Resistance Moment: What is the Polar Variation?

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Discussion Overview

The discussion revolves around the concept of "resistance moment" in statics and mechanics, particularly focusing on its polar variation. Participants explore the definitions and relationships between different moments of inertia, specifically in the context of circular geometries.

Discussion Character

  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant introduces the term "resistance moment" and its notation, noting its application to circles with specific formulas for W_x and W_y.
  • Another participant suggests that the term may refer to the area moment of inertia, distinguishing it from mass moment of inertia, and provides the mathematical definitions for moments of inertia in two planes.
  • The polar moment of inertia is described as the sum of the area moments of inertia about the X and Y axes, with a specific formula provided for circular geometries.
  • Participants discuss the implications of the moment of inertia as a measure of resistance to deformation, with the polar moment specifically indicating resistance to torsional deformation.
  • A participant expresses appreciation for the clarification provided regarding the relationship between resistance moment and moment of inertia.
  • Another participant reflects on the terminology, suggesting that the term "resistance moment" might be more memorable than "moment of inertia."

Areas of Agreement / Disagreement

Participants generally agree on the relationship between resistance moment and moment of inertia, but there is no explicit consensus on the terminology or the implications of these concepts.

Contextual Notes

The discussion does not resolve the potential confusion surrounding the terminology and definitions of resistance moment versus moment of inertia, nor does it clarify the implications of these terms in different contexts.

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In norwegian we use a term in statics/mechanics which directly translated means "resistance moment". It is denoted "W" and apparently has two directions x and y, usually written as indexes. For a circle we have
[tex]W_x=W_y=\frac{\pi}{32}d^3[/tex]
What I don't understand is that there is also talk about a "polar" variation of this, which for the circle is
[tex]W_x=W_y=\frac{\pi}{16}d^3[/tex]
Could someone explain to me what this "polar" variation is all about?
 
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It looks like to me you are referring to the moment of inertia. More specifically, the area moment of inertia (not to be confused with mass moment of inertia).

In two planes, X and Y, the corresponding moments of inertia are:

[tex]I_x = \int y^2 da[/tex] and

[tex]I_y = \int x^2 da[/tex]. Both are a measure of an object's geometry about an arbitrary set of orthogonal axis.

The polar moment of inertia is the same as the others, but is (using the same reference notation) about the Z axis. It is the sum of the other two moments of inertia:

[tex]I_z = I_x + I_y = \Int (x^2 + y^2) da[/tex]

So in your case, for the disc, [tex]W_x + W_y = W_z = 2*W_x = 2* W_y = 2*\frac{\pi}{32} d^3 = \frac{\pi}{16}d^3[/tex]

In mechanics, the moment of inertia is an indication of a plate or beam's resistance to deformation due to loading. In the same sense, the polar moment of inertia is an indication of an object's resistance to torsional deformation.
 
Last edited:
Ah, excellent! Thanks FredGarvin! o:)
 
Resistance moment. I think I wouldve remembered what the moment of inertia was sooner if it was called this here.
 

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