Rocket equation exhaust velocity question

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SUMMARY

The discussion centers on the rocket equation, specifically Delta V = Ve ln (Mo/M), which defines exhaust velocity (Ve) as crucial for achieving orbital velocity. It clarifies that a bipropellant rocket engine with an exhaust velocity of 4.4 km/s can still reach the necessary 7.8 km/s for Low Earth Orbit by utilizing a significant fuel mass, calculated to be 4.87 times the mass of the rocket. The conversation emphasizes that conservation of momentum is maintained, as the mass of the propellant far exceeds the rocket's mass, allowing for the correct application of the rocket equation even when considering the fuel still in the chamber.

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  • Understanding of the rocket equation and its components (Delta V, Ve, Mo, M)
  • Basic knowledge of conservation of momentum principles
  • Familiarity with bipropellant rocket engines and their performance metrics
  • Comprehension of gravitational forces and their impact on rocket launches
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  • Study the derivation and applications of the rocket equation in various launch scenarios
  • Explore advanced propulsion concepts, including specific impulse and thrust-to-weight ratio
  • Investigate the effects of varying exhaust velocities on rocket performance
  • Learn about real-world rocket launches and the calculations involved in mission planning
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Aerospace engineers, rocket scientists, physics students, and anyone interested in the mechanics of rocket propulsion and orbital dynamics will benefit from this discussion.

randomking333
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The rocket equation given by Delta V = Ve ln (Mo/M) says that Ve is the exhaust velocity of the rocket.

The orbital velocity for Low Earth Orbit is about 7.8 Km/s. How then, is this velocity attained by a rocket which is fuelled only by a bipropellant rocket engine producing an exhaust velocity of 4.4 Km/s. Using conservation of momentum, the heavier mass of the rocket won't reach the velocity of the exhaust?

Pls explain to me how this works..

THanks in advance
 
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In The rocket equation, Mo would be the Mass of ship+fuel and M would be the mass of the ship alone.

Given that, we can solve for the fuel mass by:

e^{\frac{\Delta V}{V_e}}= \frac{M_s+M_f}{M_s}

e^{\frac{\Delta V}{V_e}}= \frac{M_f}{M_s}+1

M_s e^{\frac{\Delta V}{V_e}}-1= M_f

With the given final velocity and escape velocity, this gives a fuel mass of 4.87 times that of the mass of the ship alone. So the mass of the fuel is far greater than the mass of the rocket, and there is no problem with conservation of momentum.
 
Mass of the stage of the rocket that reaches orbital velocity is far, far smaller than total mass of the propellant. If you were simply applying a conservation of momentum, you'd end up with final speeds well above orbital. The reason you get only 7.8km/s is that propellant ends up traveling at speeds varying from -4.4km/s to +3.4km/s. The rocket formula you quoted is a result of adding up momenta of all these contributions in correct proportions.
 
Janus said:
In The rocket equation, Mo would be the Mass of ship+fuel and M would be the mass of the ship alone.

Given that, we can solve for the fuel mass by:

e^{\frac{\Delta V}{V_e}}= \frac{M_s+M_f}{M_s}

e^{\frac{\Delta V}{V_e}}= \frac{M_f}{M_s}+1

M_s e^{\frac{\Delta V}{V_e}}-1= M_f

With the given final velocity and escape velocity, this gives a fuel mass of 4.87 times that of the mass of the ship alone. So the mass of the fuel is far greater than the mass of the rocket, and there is no problem with conservation of momentum.


Yes.. but for any point in time taken.. say a span of 1 second early in the launch...

mv=mv

so the pass of the rocket at that time is much greater.. since the exhaust velocity is of the fuel being burned per unit time?.. so that mass of fuel is a lot less? .. or are we meant to consider even the fuel that is still in the chamber and not burnt (and hence not at that exhaust velocity)

Thanks in advance
 
randomking333 said:
Yes.. but for any point in time taken.. say a span of 1 second early in the launch...

mv=mv

so the pass of the rocket at that time is much greater.. since the exhaust velocity is of the fuel being burned per unit time?.. so that mass of fuel is a lot less? .. or are we meant to consider even the fuel that is still in the chamber and not burnt (and hence not at that exhaust velocity)

Thanks in advance

Let's take the first second of launch. First you have to overcome the force of gravity which is the equivalent of 9.8m/s². Which means that it is the same as accelerating to 9.8 m/s in one second. Using the rocket equation we find that it would take 2.2e-3 times the remaining mass of the ship to do this.( In this case, Mo is equal to the mass of the rocket plus the un-used fuel on board)

IOW, with an exhaust velocity of 4.4 km/s, If you burn about 2 one-thousandths of the ships total mass in the first second, you will overcome gravity. Anything over that will accelerate the ship upward.

In terms of momentum, if MV is the final momentum of the ship and mv is the momentum of the exhausted fuel, then at a v of 4400 m/s, at V of 9.8m/s:

9.8M= 4400m

m/M = 9.8/4400 = 0.0022

Which again gives an answer of about 2/1000 of the ships total mass needed to be burned in one second to overcome gravity.

If you carry out the above solutions to a few more decimal places you will find that the rocket equation gives a slightly larger value. This is because it factors in the fact that during the first part of the second, the rocket has to still lift the fuel it will burn later in the sec. That is the point of using the rocket equation, it takes into account the mass of the remaining unused fuel.
 
Although the terminal exhaust velocity relative to the rocket is fixed, that exhaust accelerates both the rocket and the remaining on board fuel, so that as the rockets and on board fuel increases speed, so does the exhaust velocity (with repect to the initial velocity of the rocket).
 

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