| Space Travel 101: Fundamentals of Space Travel | ||||||||||||||
| Overview Propulsion systems powered by chemical reactions are quite inefficient in terms of their specific impulse. Scientists are developing new, more efficient systems which would be useful in long-term missions. |
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Analysis
IMPROVING EFFICIENCY For a basic action-reaction propulsion system, the initial mass (before using the system) M0, the final mass (after using the system) M, the final velocity v, and the velocity of the system's propellant vp can be related to each other using the equation:
ION THRUSTER Specific Impulse: 1500-8000 sec Thrust: 10-3-10 N
If you have a bunch of ions with the same charge, they can be controlled using an electric field. The ion thruster is based on this idea. A gas, such as xenon, which has a high atomic mass and is easily ionized, is injected into one end of a chamber where it is bombarded by electrons. The bombardment knocks off electrons from the xenon, ionizing it. The other end of the chamber is covered by a charged grid which attracts the ionized gas, accelerating it to speeds much higher than in chemical rockets. After the gas exits the engine, it's combined with a cloud of electrons, which neutralizes the gas to prevent a build up of charge. Ion thrusters, like the one developed for NASA's Deep Space 1 probe, can accelerate gases up to ten times the speed of gases from chemical rockets. The resulting high specific impulses make these systems ideal for long term, distant missions. However, ion thrusters have some drawbacks. The thrust produced is very low (about equivalent to the force of a piece of paper on your hand), which means the acceleration is very low. Luckily, since there's no friction in space, this small acceleration, when continued for a long period of time, can result in great velocities.
VARIABLE SPECIFIC IMPULSE MAGNETOPLASMA ROCKET (VASIMR) Specific Impulse: 1000-30000 sec Thrust: 40-1200 N
The VASIMR is broken up into three parts: two chambers and a magnetic nozzle. In the first chamber, hydrogen gas is injected and heated to the plasma state using radio waves. The plasma is then sent to the second chamber where it becomes super heated by radio waves and magnets to a few million Kelvins (temperature in Kelvins = temperature in Celcius + 273). The super-heated plasma is then directed out of the engine by the magnetic nozzle. The magnetic nozzle has the ability to adjust how much exhaust is let out. Letting out large amounts of exhaust creates greater thrust. However, since the plasma spends less time in the second chamber, it is not heated as much, and so its velocity and specific impulse are lower. On the other hand, if less exhaust is let out, less thrust is produced, but the plasma is heated more, resulting in higher specific impulse.
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