PHYSICALLY POWERED
Type
|
Description
|
Advantages
|
Disadvantages
|
Partially filled pressurised carbonated drinks container with tail and nose weighting
|
Very simple to build
|
Altitude typically limited to a few hundred feet or so (world record is 623 meters/2044 feet)
| |
A non combusting form, used for vernier thrusters
|
Non contaminating exhaust
|
Extremely low performance
| |
Hot water is stored in a tank at high temperature/pressure and turns to steam in nozzle
|
Simple, fairly safe, under 200 seconds Isp
|
Low overall performance due to heavy tank
|
CHEMICALLY POWERED
Type
|
Description
|
Advantages
|
Disadvantages
|
Ignitable, self sustaining solid fuel/oxidiser mixture ("grain") with central hole and nozzle
|
Simple, often no moving parts, reasonably good mass fraction, reasonable Isp. A thrust schedule can be designed into the grain.
|
Once
lit, extinguishing it is difficult although often possible, cannot be
throttled in real time; handling issues from ignitable mixture, lower
performance than liquid rockets, if grain cracks it can block nozzle
with disastrous results, cracks burn and widen during burn. Refuelling
grain harder than simply filling tanks, Lower specific Impulse than
Liquid Rockets.
| |
Separate oxidiser/fuel, typically oxidiser is liquid and kept in a tank, the other solid with central hole
|
Quite
simple, solid fuel is essentially inert without oxidiser, safer;
cracks do not escalate, throttleable and easy to switch off.
|
Some
oxidisers are monopropellants, can explode in own right; mechanical
failure of solid propellant can block nozzle (very rare with
rubberised propellant), central hole widens over burn and negatively
affects mixture ratio.
| |
Propellant
such as Hydrazine, Hydrogen Peroxide or Nitrous Oxide, flows over
catalyst and exothermically decomposes and hot gases are emitted
through nozzle
|
Simple in concept, throttleable, low temperatures in combustion chamber
|
catalysts can be easily contaminated, monopropellants can detonate if contaminated or provoked, Isp is perhaps 1/3 of best liquids
| |
Two fluid (typically liquid) propellants are introduced through injectors into combustion chamber and burnt
|
Up
to ~99% efficient combustion with excellent mixture control,
throttleable, can be used with turbopumps which permits incredibly
lightweight tanks, can be safe with extreme care
|
Pumps
needed for high performance are expensive to design, huge thermal
fluxes across combustion chamber wall can impact reuse, failure modes
include major explosions, a lot of plumbing is needed.
| |
Rocket takes off as a bipropellant rocket, then turns to using just one propellant as a monopropellant
|
Simplicity and ease of control
|
Lower performance than bipropellants
| |
Three
different propellants (usually hydrogen, hydrocarbon and liquid
oxygen) are introduced into a combustion chamber in variable mixture
ratios, or multiple engines are used with fixed propellant mixture
ratios and throttled or shut down
|
Reduces take-off weight, since hydrogen is lighter; combines good thrust to weight with high average Isp, improves payload for launching from Earth by a sizeable percentage
|
Similar issues to bipropellant, but with more plumbing, more R&D
| |
Essentially a ramjet where intake air is compressed and burnt with the exhaust from a rocket
|
Mach 0 to Mach 4.5+ (can also run exoatmospheric), good efficiency at Mach 2 to 4
|
Similar
efficiency to rockets at low speed or exoatmospheric, inlet
difficulties, a relatively undeveloped and unexplored type, cooling
difficulties, very noisy, thrust/weight ratio is similar to ramjets.
| |
Very close to existing designs, operates in very high altitude, wide range of altitude and airspeed
|
Atmospheric airspeed limited to same range as turbojet engine, carrying oxidizer like LOX can be dangerous. Much heavier than simple rockets.
| ||
Precooled jet engine / LACE (combined cycle with rocket)
|
Intake
air is chilled to very low temperatures at inlet before passing
through a ramjet or turbojet engine. Can be combined with a rocket
engine for orbital insertion.
|
Easily
tested on ground. High thrust/weight ratios are possible (~14)
together with good fuel efficiency over a wide range of airspeeds,
mach 0-5.5+; this combination of efficiencies may permit launching to
orbit, single stage, or very rapid intercontinental travel.
|
ELECTRICALLY POWERED
Type
|
Description
|
Advantages
|
Disadvantages
|
Resistojet rocket (electric heating)
|
A monopropellant is electrically heated by a filament for extra performance
|
Higher Isp than monopropellant alone, about 40% higher.
|
Uses a lot of power and hence gives typically low thrust
|
Arcjet rocket (chemical burning aided by electrical discharge)
|
Similar to resistojet in concept but with inert propellant, except an arc is used which allows higher temperatures
|
1600 seconds Isp
|
Very low thrust and high power, performance is similar to Ion drive.
|
Pulsed plasma thruster (electric arc heating; emits plasma)
|
Plasma is used to erode a solid propellant
|
High Isp , can be pulsed on and off for attitude control
|
Low energetic efficiency
|
Microwave heated plasma with magnetic throat/nozzle
|
Variable Isp from 1000 seconds to 10,000 seconds
|
similar
thrust/weight ratio with ion drives (worse), thermal issues, as with
ion drives very high power requirements for significant thrust, really
needs advanced nuclear reactors, never flown, requires low
temperatures for superconductors to work
|
SOLAR POWERED
The Solar thermal rocket would make use of solar power to directly heat reaction mass,
and therefore does not require an electrical generator as most other
forms of solar-powered propulsion do. A solar thermal rocket only has to
carry the means of capturing solar energy, such as concentrators and mirrors.
