Rocket Propulsion Differential Equation Solution Help?

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Homework Help Overview

The discussion revolves around a differential equation modeling the vertical takeoff of a rocket in a gravitational field, specifically focusing on the relationship between mass ejection and velocity. The equation is presented as m\dot{v} = -\dot{m}v_{ex}-mg, with the assumption of a constant mass ejection rate.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the implications of the exhaust velocity, questioning whether it is a constant or varies. There are attempts to derive the correct form of the solution, with some participants expressing confusion over the signs and terms in the equation. The original poster reflects on their approach and considers the implications of the assumptions made regarding mass ejection and exhaust velocity.

Discussion Status

The discussion is ongoing, with participants providing insights and questioning each other's interpretations of the problem. Some guidance has been offered regarding the assumptions about exhaust velocity and mass ejection, but no consensus has been reached on the correct solution or interpretation of the variables involved.

Contextual Notes

Participants note that the problem assumes a constant rate of mass ejection, which may conflict with typical textbook scenarios where exhaust velocity is not assumed to be constant. There is also mention of constraints based on the physical limits of the rocket's fuel mass.

McCoy13
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Homework Statement


Consider the case of a rocket taking off vertically from rest in a gravitational field g. The differential equation is given by

m\dot{v} = -\dot{m}v_{ex}-mg

Assume the rocket ejects mass at a constant rate, \dot{m}=-k (where k is a positive constant), so that m=m_{0}-kt. Solve equation for v as a function of t, using separation of variables.

Homework Equations



m\dot{v} = -\dot{m}v_{ex}-mg

The Attempt at a Solution



m\dot{v} = -\dot{m}v_{ex}-mg

(m_{0}-kt)\frac{dv}{dt}=-kv_{ex}-(m_{0}-kt)g

\frac{dv}{dt}=\frac{-kv_{ex}}{m_{0}-kt}-g

dv=(\frac{-kv_{ex}}{m_{0}-kt}-g)dt

v(t)=v_{ex}ln(m_{0}-kt)-gt-c

Setting t = 0, it appears that c=v_{ex}ln(m_{0}).

However, the next step of the problem is to plug in values, which revealed that this clearly isn't the right solution. I attempted to solve it again and ended up with the same solution, so I'm obviously having some difficulty recognizing my mistake.
 
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You mistook v_{ex} (I don't know what ex stands for). That is the relative velocity of the rocket relative to the mass dm it has just ejected, NOT some constant.
Derive yourself the differential equation for the motion of the rocket and you will see why :wink:
 
hikaru1221 said:
You mistook v_{ex} (I don't know what ex stands for). That is the relative velocity of the rocket relative to the mass dm it has just ejected, NOT some constant.
Derive yourself the differential equation for the motion of the rocket and you will see why :wink:

Thanks! That has got to be what I was missing.
 
McCoy13 said:
Thanks! That has got to be what I was missing.

Wait, no, it is most definitely a constant. That is the velocity of the exhaust relative to the rocket, which is constant. They take this into account during the derivation of the differential equation by noting that the velocity of the mass ejected with respect to the ground is velocity of the rocket minus the exhaust velocity.

I think my mistake may lie in something much simpler. \dot{m} = -k, not just k. This flips the sign of the two natural logs, and the equation makes much more sense. This way v grows as a function of t, though it eventually becomes asymptotic on a large enough domain of t. This is because the rocket isn't entirely made out of fuel, so we have to limit t to a domain such that 0 < k*t <= mass of fuel < initial mass of rocket. I think the solution is as follows.

v(t) = -v_{ex}*ln(m_{0}-kt)-gt+v_{ex}ln(m_{0})
 
McCoy13 said:
Wait, no, it is most definitely a constant. That is the velocity of the exhaust relative to the rocket, which is constant.
This is deadly wrong. Not so obvious. Don't state without proof.
Most textbooks when analyzing the rocket motion assume that the exhaust velocity is constant, but don't assume that dm/dt = const. Here the problem assumes that dm/dt = const, but not exhaust velocity. Therefore, the results in 2 cases (textbooks vs this problem) are different.

I think my mistake may lie in something much simpler. \dot{m} = -k, not just k.

Look back again. You DIDN'T make that mistake :biggrin: You got m=m_o-kt. Isn't it the same as dm/dt = -k?
 
hikaru1221 said:
Look back again. You DIDN'T make that mistake :biggrin: You got m=m_o-kt. Isn't it the same as dm/dt = -k?
Actually I did. Though what you say is correct, when I substituted \dot{m}=-k into -v_{ex}\dot{m} I got -v_{ex}k instead of v_{ex}k. This is the mistake I was referring to.

hikaru1221 said:
This is deadly wrong. Not so obvious. Don't state without proof. Most textbooks when analyzing the rocket motion assume that the exhaust velocity is constant, but don't assume that dm/dt = const. Here the problem assumes that dm/dt = const, but not exhaust velocity. Therefore, the results in 2 cases (textbooks vs this problem) are different.
This may be so, but this one seems to assume both. Let me give you the relevant portions of the problem to explain why I am assuming so.

"Assume that the rocket ejects mass at a constant rate, \dot{m}=-k..."

"Using rough data from Problem 3.7, find the space shuttles speed two minutes into flight...

(From problem 3.7) "...the average exhaust speed v_{ex} is about 3000 m/s..."

It provides no other indication of what v_ex is or should be. It is also fairly obvious that without an explicit formula for v_ex (or even if we had one that was non-constant), that the differential equation would not be solvable by separation of variables because of the addition of -g. Therefore, given the weight of these factors, I can only assume that both dm/dt and v_ex are constant.
 
I will, however, grant that the use of the word "average" implies that v_ex isn't constant, but again, without any other kind of knowledge of what v_ex may be, I don't think I have another choice.
 
I'm fairly certain my corrected solution is the right one.

In a later problem it gives the following as the solution for y(t):

y(t)=v_{ex}t-\frac{1}{2}gt^{2}-\frac{mv_{ex}}{k}ln(\frac{m_{0}}{m})

If we make the substitution for m=m_{0}-kt and then differentiate, you get the solution I posted above.
 
McCoy13 said:
I'm fairly certain my corrected solution is the right one.

In a later problem it gives the following as the solution for y(t):

y(t)=v_{ex}t-\frac{1}{2}gt^{2}-\frac{mv_{ex}}{k}ln(\frac{m_{0}}{m})

If we make the substitution for m=m_{0}-kt and then differentiate, you get the solution I posted above.

If that's so, then I can only assume that the problem misses a point about v_ex :smile:
 
  • #10
Could be! But if it's the textbook's fault and not mine, then I can just submit this and remember the point you raised.
 

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