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

Click For Summary
A body behaves as a point mass when a force is applied, as its center of mass (COM) accelerates according to Newton's laws. When no external force is acting (F_ext = 0), the COM remains at rest or moves at a constant speed, effectively allowing it to be treated as a point mass for certain calculations. However, if the body experiences rotational motion due to off-center forces, this complicates the scenario, as rotational dynamics must also be considered. While the translational motion of the COM can be analyzed independently, the effects of rotation and deformation cannot be ignored in practical applications. Overall, a body can be treated as a point mass in specific contexts, but its rotational behavior introduces additional complexities.
  • #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.
 
Physics news on Phys.org
  • #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)
 
  • Like
Likes PeroK and jbriggs444
  • #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}}##!
 
  • Like
Likes Delta2
  • #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?
 

Attachments

  • rrr.png
    rrr.png
    5.1 KB · Views: 125
  • Like
Likes hutchphd and jbriggs444
  • #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.
 
  • Like
Likes vanhees71, jbriggs444, Delta2 and 1 other person

Similar threads

Replies
7
Views
2K
  • · Replies 15 ·
Replies
15
Views
3K
  • · Replies 25 ·
Replies
25
Views
1K
  • · Replies 10 ·
Replies
10
Views
2K
Replies
17
Views
2K
Replies
5
Views
2K
Replies
8
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K