Spaceship ejecting mass at right angles

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Homework Help Overview

The problem involves a spaceship of mass ##m_0## moving with a constant velocity ##v_0##, which changes its direction by ejecting gas at right angles to its motion. The goal is to determine the angle ##\alpha## through which the spaceship's motion deviates as its mass decreases to ##m## during the ejection process.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the conservation of momentum and the implications of mass ejection on the spaceship's trajectory. There are attempts to derive the angle ##\alpha## using differential equations and momentum components. Some participants express uncertainty about the correctness of their approaches and the signs in their equations.

Discussion Status

Several participants have provided hints and clarifications regarding the notation and the relationships between the mass of the spaceship and the mass ejected. There is ongoing exploration of the correct expressions and signs, with some participants acknowledging potential errors in their reasoning.

Contextual Notes

Participants are grappling with the implications of mass loss on the momentum of the spaceship and the exhaust cloud, questioning the definitions and assumptions used in their calculations. There is a recognition that the mass of the spaceship decreases, which is central to the problem's setup.

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Homework Statement


A spaceship of mass ##m_0## moves in the absence of external forces with a constant velocity ##v_0##. To change the motion direction, a jet engine is switched on. It starts ejecting a gas jet with velocity u which is constant relative to the spaceship and directed at right angles to the spaceship motion The engine is shut down when the mass of the spaceship decreases to ##m##. Through what angle ##\alpha## did the motion direction of the spaceship deviate due to the jet engine operation?

Homework Equations


The Attempt at a Solution


Since there are no external forces, the momentum is conserved. Let the initial direction of motion be the x-axis. At time t, assume that spaceship rotates by an angle ##\theta## and its mass is m(t). The momentum in x direction is ##m(t)v_0\cos(\theta)##. When it ejects mass of dm at t+dt, let it rotate by angle ##d\theta##. The momentum in x-direction at t+dt is ##(m(t)-dm)v_0\cos(\theta+d\theta)+dm(u\sin\theta+v_0\cos\theta)##. Equating them and using ##\cos(\theta+d\theta)=\cos\theta-\sin\theta d\theta## gives
$$dm u=m(t)v_0d\theta$$
Solving the D.E (limits for ##\theta##: 0 to ##\alpha## and for m: ##m_0## to ##m##),
$$\alpha=(v_0/u)\ln(m/m_0)$$
But this is wrong. The given answer is ##\alpha=(v_0/u)\ln(m_0/m)##. I believe there is a sign error but I am not able to spot it. I am not sure if I approached the problem correctly.

Any help is appreciated. Thanks!
 

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Hi Pranav-Arora! :smile:

ln(1/x) = … ? :wink:
 
Pranav-Arora said:
The given answer is ##\alpha=(v_0/u)\ln(m_0/m)##.
Are you sure this is the answer?

I believe there is a sign error but I am not able to spot it.

Hint: What you have called "##dm##" is not quite the differential of ##m(t)##.

I am not sure if I approached the problem correctly.

I think your approach is ok. But there is no loss of generality in choosing the orientation of the x-axis to be the direction of the velocity of the ship at time t. Then take momentum components in the y-direction for t and t + dt.
 
tiny-tim said:
Hi Pranav-Arora! :smile:

ln(1/x) = … ? :wink:

-ln(x). Not sure how it helps though. I get a negative answer if I use this.

TSny said:
Are you sure this is the answer?
Sorry, it is ##(u/v_0)## instead of ##(v_0/u)##. :redface:

I too get ##(u/v_0)##. I wrote it wrong while making the post.
Hint: What you have called "##dm##" is not quite the differential of ##m(t)##.
Is it completely wrong or have I used incorrect notations? :confused:

I guess I should simply write m instead m(t) to avoid confusion.

I think your approach is ok. But there is no loss of generality in choosing the orientation of the x-axis to be the direction of the velocity of the ship at time t. Then take momentum components in the y-direction for t and t + dt.
At time t, momentum in y direction, ##mv_0\sin(\theta)##
At time t+dt, ##(m-dm)v_0\sin(\theta+d\theta)+dm(-u\cos\theta+v_0\sin\theta)##
Equating them and solving gives me the same answer again. I still cannot spot the sign error. :(
 
Suppose you write ##m_s(t)## for the mass of the ship and you let ##dm_e## be the mass ejected between t and t+dt. What is the relation between ##dm_e## and ##dm_s##?

The mass of the ship at t + dt is ##m_s(t+dt)##. How would you express ##m_s(t+dt)## in terms of ##m_s(t)## and ##dm_s##? How would you express ##m_s(t+dt)## in terms of ##m_s(t)## and ##dm_e##? [Edited]
 
Last edited:
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Pranav-Arora said:
Since there are no external forces, the momentum is conserved.
Just to be clear, it is the momentum of the spaceship + exhaust cloud system that is conserved. The spaceship's momentum is not a conserved quantity.
Pranav-Arora said:
I still cannot spot the sign error. :(
The quantity that you designated as dm is the (positive) quantity of mass ejected by the spacecraft during the time interval dt. The mass of the exhaust cloud increases by dm. The mass of the spacecraft ? It decreases by dm. That's your sign error.
 
Pranav-Arora said:
A spaceship of mass ##m_0## …
… when the mass of the spaceship decreases to ##m##.

Solving the D.E (limits for ##\theta##: 0 to ##\alpha## and for m: ##m_0## to ##m##),
$$\alpha=(v_0/u)\ln(m/m_0)$$
But this is wrong. The given answer is ##\alpha=(v_0/u)\ln(m_0/m)##.

Pranav-Arora said:
-ln(x). Not sure how it helps though. I get a negative answer if I use this.

no, m < mo

so the given answer ##\alpha=(v_0/u)\ln(m_0/m)## is positive :smile:
 
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TSny said:
Suppose you write ##m_s(t)## for the mass of the ship and you let ##dm_e## be the mass ejected between t and t+dt. What is the relation between ##dm_e## and ##dm_s##?
##dm_s=-dm_e##?
The mass of the ship at t + dt is ##m_s(t+dt)##. How would you express ##m_s(t+dt)## in terms of ##m_s(t)## and ##dm_s##? How would you express ##m_s(t+dt)## in terms of ##m_s(t)## and ##dm_e##? [Edited]

##m_s(t+dt)=m_s(t)-dm_s=m_s(t)+dm_e##?

tiny-tim said:
no, m < mo

so the given answer ##\alpha=(v_0/u)\ln(m_0/m)## is positive :smile:
I know that the given answer is positive because m_0>m but I don't understand why do I get the negative answer.
 
Pranav-Arora said:
I know that the given answer is positive because m_0>m but I don't understand why do I get the negative answer.
Because you did this:

##m_s(t+dt)=m_s(t)-dm_s=m_s(t)+dm_e##?
Does that expression make any sense? (That's a rhetorical question. The answer is no.)

Here, ##dm_e## and ##dt## are (small) positive quantities, so what you are saying with that expression is that the spacecraft 's mass increases from time ##t## to time ##t+dt##.
 
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D H said:
Does that expression make any sense? (That's a rhetorical question. The answer is no.)

Here, ##dm_e## and ##dt## are (small) positive quantities, so what you are saying with that expression is that the spacecraft 's mass increases from time ##t## to time ##t+dt##.
Okay sorry for my foolishness. So the correct relation is ##m_s(t+dt)=m_s(t)-dm_e=m(t)+dm_s##.

If I use the proper signs, I get the correct answer. Thanks for the help everyone! :)
 

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