Moment of Inertia: A Fundamental Property of Rotating Objects

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The discussion revolves around the concept of moment of inertia, a fundamental property of rotating objects, and its relationship to angular acceleration and torque. Participants express curiosity about the definition and implications of moment of inertia in physics.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the definition of moment of inertia, its role in equations relating torque and angular acceleration, and its comparison to mass in linear motion. Some question the general applicability of certain equations involving moment of inertia.

Discussion Status

There is an active exchange of ideas regarding the definition and implications of moment of inertia. Some participants provide insights into its mathematical relationships, while others raise concerns about the limitations of these relationships in broader contexts.

Contextual Notes

Participants are navigating the complexities of moment of inertia, including its derivation and the conditions under which certain equations apply. There is an acknowledgment of the potential confusion surrounding its application in different scenarios.

benoconnell22
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What is "moment of inertia?"

Just curious and I use it a lot but I am not entirely sure what it is. Call me an idiot but I need to know before my physics endeavors proceed.
 
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benoconnell22 said:
Just curious and I use it a lot but I am not entirely sure what it is. Call me an idiot but I need to know before my physics endeavors proceed.

It is resistance of a rigid body to angular acceleration (M=Iα), just like mass is resistance to linear acceleration (F=ma).

It is derived from F=ma. If you look at a rigid body rotating around its center of gravity, you can say each piece of the body has mass dm and experiences a force dF=Ap dm, where Ap = the total acceleration of that piece of the body. Because it is a rigid body, Ap = Ag + rω2apg + rα aT where Ag is the total acceleration of the center of gravity and the other components are angular acceleration and centripetal force since the only acceleration a piece of the rigid body can experience wrt to another piece is a rotation. If you then sum the moment of all those dF in the body around the centre of gravity, you end up with M=Iα. I can be a complicated thing so I've left out some inconvenient details.
 
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A torque, [itex]\tau[/itex], is needed to change the angular velocity of a rotating or stationary object. The effect of the torque on the body is measured by the rate of change of its angular velocity, [itex]\alpha[/itex], or its angular acceleration. These two are directly propotional:
[itex]\alpha\propto\tau[/itex] just like its linear equivalent a[itex]\propto[/itex]F, but this is hindered by its rotational inertia, I, or moment of inertia. So [itex]\alpha\propto\frac{1}{I}[/itex] just like a[itex]\propto\frac{1}{m}[/itex]. The moment of inertia quantifies rotational inertia in rotational motion - similar to how mass quantifies inertia in linear motion.
 


tiny-tim said:
moment of inertia is just the ratio between angular momentum and angular velocity (L = Iω)
Correct.
and between torque and angular acceleration (τ = Iα)
This is incorrect in general. It is valid only in very special cases. High school and freshman physics classes typically address just those special cases where τ = Iα is valid, but they steer clear of the general case where this equation is invalid.
 

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