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
813
559
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.
 
Physics news on Phys.org
  • #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.
 
  • Like
Likes PhDeezNutz
  • #3
PS I don't get any of those answers!
 
  • Like
Likes PhDeezNutz
  • #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:
$$a = \frac{M-m}{M+m+m_w}g$$
 
  • Like
Likes PhDeezNutz
  • #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$$I_w \omega^2 = m_wR^2(\frac v R)^2 = m_wv^2$$
 
  • Like
Likes PhDeezNutz
  • #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}##
 
  • Like
Likes PeroK

FAQ: 2 Masses and a Wheel (with mass)

What is the basic setup for the "2 Masses and a Wheel" problem?

The basic setup involves a wheel with mass and two masses connected by a string. The string passes over the wheel, which is typically considered to be a pulley. One mass hangs on one side of the wheel, and the other mass hangs on the opposite side. The system is used to study the dynamics of rotational motion and linear acceleration.

How do you calculate the acceleration of the masses?

To calculate the acceleration of the masses, you need to consider both the rotational inertia of the wheel and the linear forces acting on the masses. Using Newton's second law for rotation and translation, you can derive the equations of motion. The acceleration can be found by solving these coupled equations, taking into account the tension in the string and the gravitational forces on the masses.

What role does the moment of inertia of the wheel play in the system?

The moment of inertia of the wheel is crucial because it determines how the wheel resists rotational acceleration. A larger moment of inertia means the wheel will accelerate more slowly for a given torque. This affects the overall acceleration of the masses since the tension in the string must overcome not only the gravitational forces on the masses but also the rotational inertia of the wheel.

How do you account for friction in the "2 Masses and a Wheel" problem?

Friction can be accounted for by including a frictional torque in the equations of motion. This torque opposes the rotation of the wheel and is proportional to the normal force and the coefficient of friction. In some cases, friction in the axle of the wheel or between the string and the wheel might also need to be considered. These factors will reduce the net torque and, consequently, the acceleration of the system.

What assumptions are typically made to simplify the "2 Masses and a Wheel" problem?

Common assumptions include neglecting air resistance, assuming the string is massless and inextensible, and considering the wheel to be a perfect pulley with no slippage between the string and the wheel. Additionally, the system is often assumed to be in a uniform gravitational field, and the masses are point masses. These simplifications help in deriving analytical solutions to the problem.

Back
Top