Perhaps it would help to think of the transfer of momentum involved in the rocket thrust equation directly.<br />MBA_UIU, you are correct in the sense that propellant velocity is a limiting factor in the desing of a chemical rocket, as it is in all rockets, but that is only telling half the story. The other half is of course the "mdot" in the "Mdot*Ve" of the momentum thrust. This represents the mass flow rate of the propellant. Though Ve is limited by the energy contained within the fuel, in theory, if we can build a big enough rocket, we can carry as much mass as we want, allowing us to go as fast as we want (as long as we increase the propellant mass ratio. <br /><br />Let's illustrate this with a simplified example. Suppose we have a rocket with 1kg of structural mass, which carries 100kg of propellant. We then instantaneously propell this mass to 1m/s, what one considers a slow propellant speed. ("Instantaneously" just so we can skip over the calculus, which would force us to rederive the fundemental rocketry equation, DV = Ve ln(M0/Me), but essentially the point is the same)<br /><br />By conservation of momentum (the basis for momentum thrust in the rocket propulsion equation):<br /><br />m1*V1 =m2*V2 + m3*V3<br /><br />(1kg + 100kg) * V1 = 100kg * V2 + 1kg * V3<br /><br />V1 is the inital velocity of the rocket/propellant system, which we will assume was at rest (V1 = 0).<br /><br />V2 is the propellant velocity. If we define the forward direction of the rocket to be positive, and the propellant is ejected backward, then V2 = -1 m/s.<br /><br />We don't know V3, the velocity of the rocket after it expells the propellant, so lets solve for it:<br /><br />(101kg)*0m/s = 100kg * (-1m/s) + 1kg*V3<br /><br />0 kg*m/s = -100 kg*m/s + 1kg*V3<br /><br />100kg*m/s = 1kg*V3<br /><br />Thus V3 = 100 m/s, and our rocket is travelling 100 times faster than Ve!<br /><br />Note that if we remove the instantaneous bit of the equation and employ the fundamental rocketry equation, the answer becomes: