Momentum at time t and at a time t+dt for a rocket

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    Momentum Rocket Time
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Discussion Overview

The discussion revolves around the dynamics of variable-mass systems, specifically focusing on the momentum of a rocket at time t and at a time t+dt. Participants explore the implications of mass loss during motion and the corresponding changes in momentum, addressing both theoretical and conceptual aspects of the equations governing such systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Homework-related

Main Points Raised

  • Marcos presents the equation of variable-mass motion and questions the sign of ##dm## in the momentum equations, noting that it appears positive in one context and negative in another.
  • Some participants clarify that ##dm## is consistently negative, indicating mass loss, and that the signs in the equations reflect different contexts of mass gain and loss.
  • There is a discussion about the relative velocity of the mass being ejected and the rocket, with a participant asking whether these velocities are relative to Earth.
  • Another participant responds that the velocities are relative to any inertial reference frame, not just Earth.
  • A participant shares a geogebra file related to the momentum of a rocket, seeking validation of their work.
  • One participant acknowledges an error in a previously shared PDF regarding mass ablation and describes their drawing of the system as part of their studies for an entrance exam.

Areas of Agreement / Disagreement

Participants generally agree on the interpretation of ##dm## as negative due to mass loss, but there are varying perspectives on the application of the equations and the context of relative velocities. The discussion remains unresolved regarding the broader implications of these equations in different reference frames.

Contextual Notes

Some assumptions about the reference frames and the conditions under which the equations apply are not fully explored. The discussion includes different interpretations of the momentum equations without resolving the underlying complexities.

mcastillo356
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Hello, my name is Marcos, I have a bachelor in advertising and public relations, and my hobby is maths and physics
The equation of variable-mass motion is written as ##\mathbf{F}_{ext}+\mathbf{v}_{rel}\dfrac{dm}{dt}=m\dfrac{d\mathbf{v}}{dt}##
There are different derivations for the equation:
Mass accretion:
1575939389252.png

Mass ablation/ejection:
1575939579538.png

The initial momentum of the system is ##\mathbf{p}_1=m\mathbf{v}##. Since the mainbody will be losing mass, ##dm## will be negative. At a time ##t+dt## the momentum is ##\mathbf{p}_2=(m+dm)(\mathbf{v}+d\mathbf{v})+\mathbf{u}(-dm)##. Why in the same equation ##dm## is first positive and at the end negative?.
Full text at https://en.wikipedia.org/wiki/Variable-mass_system
Thanks!
 
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Since dm is negative, m+dm < m and -dm > 0. dm itself is negative, it does not change sign.

Since dm is the mass gained by the rocket (being negative means the rocket loses mass), the mass of the ejecta is -dm.
 
mcastillo356 said:
Why in the same equation ##dm## is first positive and at the end negative?.

It's not positive and negative in the same equation. ##dm## is whatever it is. Your question is really: "Why in the equation do we use ##+dm## in one place and ##-dm## in another? Or, why do we sometimes add ##dm## and sometimes subtract it?

To answer this, consider this equation, for example:

##a + b = (a + c) + (b - c)##
 
Thank you very much, Orodruin and Perok!. Question solved
 
Hello
The general equation of variable-mass motion is written as ##\mathbf{F}_{ext}+\mathbf{v}_{rel}\dfrac{dm}{dt}=m\dfrac{d\mathbf{v}}{dt}##, where ##\mathbf{F}_{ext}## is the net external force on the body, ##\mathbf{v}_{rel}## is the relative velocity of the escaping or incoming mass with respect to the center of mass of the body, and ##\mathbf{v}## is the velocity of the body
1576037359666.png

Noting that ##\mathbf{u}-\mathbf{v}## is the velocity of ##dm## relative to ##m##, simbolized as ##\mathbf{v}_{rel}##
The question is: velocity of ##dm## and ##m##, is relative to Earth?
Thanks!
 
It is relative to any inertial reference frame. The Earth is a good example, but any other inertial frame will do just as well too.
 
Hello!
Is the geogebra file I've attached the momentum for a rocket in motion at a time ##t## and at a time ##t+dt##?. I've done it inspired by
1576074794630.png

witch shows mass accretion for a variable-mass system.
Thanks!
 

Attachments

Thank you very much, Dale
 
Hello Orodruin
The pdf I attached drawing mass ablation for a variable-mass system like a rocket was not wright. I am student of spanish Uned, I am preparing a specific entrance exam to access maths degree. The image I've drawn is their advice. The system taken in account is the rocket and the fuel yet to burn. Thanks!
1576610090292.png

At time t it's m with velocity vector v, in the left; and in the right, at time t+dt, it's the rocket, with mass m-dm and velocity vector v+dv, and below, dm, with velocity vector u downwards, to preserve momentum
 

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