The heated propellant is fed through a conventional rocket nozzle to
produce thrust. The engine thrust is directly related to the surface
area of the solar collector and to the local intensity of the solar
radiation and inversely proportional to the Isp.
Type
|
Description
|
Advantages
|
Disadvantages
|
Propellant is heated by solar collector
|
Simple design. Using hydrogen propellant, 900 seconds of Isp
is comparable to Nuclear Thermal rocket, without the problems and
complexity of controlling a fission reaction. Using
higher–molecular-weight propellants, for example water, lowers
performance.
|
Only useful once in space, as thrust is fairly low, but hydrogen is not easily stored in space, otherwise moderate/low Isp if higher–molecular-mass propellants are used
|
BEAM POWERED
Type
|
Description
|
Advantages
|
Disadvantages
|
Propellant
is heated by light beam (often laser) aimed at vehicle from a
distance, either directly or indirectly via heat exchanger
|
simple in principle, in principle very high exhaust speeds can be achieved
|
~1
MW of power per kg of payload is needed to achieve orbit, relatively
high accelerations, lasers are blocked by clouds, fog, reflected laser
light may be dangerous, pretty much needs hydrogen monopropellant for
good performance which needs heavy tankage, some designs are limited
to ~600 seconds due to reemission of light since propellant/heat
exchanger gets white hot
| |
Propellant is heated by microwave beam aimed at vehicle from a distance
|
microwaves avoid reemission of energy, so ~900 seconds exhaust speeds might be achieveable
|
~1
MW of power per kg of payload is needed to achieve orbit, relatively
high accelerations, microwaves are absorbed to a degree by rain,
reflected microwaves may be dangerous, pretty much needs hydrogen
monopropellant for good performance which needs heavy tankage,
transmitter diameter is measured in kilometres to achieve a fine
enough beam to hit a vehicle at up to 100 km.
|
NUCLEAR POWERED
Nuclear propulsion includes a wide variety of propulsion methods that use some form of nuclear reaction
as their primary power source. Various types of nuclear propulsion have
been proposed, and some of them tested, for spacecraft applications:
Type
|
Description
|
Advantages
|
Disadvantages
|
Radioisotope rocket/"Poodle thruster" (radioactive decay energy)
|
Heat from radioactive decay is used to heat hydrogen
|
about 700–800 seconds, almost no moving parts
|
low thrust/weight ratio.
|
Nuclear thermal rocket (nuclear fission energy)
|
propellant (typ. hydrogen) is passed through a nuclear reactor to heat to high temperature
|
Isp can be high, perhaps 900 seconds or more, above unity thrust/weight ratio with some designs
|
Maximum
temperature is limited by materials technology, some radioactive
particles can be present in exhaust in some designs, nuclear reactor
shielding is heavy, unlikely to be permitted from surface of the
Earth, thrust/weight ratio is not high.
|
Gas core reactor rocket (nuclear fission energy)
|
Nuclear reaction using a gaseous state fission reactor in intimate contact with propellant
|
Very hot propellant, not limited by keeping reactor solid, Isp between 1500 and 3000 seconds but with very high thrust
|
Difficulties
in heating propellant without losing fissionables in exhaust, massive
thermal issues particularly for nozzle/throat region, exhaust almost
inherently highly radioactive. Nuclear lightbulb variants can contain
fissionables, but cut Isp in half.
|
Fission-fragment rocket (nuclear fission energy)
|
Fission products are directly exhausted to give thrust
|
Theoretical only at this point.
| |
Fission sail (nuclear fission energy)
|
A sail material is coated with fissionable material on one side
|
No moving parts, works in deep space
|
Theoretical only at this point.
|
Nuclear salt-water rocket (nuclear fission energy)
|
Nuclear salts are held in solution, caused to react at nozzle
|
Very high Isp, very high thrust
|
Thermal issues in nozzle, propellant could be unstable, highly radioactive exhaust. Theoretical only at this point.
|
Nuclear pulse propulsion (exploding fission/fusion bombs)
|
Shaped nuclear bombs are detonated behind vehicle and blast is caught by a 'pusher plate'
|
Very high Isp, very high thrust/weight ratio, no show stoppers are known for this technology
|
Never been tested, pusher plate may throw off fragments
due to shock, minimum size for nuclear bombs is still pretty big,
expensive at small scales, nuclear treaty issues, fallout when used
below Earth's magnetosphere.
|
Antimatter catalyzed nuclear pulse propulsion (fission and/or fusion energy)
|
Nuclear pulse propulsion with antimatter assist for smaller bombs
|
Smaller sized vehicle might be possible
|
Containment
of antimatter, production of antimatter in macroscopic quantities
isn't currently feasible. Theoretical only at this point.
|
Fusion rocket (nuclear fusion energy)
|
Fusion is used to heat propellant
|
Very high exhaust velocity
|
Largely beyond current state of the art.
|
Antimatter rocket (annihilation energy)
|
Antimatter annihilation heats propellant
|
Extremely energetic, very high theoretical exhaust velocity
|
Problems with antimatter production and handling; energy losses in neutrinos, gamma rays, muons; thermal issues. Theoretical only at this point
|
No comments:
Post a Comment
Note: Only a member of this blog may post a comment.