How about Ozone for nuclear rocket reaction mass? Would that be better or worse than Oxygen?
In a chemical engine ozone performs a little better than oxygen, but the difference isn’t enough to make it worth the hassle.
In a nuclear thermal rocket (NTR) I see no advantage to ozone. Granted, I haven’t performed any calculations, but I have to believe that at high temperature it’s just going to breakdown into diatomic oxygen, making its perform the same or similar to oxygen.
To improve the performance of a NTR we want a fuel that is going to decompose into products with a low molecular weight. This means we want a fuel with a lot of hydrogen and not many heavy atoms.
Clearly hydrogen is the best fuel, but its extremely low density is troublesome. The problem isn’t as bad in a chemical engine because there is about 5 to 6 kilograms of LOX for every kilogram of LH2, which lowers the average density to something more manageable. But in a NTR the fuel is 100% LH2, so the low density is a bigger problem.
Although any other propellant we choose is going to perform worse than LH2 in terms of specific impulse, one with a higher density might come close to matching LH2 in terms of Δv because of the higher mass ratio attainable with the denser fuel.
One way to compare potential fuels is to simply calculate the average molecular weight of the exhaust products. The lower the better. At temperatures below 3000 K there is very little dissociation, so for a quick comparison we can assume gases will be in their diatomic form.
Fuel Exhaust Products Mass Moles Mass/Mole
Hydrogen, H2 1 H2 2.02 1 2.02
Methane, CH4 1 C(s) + 2 H2 16.04 3 5.35
Propane, C3H8 3 C(s) + 4 H2 44.10 7 6.30
Pentaborane, B5H9 5 B(s) + 4½ H2 63.12 9.5 6.64
Ethanol, C2H6O 2 C(s) + 3 H2 + ½ O2 46.07 5.5 8.38
Ammonia, NH3 1½ H2 + ½ N2 17.03 2 8.52
MMH, CH6N2 1 C(s) + 3 H2 + 1 N2 46.07 5 9.21
UDMH, C2H8N2 2 C(s) + 4 H2 + 1 N2 66.10 7 9.44
Water, H2O 1 H2O 18.02 1 18.02
This gives us only a rough comparison because there’s more that goes into calculating exhaust velocity than just molecular weight. The calculations are particularly complicated when there is condensed species (liquids and solids) in the exhaust. Nonetheless, this simple calculation allows us to see which fuels warrant a closer examination.
Pentaborane is a compound that I dug up just by looking for something that appeared to meet the criteria – low exhaust molecular weight and liquid through a good temperature range. However, someone pointed out to me that boron is a neutron absorber; therefore it might adversely affect the function of the reactor. I’m also concerned about the carbon containing compounds because they might foul the engine with soot, particularly if the engine is to be restartable or reusable.
If you can find any other potential fuels, please share them with us.
The situation changes at higher temperature, say >6000 K. At these temperatures, hydrogen and oxygen exist mainly in their monatomic forms. Water will also breakdown into predominately H and O. Nitrogen, however, will remain mostly in its diatomic form. At high temperature we have,
Fuel Exhaust Products Mass Moles Mass/Mole
Hydrogen, H2 2 H 2.02 2 1.01
Methane, CH4 1 C(g) + 4 H 16.04 5 3.21
Propane, C3H8 3 C(g) + 8 H 44.10 11 4.01
Pentaborane, B5H9 5 B(s) + 9 H 63.12 14 4.51
Ammonia, NH3 3 H + ½ N2 17.03 3.5 4.87
Ethanol, C2H6O 2 C(g) + 6 H + 1 O 46.07 9 5.12
MMH, CH6N2 1 C(g) + 6 H + 1 N2 46.07 8 5.76
Water, H2O 2 H + 1 O 18.02 3 6.01
UDMH, C2H8N2 2 C(g) + 8 H + 1 N2 66.10 11 6.01