-DUMBO |
14.0-
4.6 |
see above |
3,500,000 |
5 |
yes |
|
|
H-B Fusion |
30 |
980,000 |
61,000 |
300 |
no |
|
|
AM-Plasma/Water |
30 |
980,000 |
61,000 |
500 |
no |
|
|
NTR-SOLID MAX |
42 |
12,000 |
7,000,000 |
15 |
yes |
|
|
NTR-LIQUID max |
56 |
16,000 |
7,000,000 |
70 |
yes |
|
|
NTR-GAS-Open (H2) |
61 |
35,000 |
3,500,000 |
30-200 |
yes |
|
|
Mini-MagOrion |
66 |
210,000 |
625,000 |
? |
yes? |
|
|
NTR-GAS-Open 2nd Gen |
100 |
50,000 |
5,000,000 |
30-200 |
yes |
|
|
NTR-GAS MAX |
150 |
98,000 |
3,000,000 |
15 |
yes |
|
|
NTR-GAS-Coaxial (H2) |
157 |
17,658 |
17,800,000 |
127 |
yes |
|
|
He3-D Fusion |
192 |
7,840,000 |
49,000 |
1200 |
no |
|
|
AM-Plasma/Hydrogen |
192 |
7,840,000 |
49,000 |
500 |
no |
|
|
MC-Fusion MAX |
200 |
8,000,000 |
50,000 |
0.6 |
yes |
|
|
NSWR 20% UTB |
430 |
66,000 |
13,000,000 |
? |
yes |
|
|
1959 ORION 1st Gen |
1,600 |
39,000 |
80,000,000 |
1,700 |
yes |
|
|
1959 ORION 2nd Gen |
24,000 |
120,000 |
400,000,000 |
3,250 |
yes |
|
|
NSWR 90% UTB MAX |
31,000 |
4,700,000 |
13,000,000 |
? |
yes |
|
|
ORION MAX |
39,000 |
9,800,000 |
8,000,000 |
8 |
yes |
|
|
IC-Fusion MAX |
500,000 |
10,000,000 |
100,000,000 |
1000 |
yes |
|
|
AM-Beam MAX |
500,000 |
100,000,000 |
10,000,000 |
10 |
yes |
|
|
ACMF:
ANTIPROTON-CATALYZED
MICROFISSION / INERTIAL CONFINMENT FISSION
AIM:
ANTIPROTON-INITIATED
MICROFUSION / INERTIAL CONFINMENT FUSION
AM-Beam: ANTIMATTER BEAM CORE. Microscopic amounts
of antimatter are reacted with equal amounts of matter. The charged
pions from the reaction are used directly as thrust, instead of being
used to heat a propellant. They are channeled by a magnetic nozzle.
Without a technological break-through, this is a very low thrust
propulsion system. All antimatter rockets produce dangerous amounts of
gamma rays.
AM-Gas: ANTIMATTER GAS CORE. Microscopic amounts of
antimatter are injected into large amounts of water or hydrogen
propellant. The intense reaction flashes the propellant into plasma
which exits through the exhaust nozzle. Magnetic fields constrain the
charged pions from the reaction so they heat the propellant, but
uncharged pions escape and do not contribute any heating. Less efficient
than AM-Solid core, but can achieve a higher specific impulse. For
complicated reasons, a spacecraft optimized to use an antimatter
propulsion system need never to have a mass ratio greater than 4.9, and
may be as low as 2. No matter what the required delta V, the spacecraft
requires a maximum of 3.9 tons of reaction mass per ton of dry mass, and
a variable amount of antimatter measured in micrograms to grams.
AM-Plasma: ANTIMATTER PLASMA CORE. Similar to AM-Gas,
but more antimatter is used, raising the the propellant temperature to
levels that convert it into plasma. A magnetic bottle is required to
contain the plasma.
AM-Solid: ANTIMATTER SOLID CORE. Basically a NERVA
design where the reactor is replaced by a tungsten target. 13 micrograms
per second of antiprotons are annihilated. The gamma rays and pions are
captured in the tungsten target, heating it. The tungsten target in turn
heats the hydrogen. Produces high thrust but the specific impulse is
limited due to material constraints (translation: above a certain
power level the blasted tungsten melts)
ArcJet: Hydrogen propellant is heated by an
electrical arc.
