Resistance Moment: What is the Polar Variation?

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SUMMARY

The discussion centers on the concept of "resistance moment," denoted as "W," in statics and mechanics, specifically its polar variation. The resistance moment for a circle is defined as W_x = W_y = π/32 d³, while the polar variation is W_z = π/16 d³. This polar moment of inertia, I_z, is calculated as the sum of the moments of inertia about the X and Y axes, indicating resistance to torsional deformation. The area moment of inertia is emphasized as distinct from mass moment of inertia.

PREREQUISITES
  • Understanding of statics and mechanics principles
  • Familiarity with moment of inertia concepts
  • Knowledge of area moment of inertia calculations
  • Basic mathematical skills for integration
NEXT STEPS
  • Study the derivation of area moment of inertia formulas
  • Learn about torsional deformation in mechanical structures
  • Explore applications of polar moment of inertia in engineering
  • Investigate the differences between area moment of inertia and mass moment of inertia
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Mechanical engineers, structural analysts, and students studying statics and mechanics will benefit from this discussion, particularly those focusing on resistance to deformation in materials.

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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
W_x=W_y=\frac{\pi}{32}d^3
What I don't understand is that there is also talk about a "polar" variation of this, which for the circle is
W_x=W_y=\frac{\pi}{16}d^3
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:

I_x = \int y^2 da and

I_y = \int x^2 da. 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:

I_z = I_x + I_y = \Int (x^2 + y^2) da

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

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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