Why Doesn't Constant Center of Mass Velocity Reduce Degrees of Freedom?

In summary, the concept of constant center of mass (COM) velocity in a system does not reduce the degrees of freedom because the motion of individual components can vary while still maintaining a fixed COM velocity. Each particle's movement can be independent, allowing for complex interactions and configurations without impacting the overall velocity of the system's center of mass. Consequently, the system retains its full degrees of freedom, as constraints on motion do not limit the variety of configurations that can exist while the COM remains constant.
  • #1
deuteron
60
13
Homework Statement
What are the constraints of the system?
Relevant Equations
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Consider the above system, where both the wedge and the mass can move without friction. We want to get the equations of motion for the both of them using Lagrangian formalism, where the constraints in the solution sheet are given as:

$$y_2=0$$
$$\tan \alpha=\frac {y_1}{x_1-x_2}$$

However, since there is no net force on the system in the ##x-##direction, can't we also say that the center of mass has constant velocity, where we can choose an inertial frame in which ##\dot x_{cm}=0##, and thus

$$\dot x_{cm} =\frac {m_1\dot x_1 +m_2\dot x_2}{m_1+m_2}=0\ \Rightarrow\ m_1\dot x_2 = -m_2\dot x_2$$

which would reduce the number of degrees of freedom to ##1##?
 
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  • #2
Okay, but you were asked for the equations of motion.
 
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  • #3
deuteron said:
Homework Statement: Find the equations of motion
Relevant Equations: .

View attachment 332662

Consider the above system, where both the wedge and the mass can move without friction. We want to get the equations of motion for the both of them using Lagrangian formalism, where the constraints in the solution sheet are given as:

$$y_2=0$$
$$\tan \alpha=\frac {y_1}{x_1-x_2}$$

However, since there is no net force on the system in the ##x-##direction, can't we also say that the center of mass has constant velocity, where we can choose an inertial frame in which ##\dot x_{cm}=0##, and thus

$$\dot x_{cm} =\frac {m_1\dot x_1 +m_2\dot x_2}{m_1+m_2}=0\ \Rightarrow\ m_1\dot x_2 = -m_2\dot x_2$$

which would reduce the number of degrees of freedom to ##1##?
Not really. The system has two degrees of freedom, but under gravity alone, the motion of the small block down the wedge is related to the motion of the wedge.
 
  • #4
PeroK said:
Okay, but you were asked for the equations of motion.
The constraints were a sub-question, I changed it now, sorry :')
 
  • #5
PeroK said:
Not really. The system has two degrees of freedom, but under gravity alone, the motion of the small block down the wedge is related to the motion of the wedge.
Why is the relationship not a constraint that reduces the number of degrees of freedom? Wouldn't we know the position of the wedge if we knew the position of the mass, using ##\dot x_{cm}=0##?
 
  • #6
deuteron said:
Why is the relationship not a constraint that reduces the number of degrees of freedom? Wouldn't we know the position of the wedge if we knew the position of the mass, using ##\dot x_{cm}=0##?
Suppose you put a small block on a larger rectangular block on a smooth surface. The system, under gravity alone, does not move. That doesn't mean it has zero degrees of freedom. The blocks are still free to move independently.
 

FAQ: Why Doesn't Constant Center of Mass Velocity Reduce Degrees of Freedom?

How do you set up the coordinate system for analyzing the mass on a wedge problem?

To analyze the mass on a wedge problem, set up a coordinate system where one axis (usually the x-axis) is aligned with the inclined plane of the wedge, and the other axis (the y-axis) is perpendicular to it. This simplifies the decomposition of forces acting on the mass. For the wedge itself, a horizontal and vertical coordinate system can be used to analyze its motion.

What forces act on the mass placed on the wedge?

The forces acting on the mass include gravitational force (mg), the normal force exerted by the wedge, and the frictional force if friction is present. The gravitational force can be decomposed into components parallel and perpendicular to the inclined plane of the wedge.

How do you account for the motion of both the mass and the wedge?

To account for the motion of both the mass and the wedge, apply Newton's second law to each body separately. For the mass, consider the forces along the inclined plane and perpendicular to it. For the wedge, consider the horizontal and vertical forces. Use constraints like the no-slip condition if friction is involved to relate their accelerations.

What is the role of friction in the mass on a wedge problem?

Friction plays a crucial role in determining whether the mass will slide on the wedge or stay in place. If friction is sufficient, it can prevent relative motion between the mass and the wedge. If friction is not enough, the mass will slide, and you will need to include the frictional force in your equations of motion.

How do you solve for the accelerations of the mass and the wedge?

To solve for the accelerations, set up the equations of motion for both the mass and the wedge using Newton's second law. For the mass, resolve the forces into components along the inclined plane and perpendicular to it. For the wedge, consider the horizontal forces. Solve the system of equations simultaneously to find the accelerations of both the mass and the wedge.

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