BEER: In The Makeshift Rocket, the old geezer
cobbles together a crude rocket out of hogs-heads of pressurized beer in
order to escape to an adjacent asteroid.
Chemical: Hydrogen-Oxygen. The same thing used on
the Space Shuttle.
D-T Fusion: DEUTERIUM-TRITIUM FUSION. Fuel:
deuterium and tritium. Propellant: lithium.
H-B Fusion: HYDROGEN-BORON FUSION: Fuel is hydrogen
and boron. Propellant is hydrogen. A pity about the low thrust. The
fusion drives in Larry Niven's "Known Space" novels probably have
performance similar to H-B Fusion, but with millions of newtons of
thrust.
He3-D Fusion: HELIUM 3-DEUTERIUM FUSION.
Fuel is helium3 and deuterium. Propellant is hydrogen.
IC Fusion: INERTIAL CONFINEMENT FUSION. A pellet of
fusion fuel is bombarded on all sides by strong pulses from laser or
particle accelerators. The inertia of the fuel holds it together long
enough for most of it to undergo fusion.
Ion: Potassium seeded argon is ionized and the ions
are accelerated electrostatically by electrodes. Other propellants can
be used, such as cesium and buckyballs. Though it has admirably high
exhaust velocity, there are theoretical limits that ensure all Ion
drives are low thrust. It also shares the same problem as the other
electrically powered low-thrust drives. In the words of a NASA engineer
the problem is "we can't make an extension cord long enough." That is,
electrical power plants are weighty enough to make the low thrust an
even larger liability.
If you are interested in the technical details about why ion drives
are low thrust, read the next two paragraphs by
Dr. John Schilling.
And it suffers from the same critical thrust-limiting problem as any
other ion engine: since you are accelerating ions, the acceleration
region is chock full of ions. Which means that it has a net space charge
which repels any additional ions trying to get in until the ones already
under acceleration manage to get out, thus choking the propellant flow
through the thruster.
The upper limit on thrust is proportional to the cross-sectional area
of the acceleration region and the square root of the voltage gradient
across the acceleration region, and even the most optimistic plausible
values (i.e. voltage gradients just shy of causing vacuum arcs across
the grids) do not allow for anything remotely resembling high thrust.
Erik Max Francis adds:
You can only increase particle energy so much; you then start to get
vacuum arcing across the acceleration chamber due to the enormous
potential difference involved. So you can't keep pumping up the voltage
indefinitely.
To get higher thrust, you need to throw more particles into the mix.
The more you do this, the more it will reduce the energy delivered to
each particle.
It is a physical limit. Ion drives cannot have high
thrusts.
J x B Electric: "Jay cross Bee". A crossed field
plasma accelerator.
LANTR: LOX-AUGMENTED NUCLEAR THERMAL ROCKET. This
concept involves the use of a "conventional" hydrogen (H2)
NTR with oxygen (O2) injected into the nozzle. The injected O2
acts like an "afterburner" and operates in a "reverse scramjet" mode.
This makes it possible to augment (and vary) the thrust (from
what would otherwise be a relatively small NTR engine) at the
expense of reduced Isp
MC Fusion: MAGNETIC CONFINEMENT FUSION. A magnetic
bottle contains the fusion reaction. Very difficult to do. Researchers
in this field say that containing fusion plasma in a magnetic bottle is
like trying to support a large slab of gelatin with a web of rubber
bands. Making a magnetic bottle which has a magnetic rocket exhaust
nozzle is roughly 100 times more difficult.
Meta-helium He*:
SPIN-POLARIZED
TRIPLET HELIUM. Three helium atoms are aligned in a metastable state.
When it reverts to normal state it releases 0.48 gigjoules per kilogram.
The trouble is that it tends to decay spontaneously, with a lifetime of
a mere 2.3 hours.
Meta-helium He IV-A:
DIATOMIC
METASTABLE HELIUM. One normal and one excited helium atom are paired
to form a stable solid.
The trick is to keep the touchy stuff from exploding prematurely and
destroying the spacecraft. The fuel is stored in a resonant waveguide.
This is another propulsion system that renders the spacecraft unusually
vulnerable to weapons strikes.
