docabn
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Could anyone explain how tritium could be used as a propellent more efficiently than the LH2 / LO2 used now? Or have I misinterpreted the science?
Thanks
Thanks
Could anyone explain how tritium could be used as a propellent more efficiently than the LH2 / LO2 used now? Or have I misinterpreted the science?
Thanks
As far as I know, HE3 would be a good FUEL (read: the substance providing the energy) for a fusion drive, while for PROPELLANT (read: the stuff being thrown out of the nozzle) normal H2 would be used.
The only reason why one should introduce more mass is to cool the reactor. That energy could go towards propulsion, but I see no reason why you should introduce more propellant just to increase thrust at the cost of Isp. You might as well build a bigger reactor to increase your thrust at no expense of Isp.
The only reason why one should introduce more mass is to cool the reactor. That energy could go towards propulsion, but I see no reason why you should introduce more propellant just to increase thrust at the cost of Isp. You might as well build a bigger reactor to increase your thrust at no expense of Isp.
I am well aware of the added mass the bigger reactor would bring and even if the the mass penalty for the reactor would be twice as great as the original reactor and the thrust would be doubled, the reactor does not comprise the entire mass of the ship. The power to mass ratio of the ship in general would increase, resulting in a higher acceleration.
Think of it in terms of Dawn, a probe heading to Cares and Vesta. It has 3 ion engines - the same design as used on Deep Space 1 - and has a total of 425 kg of Xenon propellant. The total mass of the spacecraft at launch was around 1250 kg. Now... only one of the ion thrusters can be fired at the same time, because of insufficient power... but despite that fact, there are 3 on board. That means that even though 1 extra thruster could have been used as a backup, 3 were put on board regardless of the mass penalty. It's safe to assume that the future vessels will not consist of an engine and fuel and that most of the weight will be provided by the payload.
Dawn is able to achieve around 10 km/s Delta-V with just over 400 kg of propellant. That's about as much as a rocket needs to get into LEO, with tons and tons of propellant.
@ Mindblast:
For one, I can imagine that a vessel with a fusion drive will not be used on an Earth-Moon trip, but rather a trip around the solar system, or as part of a Buzzard ramjet.
If the mass of the ship is m and the mass of one reactor is m/10, the thrust provided by the reactor is F, then the original thrust to mass ratio is F/m, but the new one is 2 * F / (11/10) * m = 20/11 * F/m, therefore, the thrust to mass ratio of the ship overall has almost doubled.
If the mass of the ship is m and the mass of one reactor is m/10, the thrust provided by the reactor is F, then the original thrust to mass ratio is F/m, but the new one is 2 * F / (11/10) * m = 20/11 * F/m, therefore, the thrust to mass ratio of the ship overall has almost doubled.
The ion engine powering Deep Space 1 took 4 days to increase velocity by some 30 m/s and yet we're pretty keen on developing such technology.
On a trip around the solar system, 1 km/s per week would be quite favorable.
@ Mindblast:
For one, I can imagine that a vessel with a fusion drive will not be used on an Earth-Moon trip, but rather a trip around the solar system, or as part of a Buzzard ramjet.
Therefore it is safe to assume that a ridiculously high Isp is desirable, as the engine will undoubtedly operate in the range of weeks, months or more.
No need to get offensive..Which brings me to your equations...
While you certainly have the ability to read equations off Wikipedia, you don't seem to have any understanding of them.
No in fact it exactly corresponds to my assumptions:Now... as you can see from this equation, doubling the mass flow rate will NOT increase your acceleration by two times. It will increase it by square root of 2 =~ 1.41. You'll need to increase it by 4 times to double your acceleration, which quite clearly goes against your assumptions.
Mindblast said:So if you halve the velocity you can throw in 4 times the mass for the same kinetic energy but you get 2 times the thrust.
Thats all fine if you can build light weight fusion reactors with powerlevels in the TeraWatt range to get enough thrust while only using the fusion products as drive mass. I guess this will not be within our reach for quite a while though.a = Sqrt(2 * M * M * q) / m
a = Sqrt(2 * q) * M / m
And as you can see, acceleration increases linearly with the mass flow through the reactor, however, this equation will only apply if the mass flow is actually being burned. If you introduce mass after burning has been finished, the first equation will apply.
Who do you think would spend 10 billion dollars building a reactor in space to go to the Moon? Do we build ion engines to send probes to the Moon? No, we build them to send them off on years long voyages.
Also, I don't think anyone would spend that much money to get 10 km/s Delta-V and burn for 3 days. Besides, even with this "high thrust", to get to the Moon, you'd still have to slowly spiral out into a higher orbit... kinda like how they get unmanned probes to the Moon. So it's clear that for ejects, you'd still need propulsion that's in the range of 10 times more powerful.
So... assuming 1000 tons of propellant on a ship that has such a low acceleration would mean a delta-V of roughly 18 400 km/s. That's a horribly high number. I'm pretty sure getting to Saturn with this high Isp would be quicker then by getting there at "high thrust". Even optimizing the thrust to increase velocity all the way there and then turn around and start thrusting to kill that velocity... this kind of travel, which is the fastest, would still need an insanely high Isp - far higher then what you proposed.