2 Masses and a Wheel (with mass)

In summary, "2 Masses and a Wheel (with mass)" explores the dynamics of a mechanical system consisting of two masses and a wheel that has its own mass. The study focuses on how the masses interact with the wheel, considering factors like inertia, rotational motion, and the forces acting on the system. The analysis includes mathematical modeling to understand the equilibrium and motion of the masses in relation to the wheel, providing insights into the principles of physics governing such systems.
  • #1
PhDeezNutz
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Homework Statement
See Pic Below
Relevant Equations
##v_f^2 = v_i^2 + 2a \Delta y##
##I_{ring} = m_w R^2##
## a = R \alpha##
##\sum \tau = I \alpha##
FF7B6B34-823F-4FAD-BB21-F7D4F98EB389.jpeg



The equation that connects final velocity with distance traveled is

##v_f^2 = v_i^2 + 2a \Delta y##

Since the system starts from rest ##v_i = 0##

and the above equation becomes.

##v_f^2 = 2a \Delta y##

Since there is rotation in this system we need to connect ##a## to the rotation of the wheel. ##a = \alpha R##. So that becomes

##v_f^2 = 2 \alpha R \Delta y##

Now we need to find ##\alpha## my summing the torques and setting it equal to ##I \alpha## where ##I = m_w R^2##. Although R wasn't given in the problem statement I figure we still need it even though it will cancel out in the end.


##\sum \tau = I \alpha##

I'm going to choose the counterclockwise direction as positive.

##MgR - mgR = m_w R^2 \alpha##

##\alpha = \frac{g R\left(M-m \right)}{m_w R^2} = \frac{g \left(M - m \right)}{m_w R}##

So

##v_f^2 = 2 \left(\frac{g\left( M - m\right)}{m_w R} \right) R \Delta y##

##v_f = \sqrt{\frac{2g \left(M-m\right)}{m_w} \Delta y}##

When I plug in ##M = 20##, ##m = 5##, ##m_w = 10##, and ##\Delta y = 1## I get

##v_f = 5.42##

Where did I go wrong? This is different than the stated answer.
 
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  • #2
You can't assume that the mass ##M## creates a tension of ##Mg## in the string. If it did, it would not iself be accelerating.
 
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  • #3
PS I don't get any of those answers!
 
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  • #4
PeroK said:
PS I don't get any of those answers!
Did you get 2.89 m/s?
 
  • #5
PhDeezNutz said:
Did you get 2.89 m/s?
Yes, with ##g = 9.8m/s^2##.

Here's a quick way. Note that ##M, m## and every mass element on the rim of the wheel must have the same speed ##v##. The total external force on the system is ##Mg - mg##, so we have:
$$a = \frac{M-m}{M+m+m_w}g$$
 
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  • #6
PS From the kinematic equation, we have:
$$v^2 = 2as$$And this is also what we get from the energy equation:
$$\frac 1 2(M + m + m_w)v^2 = (M-m)gs$$Where ##s## is the distance ##M## moves.

You can also verify the trick, as the total KE is:
$$KE = \frac 1 2(M+m)v^2 + \frac 1 2 I_w \omega^2$$And$$I_w \omega^2 = m_wR^2(\frac v R)^2 = m_wv^2$$
 
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  • #7
PeroK said:
Yes, with ##g = 9.8m/s^2##.

Here's a quick way. Note that ##M, m## and every mass element on the rim of the wheel must have the same speed ##v##. The total external force on the system is ##Mg - mg##, so we have:
$$a = \frac{M-m}{M+m+m_w}g$$
That’s exactly what I got!!

Just to hash out details.

Torque Equation on the Wheel

##m_w R^2 \alpha = m_w R^2 \frac{a}{R} = m_w aR = F_1 R - F_2 R##

Force on ##M##

##Mg - F_1 = Ma##

##F_2 - mg = ma##

So

##F_1 = M \left( g - a\right)##
##F_2 = m\left( a + g \right)##

Plugging that into the sum of torques equation

##m_w a R = MgR - MaR - maR -mgR##

leading to your result

## a = \frac{\left( M-m \right)g}{m_w + m + M}##

All that is left to do is plug it into ##v_f = \sqrt{2 a \Delta y}##
 
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