Mini-MagOrion: This is a sort of micro-fission Orion
propulsion system. The fuel and propellant are subcritical pellets of
Curium-245. These are compressed electrodynamically by a Z-pinch
magnetic field until they reach criticality and explode. The momentum
from the explosion is transferred to the spacecraft by the magnetic
field. The field coils are attached to a shock absorber Orion style. The
detonations occur at a rate of 1 Hz.
MPD: MAGNETOPLASMADYNAMIC. A travelling wave plasma
accelerator. Propellant is potassium seeded helium.
NSWR:
NUCLEAR SALT-WATER
ROCKET. This concept by Dr. Zubrin is considered far-fetched by many
scientists. The fuel is a 20% solution of Uranium tetrabromide in water.
The fuel tanks are thin capillary tubes embedded in a neutron damper
(like cadmium) to prevent a chain reaction. The fuel is injected
into the reaction chamber to create a critical mass. It is basically a
continuously detonating Orion type drive with water as propellant. The
controversy is over how to contain such a reaction. Zubrin maintains
that skillful injection of the fuel can force the reaction to occur
outside the reaction chamber. Naturally in such a spacecraft, damage to
the fuel tanks can have unfortunate results (say, damage caused by
hostile weapons fire). The advantage of NSWR is that this is the
only known propulsion system that combines high exhaust velocity with
high thrust. The disadvantage is that it combines many of the worst
problems of the Orion and Gas Core systems. For starters, using it for
take-offs will leave a large crater that will glow blue for several
hundred million years, as will everything downwind in the fallout area.
NTR-GAS-Closed: CLOSED-CYCLE GASEOUS CORE FISSION /
NUCLEAR THERMAL ROCKET aka "Nuclear Lightbulb". Similar to a gas core
fission rocket, but the uranium plasma is confined in a fused quartz
chamber. The good news is that there is no uranium escaping in the
exhaust. The bad news is that the exhaust velocity is halved.
NTR-GAS-Coaxial: GASEOUS CORE COAXIAL FLOW FISSION /
NUCLEAR THERMAL ROCKET
NTR-GAS-Open: GASEOUS CORE FISSION / NUCLEAR THERMAL
ROCKET aka consumable nuclear rocket, plasma core, fizzler, cavity
reactor rocket. The limit on NTR-SOLID exhaust velocities is the melting
point of the reactor. Some engineer who obviously likes thinking "outside
of the box" tried to make a liability into a virtue. They asked the
question "what if the reactor was already molten?"
Gaseous uranium is injected into the reaction chamber until there is
enough to start a furious chain reaction. Hydrogen is then injected into
the center of this nuclear inferno where is flash heats and shoots out
the exhaust nozzle.
The trouble is the uranium shoots out the exhaust as well.
The reaction is maintained in a vortex tailored to minimize loss of
uranium out the nozzle. Fuel is uranium hexaflouride (U235F6)
, propellant is hydrogen. The loss of uranium in the exhaust reduces
efficiency and angers environmentalists.
If used for lift off it can result in a dramatic decrease in the
property values around the spaceport. Amusingly enough, this is the best
match for the propulsion system used in the TOM CORBETT: SPACE CADET
books. However the books are sufficiently vague that it is possible the
Polaris used a nuclear lightbulb. According to technical advisor Willy
Ley, "reactant" is the hydrogen propellant, but the books imply that
reactant is the liquid uranium.
NTR-LIQUID: NUCLEAR THERMAL ROCKET / LIQUID CORE
FISSION. Similar to an NTR-GAS, but the fissionable core is merely
molten, not gaseous.
NTR-SOLID: NUCLEAR THERMAL ROCKET / SOLID CORE
FISSION. It's a real simple concept. Put a nuclear reactor on top of an
exhaust nozzle. Instead of running water through the reactor and into a
generator, run hydrogen through it and into the nozzle. By diverting the
hydrogen to a turbine generator 60 megawatts can be generated. The
reactor elements have to be durable, since erosion will contaminate the
exhaust with fissionable materials. The exhaust velocity limit is fixed
by the melting point of the reactor. Hydrogen gives the best exhaust
velocity, but the other propellants are given in the table since a
spacecraft may be forced to re-fuel on whatever working fluids are
available locally (Wilderness re-fuelling or "the enlisted men get
to go out and shovel whatever they can find into the propellant tanks").
