Does a body behave as a point mass even at rest?

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Discussion Overview

The discussion revolves around whether a body behaves as a point mass when at rest, specifically when no external force is applied. Participants explore the implications of this behavior in the context of Newton's laws and the motion of the center of mass, considering both translational and rotational dynamics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that a body behaves as a point mass when a force is applied, questioning if this holds true when no external force is present.
  • Others argue that a rigid body does not behave as a point mass due to potential rotational motion, even if the center of mass moves as if all mass is concentrated there.
  • It is proposed that when external forces sum to zero, the center of mass will remain at rest or move at constant speed, suggesting that the mass can be treated as concentrated at the center of mass for problem-solving purposes.
  • Some participants emphasize the importance of considering both translational and rotational motion, noting that external forces can lead to changes in rotational kinetic energy.
  • There are discussions about the complexities involved in conservation laws when both translational and rotational motions are present.
  • One participant mentions that the concept of treating a body as a point mass depends on the size of the body relative to other distances involved in the problem.

Areas of Agreement / Disagreement

Participants express differing views on whether a body can be treated as a point mass at rest without external forces. While some agree on the conditions under which this is valid, others highlight the complications introduced by rotational motion and the need for careful consideration of forces and torques.

Contextual Notes

Limitations include the dependence on definitions of point mass and center of mass, as well as the unresolved implications of rotational motion on translational dynamics. The discussion does not reach a consensus on the treatment of bodies at rest as point masses.

  • #31
mark2142 said:
How can if one force is causing the rotational motion can cause translational motion too. Like we can either toss a body high up or rotate it in air. We can't toss and rotate both at the same time.
Have you never played or watched any sport?

In particular, if you go to "Highland Games" in Scotland, you'll find a contest called "tossing the caber", where a tree trunk is projected with both linear and rotational motion. Look on YouTube.

You seem to be unable to relate physics to the real world. If you went out into the street and gave someone a ball, they could throw it and spin it at the same time. You don't have to study physics to know that.
 
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  • #32
PeroK said:
Have you never played or watched any sport?

In particular, if you go to "Highland Games" in Scotland, you'll find a contest called "tossing the caber", where a tree trunk is projected with both linear and rotational motion. Look on YouTube.

You seem to be unable to relate physics to the real world. If you went out into the street and gave someone a ball, they could throw it and spin it at the same time. You don't have to study physics to know that.
No. That's not what I meant. I am doubtful in the independence of both types of motion. I am trying an experiment but I don't know how can I apply constant force each time. Plus when I apply force offcenter the body deflects from the original path.
 
  • #33
mark2142 said:
No. That's not what I meant. I am doubtful in the independence of both types of motion. I am trying an experiment but I don't know how can I apply constant force each time. Plus when I apply force offcenter the body deflects from the original path.
What does "independence" mean in this context?

In practice, a force applied over time to a rotating body may tend to vary in direction. Unless you carefully control the direction of the force.
 
  • #34
PeroK said:
What does "independence" mean in this context?
Means no effect of rotation on translational motion in case of a rigid body.
 
  • #35
No one has said that they are independent in the sense you are trying to prove. They can often be separated for convenience of thought and calculation. In general if one imparts some force to a free body (and conversely a la Newton a free body imparts an opposite force on you) this will couple to both rotational and translational degrees of freedom in a complicated fashion. After the interaction the the two motions are independent for a rigid body. That is why the Center of Mass is useful (and for gravity too)
 
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  • #36
mark2142 said:
I am trying an experiment but I don't know how can I apply constant force each time.
Possibly it is time to actually learn the math. It is not like ##\sum F_\text{ext} = m_\text{tot} a_\text{cm}## is terribly difficult.

Then you can do a thought experiment. Consider a bar-bell type object. A thin and nearly massless rod connecting two massive balls that are small compared to the length of the rod.

Apply (on paper) a small force on the right-hand ball for a small time.
Consider the resulting motion of the assembly. How fast does the center of mass move? In what direction does the center of mass move?
 
