HiIf the moment of inertia exist to resist a body to change from its

In summary, the conversation discusses the concept of inertia and how it applies to a point mass on a rotating body. It is mentioned that a point mass exhibits both linear and rotational inertia at the same time. The participants also touch on the idea of fictitious centrifugal force and the relationship between spin and linear momentum. It is ultimately concluded that inertia can manifest in different ways depending on the system and parameters involved.
  • #1
Red_CCF
532
0
Hi

If the moment of inertia exist to resist a body to change from its rotational motion and linear inertia exists to resist a body's change from its linear motion, then for a point mass on a rotating body, which inertia does it obey?

Thanks.
 
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  • #2


Both, of course. Mass exhibits both linear and rotational aspects of inertia at the same time.
 
  • #3


Doc Al said:
Both, of course. Mass exhibits both linear and rotational aspects of inertia at the same time.

But how can it satisfy linear inertia if it wants to satisfy rotational inertia and vice versa; like how can it want to go both straight and in a circle at the same time?
 
  • #4


Red_CCF said:
But how can it satisfy linear inertia if it wants to satisfy rotational inertia and vice versa; like how can it want to go both straight and in a circle at the same time?
I don't understand what you mean. The same object has both linear and rotational inertia at the same time. It's not either or.

Perhaps you can give a specific example?
 
  • #5


I don't know if DocAl meant that a point mass has rotational inertia about its own axis and can thus spin and translate at the same time.

But the thing to remember is that there are two 'components' to inertia. Viz the resistance to change of the body itself and the nature of the forcing or changing agent.

We can calculate a moment of inertia about any axis we choose, but it does not mean there is an agent acting to cause rotation about this axis. Similarly we can calculate a linear inertia (mass) in any direction we choose ( they are usually the same in all directions) but there is only an effect if there is a force acting in that direction.
 
  • #6


I can't help wondering whether or not Red is confused regarding rotation vs. revolution.
 
  • #7


Studiot said:
I don't know if DocAl meant that a point mass has rotational inertia about its own axis and can thus spin and translate at the same time.
That's not what I meant. The rotational inertia of a point mass about its own axis would be zero. But a point mass can certainly have rotational inertia about some other axis.
 
  • #8


Doc Al said:
That's not what I meant. The rotational inertia of a point mass about its own axis would be zero. But a point mass can certainly have rotational inertia about some other axis.

I think I figured out what I was confused about. I was thinking that for a particle rotating about an axis, to satisfy its inertia in rotational motion would mean that it couldn't satisfy its inertia in linear motion since its velocity would be changing directions.

I think it arises from my (poor) understanding of fictitious centrifugal force as the linear inertia resists the change in velocity but yet a particle has an rotational inertia.
 
  • #9


One interpretation of inertia is a measure of the energy required to stop a body doing whatever it is doing.

A particle that is spinning, but not translating, has more energy, by virtue of its spin, than a similar one that is also not spinning.

It would take energy to stop the spin. Do you not count this as a manifestation of inertia?
 
  • #10


Red_CCF said:
I think I figured out what I was confused about. I was thinking that for a particle rotating about an axis, to satisfy its inertia in rotational motion would mean that it couldn't satisfy its inertia in linear motion since its velocity would be changing directions.

I think it arises from my (poor) understanding of fictitious centrifugal force as the linear inertia resists the change in velocity but yet a particle has an rotational inertia.
The particle rotating about an axis is behaving just as you'd expect: It's linear momentum is changing since the object it's attached to is exerting a centripetal force on it.
 
  • #11


Another thing to keep in mind, now that the parameters have been defined, is that "spin" is a physicist's expression for a particle property that does not involve "spinning" as in the sense of a top or curveball. By the same token, you can't say that a particular quark is "charming", although "charm" is one of its characteristics.
 
  • #12


'spin' is also used by children playing with tops, cricket and tennis players - USW
 
  • #13


Well, it gets into weird stuff like I3, which I believe is properly referred to as "the vertical component of isotopic spin". WTF?!
 

1. What is the definition of moment of inertia?

The moment of inertia is a physical property of a body that describes how resistant it is to rotational motion about a given axis.

2. How is moment of inertia different from mass?

Moment of inertia measures the distribution of mass in a body, while mass is a measure of the amount of matter in a body.

3. What factors affect the moment of inertia of a body?

The moment of inertia is affected by the mass and shape of a body, as well as the axis of rotation.

4. How is moment of inertia calculated?

The moment of inertia is calculated by multiplying the mass of each particle in a body by the square of its distance from the axis of rotation, and then summing these values for all particles in the body.

5. Why does moment of inertia exist?

Moment of inertia exists to resist a body from changing its rotational motion. It is an important property that helps us understand and predict the behavior of rotating objects.

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