Atwood machine with variable mass

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Homework Help Overview

The discussion revolves around an Atwood machine involving a bucket with water that has a hole at the bottom, causing the mass to change over time. The problem involves determining the speed of the two masses in the system as a function of time, given certain constants and conditions.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the use of momentum equations and the role of external forces in the system. There is discussion about how to handle the tension in the rope and the implications of the variable mass of the bucket. Questions arise regarding the definitions of mass and forces involved, as well as the integration of equations to find speed as a function of time.

Discussion Status

Participants are actively engaging with the problem, attempting to derive equations and clarify the relationships between the variables. There are multiple interpretations of how to approach the tension and force balance, with some participants suggesting different methods to eliminate variables. No consensus has been reached on a single approach, but there is a productive exchange of ideas and equations.

Contextual Notes

Participants note the complexity of the equations involved and the potential for confusion due to the changing mass of the bucket. There are also references to specific constants and initial conditions that may affect the formulation of the problem.

titansarus
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Homework Statement


We have an Atwood machine like the picture below. one side (left) is a bucket full of water which has a hole on the bottom and the water is flowing with rate ##dm/dt = \alpha = const##. The initial mass of bucket with the water is ##m_0##. On the other side (right) we have a box with constant mass ##m_1##. We also know the speed of water relative to the system at every time is a constant number ##v_0## (It is given in the question). we want to find the speed of each box (which is equal in opposite directions) at every time ##t##. In fact we want to find ##v(t)## (##v## as a function of ##t##).
Note: Pulley and rope and etc... are all frictionless - massless and completely ideal. And the pulley is fixed to somewhere (maybe wall or roof, so it doesn't move)

variable mass.png


The Attempt at a Solution


After solving the equations of momentum for an arbitrary system of initial mass ##M##, I get the formula
##M dv/dt = F_{ext} + v_{rel}~~ dm/dt##.

in this question ##v_{rel}## and ##dm/dt## are both known constants. But I don't know what to do with ##F_{ext}##. Is it for the whole system? Is it just for the bucket? What is ##M## in the question: ##m_0## or ##m_0 + m_1##? What should I do to get a integrable equation?
 

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The least confusing approach is to assign a variable T=T(t) to the tension and consider the two suspended masses separately.
 
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haruspex said:
The least confusing approach is to assign a variable T=T(t) to the tension and consider the two suspended masses separately.
Now how to work with this T? I wrote ##m_1 g - T = m_1 a## and ##T - m(t) g = m(t) a## . Now maybe by dividing both sides, we get something like ##m_1 g - T / (T - m(t) g) = m_1 / m(t)## , we get an equation for T(t) in terms of ##m_1## and ##m(t)##. It is ##T(t) = 2 m_1 m(t) g / (m_1 + m(t)) ## Also ##m(t) = m_0 + \alpha t## (##\alpha## is negative).

Now I think I must write something like ##m_0 dv/dt = (T - m(t) g) + v_0 \alpha~~~## ? Is it OK? from this I get ## m_0 dv = (T - (m_0 + \alpha t) g)~dt + v_0 \alpha ~ dt##
I used wolfram alpha to evaluate this and I get:
##
\left(-\frac{2 g m_1^2 \log (\alpha t+m_0+m_1)}{\alpha}-\frac{1}{2} \alpha g t^2+\alpha v_0 t-m_0 g t+2 g m_1
t\right)
= m_0 V(t)## by assuming that ##v## of the system was at ##t=0## was zero. And we get ##V(t)## from here. Is it Right? Does it really get that complicated?
 
titansarus said:
Now I think I must write something like ##m_0 dv/dt = (T - m(t) g) + v_0 \alpha~~~## ?
No, you should have used that earlier:
titansarus said:
Now how to work with this T? I wrote ##m_1 g - T = m_1 a## and ##T - m(t) g = m(t) a## .
v0 features in the force balance on m0.
When you have that right, your first step should be to eliminate T.
 
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haruspex said:
No, you should have used that earlier:

v0 features in the force balance on m0.
When you have that right, your first step should be to eliminate T.
I think you mean something like: ##m_0 dv / dt + (m_0 + \alpha t) g - v_0 \alpha = T##, right? Now should I substitute this in ##T - m(t) g = m(t) a## or maybe ##m_1 g - T = m_1 a##? Or should I write something like ##m_1 g - m(t) g = (m_1 + m(t)) a##? Or maybe both?
 
haruspex said:
No, you should have used that earlier:

v0 features in the force balance on m0.
When you have that right, your first step should be to eliminate T.
I evaluated what I said in post #5 (above post) and substituted T in the equation that has m(t) and multiplied them by ##dt## and I got a huge formula like: ##
\frac{2 \alpha^2 t {v_0}-4 g {m_1}^2 \log (\alpha t+{m_0}+{m_1})-g (\alpha
t+{m_0}+{m_1})^2+6 g {m_1} (\alpha t+{m_0}+{m_1})}{2 \alpha} = m_0 v(t)
##or actually this according to wolfram alpha:
integral.png


If I substituted that in the equation with m1, it might get a little smaller but it will still be a big equation.
 

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titansarus said:
I think you mean something like: ##m_0 dv / dt + (m_0 + \alpha t) g - v_0 \alpha = T##, right?
A few problems there.
What is the mass on the left at time t?
Write the equation in the form ΣF=ma; that helps in getting the signs right.
 
titansarus said:
I got a huge formula like:
I also get a log function, but I don't think you should have had quadratic terms. Please post your working next time.
 

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