  • #37
One should also be careful, which external force you consider. All you discuss here is about the motion in the homogeneous gravitational field close to Earth.

To that end consider the body under consideration (it can be an elastic or rigid solid body or even a fluid) as a discrete set of point particles, held together by interaction forces, which can be described as "pair forces", i.e., on the particle with the label ##j## the total force is given by
$$\vec{F}_j=\sum_{k \neq j} \vec{F}_{jk} + m_j \vec{g},$$
where ##\vec{g}## is the constant gravitational acceleration on due to the Earth (an approximation valid for motions close to Earth). The equations of motion for the particles thus read
$$m_j \ddot{\vec{x}}_j = \sum_{k \neq j} \vec{F}_{jk} + m_j \vec{g}.$$
Now we sum this equation over ##j## and use Newton's Third Law ("lex tertia"), according to which ##\vec{F}_{jk}=-\vec{F}_{kj}##, i.e., if the interaction force on particle ##j## due to the presence of particle ##k## is ##\vec{F}_{jk}## then the interaction force on particle ##k## due to the presence of particle ##j## is opposite. This means that by summing over ##j## all the interaction forces cancel and you get
$$\sum_j m_j \ddot{\vec{x}}_j=M \ddot{\vec{x}}_{\text{cm}} =M \vec{g},$$
where
$$M=\sum_j m_j, \quad \vec{x}_{\text{cm}}=\frac{1}{M} \sum_j m_j \vec{x}_j.$$
Our calculation shows that indeed the center of mass moves like a point particle in the gravitational field of the Earth,
$$\ddot{\vec{x}}_{\text{cm}}=\vec{g}=\text{const}.$$
For all other forces, and even the gravitational interaction with the Earth when considering the position dependence, is not as simple, because then you have (treating the Earth as a "point particle" sitting fixed at the origin of the coordinate frame),
$$m \ddot{\vec{x}}_j = \sum_{k \neq j} \vec{F}_{jk} -\gamma m_j m_{\text{Earth}} \frac{\vec{x}_j}{r_j^3} \quad \text{with} \quad r_j=|\vec{x}_j|.$$
Then summing over ##j## gives
$$M \ddot{\vec{x}}_{\text{cm}} = -\gamma m_{\text{Earth}} \sum_j \frac{m_j \vec{x}_j}{r_j^3}=\vec{F}_{\text{ext}},$$
and ##\vec{F}_{\text{ext}}## cannot be expressed in terms of ##\vec{x}_{\text{cm}}##!
 
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  • #38
jbriggs444 said:
If you look at the pencil tip where the force is applied, you can see that because the pencil both translates and rotates that the pencil tip moves farther than it would under either effect alone. So the work done and the kinetic energy gained will be greater than it would be under either effect alone. A force with the same magnitude can have greater effect because it acts over a greater distance.
jbriggs444 said:
We need more energy. We do not need more force.
jbriggs444 said:
But if we apply the force to the end of the pencil, the same force will be applied to a point on the pencil that moves for a greater distance. That means that the same magnitude of force can do a greater amount of work. It also means that we will have to put more effort into pushing the pencil on its end to maintain the same magnitude of force.
jbriggs444 said:
Intuitively, it is easier to push hard on a bowling ball than it is to push hard on a golf ball. The golf ball moves away fast when you push on it hard. It is difficult to keep up.
jbriggs444 said:
Both bowling ball and golf ball get the same momentum. But the golf ball gets 100 times more energy.
I think I got you. Its because its difficult to keep up at the end of a pencil(less mass) than at COM(more mass) when applying the force on its end that we are unable to provide it same momentum. We are unable to apply force for the required time. That's is why my glass cone on water experiment is failing. It is not covering the same distance when applying force off center.
Similarly the work done also becomes less since force is applied for lesser distance and so reduced KE for rotating object. Difficult to do. Yes?
 

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  • #39
It takes time to connect the dots. Thank you guys @hutchphd @jbriggs444 and everyone else. That was some new and interesting information not given in a book.
 
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