Another reason to avoid hydrogen is the difficulty of storing the
blasted stuff, and its annoyingly low density (Ammonia is about
eight times as dense!). Exhaust velocities are
listed for a realistically attainable core temperature of 3200 degrees K
for the propellants Hydrogen (H2), Methane (CH4),
Ammonia (NH3), Water (H2O),
Carbon Dioxide (CO2), Carbon Monoxide (CO),
and Nitrogen (N2)
Dr. John Schilling figures that as an order of magnitude guess, about
one day of full power operation would result in enough fuel burnup to
require reprocessing of the fissionable fuel elements. (meaning that
while there is still plenty of fissionables in the fuel rod, enough by-products
have accumulated that the clogged rod produces less and less energy)
A reprocessing plant could recover 90-95% of the fuel. With reprocessing,
in the long term each totally consumed kilogram of plutonium or highly
enriched uranium (HEU) will yield ~1E10 newton-seconds of
impulse at a specific impulse of ~1000 seconds.
Dr. Schilling also warns that there is a minimum amount of
fissionable material for a viable reactor. Figure a minimum of 50
kilograms of HEU.
NTR-SOLID-DUMBO: This was a competing design to
NERVA. It was shelved political decision that, (in order to cut
costs on the atomic rocket projects) required both
projects to use an already designed NEVRA engine nozzle. Unfortunately,
said nozzle was not compatible with the DUMBO active cooling needs..
Dumbo does, however, have a far superior mass flow to the NERVA, and
thus a far superior thrust. Dumbo actually had a thrust to weight ratio
greater than one. NASA still shelved DUMBO because [a] NERVA used off
the shelf components and [b] they knew there was no way in heck that
they could get permission for nuclear lift-off rocket so who cares if
T/W < 0?
NTR-SOLID-NERVA: NUCLEAR ENGINE for ROCKET VEHICLE
APPLICATIONS. The first type of NTR-SOLID propulsion systems. It used
reactor fuel rods surrounded by a neutron reflector. Unfortunately its
thrust to weight ratio is less than one, so no lift-offs with this
rocket. The trouble was inadequate propellant mass flow, the result of
trying to squeeze too much hydrogen through too few channels in the
reactor.
NTR-SOLID-PBed: PARTICLE BED / NUCLEAR THERMAL
ROCKET aka fluidized-bed, dust-bed, or rotating-bed reactor. In the
particle-bed reactor, the nuclear fuel is in the form of a particulate
bed through which the working fluid is pumped. This permits operation at
a higher temperature than the solid-core reactor by reducing the fuel
strength requirements . The core of the reactor is rotated (approximately
3000 rpm) about its longitudinal axis such that the fuel bed is
centrifuged against the inner surface of a cylindrical wall through
which hydrogen gas is injected. This rotating bed reactor has the
advantage that the radioactive particle core can be dumped at the end of
an operational cycle and recharged prior to a subsequent burn, thus
eliminating the need for decay heat removal, minimizing shielding
requirements, and simplifying maintenance and refurbishment operations.
ORION:
CONSUMABLE NUCLEAR THERMAL ROCKET aka "old Boom-boom". The ultimate
consumable nuclear rocket, based on the "firecracker under a tin can"
principle. This concept has the spacecraft mounted with shock absorbers
on an armored "pusher plate". A stream of small (5 to 15 kiloton)
fission or fusion explosives are detonated under the plate to provide
thrust. While you might find it difficult to believe that the spacecraft
can survive this, you will admit that this will give lots of thrust to
the spacecraft (or its fragments). On the plus side, a pusher
plate that can protect the spacecraft from the near detonation of
nuclear explosives will also provide dandy protection from any incoming
weapons fire. On the minus side I can hear the environmentalists howling
already. It will quite thoroughly devastate the lift-off site, and give
all the crew bad backs and fallen arches. And they had better have extra-strength
brassieres and athletic supporters. However, there is a
recent
report that suggests ways of minimizing the fallout from an ORION
doing a ground lift-off (or a, wait for it, "blast-off" {rimshot}).
Apparently if the launch pad is a large piece of armor plate with a
coating of graphite there is very little fallout.
