2 Masses and a Wheel (with mass)

AI Thread Summary
The discussion focuses on deriving the final velocity of a system involving two masses and a rotating wheel. The initial equation connecting final velocity to distance is modified to account for rotational motion, leading to the expression for angular acceleration. Participants clarify the need to consider the forces acting on the masses and the wheel, ultimately deriving the acceleration formula. The final velocity is calculated using the derived acceleration, with participants confirming a specific value of 2.89 m/s as the correct answer. The conversation emphasizes the importance of correctly applying torque and force equations in the analysis.
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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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.
 
PS I don't get any of those answers!
 
PeroK said:
PS I don't get any of those answers!
Did you get 2.89 m/s?
 
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:
$$a = \frac{M-m}{M+m+m_w}g$$
 
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$$I_w \omega^2 = m_wR^2(\frac v R)^2 = m_wv^2$$
 
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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