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Rocket engine performance?
Does the amount of heat in the exhaust have any bearing on the isp and
amount of thrust the engine produces? i.e. the heat produced by the SSME is only a few thousand degrees, and the SSME is a low isp but high thrust engine, and the VASMIR is expected to have a plasma exhaust temp of a million or so degrees, but it is a high isp with a low thrust engine as the plasma emmited is a tenious plasma, and is only a fraction as dense as te exhaust emmited by the SSME. I guess the ideal rocket engine for sublight travel around this/a system with our existing tech knowledge is a high thrust VASIMR type plasma engine. Christopher +++++++++++++++++++++++++ "There's a light at the end of the tunnel" says the optimist. "It's probably a train coming stright at us" responds the pessimist. |
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Rocket engine performance?
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Rocket engine performance?
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Rocket engine performance?
"Christopher" wrote:
Does the amount of heat in the exhaust have any bearing on the isp and amount of thrust the engine produces? i.e. the heat produced by the SSME is only a few thousand degrees, and the SSME is a low isp but high thrust engine, and the VASMIR is expected to have a plasma exhaust temp of a million or so degrees, but it is a high isp with a low thrust engine as the plasma emmited is a tenious plasma, and is only a fraction as dense as te exhaust emmited by the SSME. Very much so. Temperature is a measurement of the average kinetic energy of the molecules in a gas (or a liquid or a solid, but we're concerned with gasses right now). In fact, they are related by the equation KE = 3/2 k T, where KE is the average kinetic energy of a molecule in the gas, k is Boltzmann's constant (1.38e-23 J/K), and T is the temperature of the gas in Kelvin. Further, using the equation KE = 1/2 m v^2, you can determine the average velocity of a gas at a specific temperature. For example, take CO2 at 1,000 K, the mass of the molecule is 14 amu (2.32e-26 kg), the average kinetic energy per molecule is 2.07e-20 J, and so the average speed of the molecules is around 1.3 km/s. Neat, huh? As you can see, doubling the temperature raises the molecular speed by sqrt(2), and halving the molecular mass has the same effect. I guess the ideal rocket engine for sublight travel around this/a system with our existing tech knowledge is a high thrust VASIMR type plasma engine. Not necessarily. VASIMR is a tricky beast, because it, like all electric rockets, has separate propellant and power systems. This is disadvantages compared to many other high-thrust, high-ISP designs which have combined power and propellant (i.e. the propellant generates its own power to heat itself, as in chemical rockets) such as NSWR, Orion, fusion rockets, etc. This separation means that the rocket equation needs a little mending to accurately describe the functioning of the propulsion system. If it takes a certain amount of, for example, fission fuel to create the energy needed to expell a certain amount of propellant from the VASIMR rocket then you can't just figure the mass of the propellant alone into the equation. Fortunately, nuclear reactions are very energetic so they hardly don't need accounting for mass usage, but not entirely, and there are other concerns as well, such as the mass overhead of the entire reactor system needed to power the rocket. Personally, I don't see VASIMR as being capable of providing the performance necessary for interstellar travel in reasonable (sub millenial) travel times and I think especially fusion, NSWR, and Orion are the best bets there. |
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