Each pulse unit has a radiation case that channels the initial blast
upwards towards the pusher plate. Along the way it vaporizes a solid
chunk of propellant and accelerates it to the plate. The device is
basically a nuclear shaped charge. Each charge accelerates the
spacecraft by roughly 12 m/s. A 4,000 ton spacecraft would use 5 kiloton
charges, and a 10,000 ton spacecraft would use 15 kiloton charges. For
blast-off, smaller charges of 0.15 kt and 0.35 kt respectively would be
used while within the Earth's atmosphere. The air between the charge and
the pusher plate amplifies the impulse delivered. The propellant is
tungsten, the channel filler is beryllium oxide, and the radiation case
is uranium. A 5 kiloton charge is about 850 kg.
So the x-rays and other radiation from the nuclear explosion are
channeled by the x-ray opaque uranium up into the beryllium oxide
channel filler. This absorbs the radiation, converting it into heat. The
heat blasts upward, flashing the tungsten propellant into a jet of
tungsten plasma. The jet hits the pusher plate, accelerating the
spacecraft. The jet is confined to a cone about 22.5 degrees.
The following table is from a 1959 report on Orion, and is probably a
bit optimistic. But it makes for interesting reading.
Model |
Interplanetary
Ship |
Advanced
Interplanetary
Ship |
Gross Mass |
4,000 tons |
10,000 tons |
Propulsion System Mass |
1,700 tons |
3,250 tons |
Exhaust Velocity |
39,000 m/s |
120,000 m/s |
Diameter |
41 m |
56 m |
Height |
61 m |
85 m |
Average acceleration |
up to 2g |
up to 4g |
Thrust |
8e7 N |
4e8 N |
Propellant Mass Flow |
2000 kg/s |
3000 kg/s |
Atm. charge size |
0.15 kt |
0.35 kt |
Space charge size |
5 kt |
15 kt |
Num charges for 38,000 m |
200 |
200 |
Total yield for 38,000 m |
100 kt |
250 kt |
Num charges for 480 km orbit |
800 |
800 |
Total yield for 480 km orbit |
3 mt |
9 mt |
Dv
10 km/s Mass Ratio (Payload) |
1.2 (1,600 tons) |
1.1 (6,100 tons) |
Dv
15.5 km/s Mass Ratio (Payload) |
1.4 (1,200 tons) |
1.1 (5,700 tons) |
Dv
21 km/s Mass Ratio (Payload) |
1.6 (800 tons) |
1.2 (5,300 tons) |
Dv
30 km/s Mass Ratio (Payload) |
2.1 (200 tons) |
1.3 (4,500 tons) |
Dv
100 km/s Mass Ratio (Payload) |
cannot |
2.2 (1,300 tons) |
Dv 10 km/s = Earth surface
to 480 km Earth orbit
Dv 15.5 km/s = Earth surface
to soft Lunar landing
Dv 21 km/s = Earth surface to
soft Lunar landing to 480 km Earth orbit
or Earth surface to Mars orbit to 480 km Earth orbit
Dv 30 km/s = Earth surface to
Venus orbit to Mars orbit to 480 km Earth orbit
Dv 100 km/s = Earth surface to
inner moon of Saturn to 480 km Earth orbit
NASA has been quietly re-examining ORION, under the new name of "External
Pulsed Plasma Propulsion". As George Dyson observed, the new name
removes most references to "Nuclear", and all references to "Bombs."
Painting on the right by Professor Sol Dember
Solar Moth: SOLAR THERMAL ROCKET 175 meter diameter
aluminum coated reflector concentrates solar radiation onto a window
chamber hoop boiler, heating and expanding the propellant through a
regeneratively-cooled hoop nozzle. The concentrating mirror is one half
of a giant inflatable balloon, the other half is transparent. Propellant
is hydrogen seeded with alkali metal. The advantage is that you have
power as long as the sun shines. The disadvantage is it doesn't work
well past the orbit of Mars and the exhaust velocity is pathetic. This
might be carried on a spacecraft as an emergency propulsion system,
since the engine mass is so miniscule.
VASIMR: VARIABLE SPECIFIC IMPULSE MAGNETOPLASMA
ROCKET. This is a plasma drive with the amusing ability to "shift gears."
This means it can trade exhaust velocity for thrust and vice versa.
Three "gears" are shown on the table. |