1st, 2nd and mass moment of inertia

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SUMMARY

The discussion focuses on the concepts of the first and second moments of area and mass moment of inertia, emphasizing their applications in predicting resistance to shear stress and bending. The first moment of area (Qx, Qy) is used to determine shear stress resistance, while the second moment of area (Ixx, Iyy, Ixy) assesses bending resistance. The inertia tensor is introduced as a means to understand the distribution of mass in relation to rotational motion and deformation. Clarifications on terminology and formulas are sought to enhance conceptual understanding.

PREREQUISITES
  • Understanding of basic mechanics principles
  • Familiarity with calculus for integration
  • Knowledge of tensor mathematics
  • Concept of shear stress and bending moments
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  • Study the derivation of the first moment of area and its applications in structural engineering
  • Learn about the inertia tensor and its role in rotational dynamics
  • Explore the relationship between moments of area and mass in mechanical systems
  • Investigate advanced topics in elasticity and stress analysis
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Mechanical engineers, structural analysts, and students studying mechanics who seek to deepen their understanding of moments of area and inertia in physical systems.

gravity121
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I know most of the formula's but I'm trying to get a conceptual understanding of everything and finding it very hard to get concise information about everything all in one place especially when there are so many names for the same thing. Most resources just rehash the formulas without explaining what's going on. Please help. I'm looking for the physical understanding of what's going on and clarity on the formulas. Please fill in and correct any mistakes below or confirm if I'm understanding correctly. Thank you

1st moment of area - used to predict resistance to shear stress

Qx - area distribution around x-axis and resistance to shear stress about x-axis? = int yda
Qy - area distribution around y-axis and resistance to shear stress about x-axis? = int xda
Qz - area distribution around z-axis and resistance to shear stress about z-axis? = ?
is this the polar ist moment of area, is there such a thing? Is this correct??
Is there a product 1st area moment? If so, what is it for? = ?

2nd moment of area - a cross sectional resitance to bending
Ixx - resistance to bending about x-axis due moment about x-axis = int y^2 da
Iyy - resistance to bending about y-axis due to moment about y-axis = int x^2 da
Ixy - resistance to bending about x-axis due to moment about y-axis (assuming moment is not applied on through the centroid or this would be zero) = int yx da
Iyx - as above
Iz - resistance to torsion (polar 2nd moment of area) = = int (x^2 + y^2 da) = Ixx + Iyy

Moment of Inertia
Ixx - resistance to rotation about x-axis due moment about x-axis = int y^2 dm
Iyy - resistance to rotation about y-axis due to moment about y-axis = int x^2 dm
Ixy - resistance to rotation about x-axis due to moment about y-axis (assuming moment is not applied on through the center of gravity or this would be zero) = int xy dm
Iyx - as above
Iz - resistance to resistance to rotation about z-axis due to moment about z-axis. Is this also called the polar moment of inertia. = int (x^2 + y^2) dm ?

Is there any other moments of something out there, like volume or whatever?
 
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gravity121 said:
I'm looking for the physical understanding of what's going on and clarity on the formulas. Please fill in and correct any mistakes below or confirm if I'm understanding correctly.

I agree, the range of terms is confusing, and my lack of TeX skills is about to make this equally confusing...

How's this- for a planar section 'S' of an object with density 'ρ', the center of mass 'M0' and first moments of area 'A1' and mass 'M1' are:
M0 = ∫ρdS, A1=∫x dS and M1 = ∫xρ dS

You have Q = A1 above.

Second moments involve tensor-valued integrands, but I'll do my best. The inertia tensor, which generates second moments A2 and M2, is:

N = ∫[(xx)I-xx]ρ dS

This will generate your second moments of area (omit the density) and moments of inertia above. I expect you could continue this to a third moment, but they don't mean anything (AFAIK). M0 corresponds to the response of a body to a force F, while A1, M1 and N relate to the response of a body to the 'moment' x×F. This 'moment' is also sometimes called a 'force couple' or 'torque':
http://physicsnet.co.uk/a-level-physics-as-a2/mechanics/moments/

Now, if you consider the stress tensor instead of forces, you have a 'stress couple', which is generally taken to be zero:
http://elibrary.matf.bg.ac.rs/bitst...ty_with_couple_stress_ToupinRA.pdf?sequence=1

Does this help?
 
It does a little but it doesn't clarify the physical understanding for me, as in what each term represents. What I wrote originally, is it correct or incorrect?
 
gravity121 said:
It does a little but it doesn't clarify the physical understanding for me, as in what each term represents. What I wrote originally, is it correct or incorrect?

Hows this- if a body's interia tells you how much mass there is, the interia tensor tells you how it is distributed in space. The inertia tensor relates to rotational motion, but also deformation (not just bending).
 
gravity121 said:
It does a little but it doesn't clarify the physical understanding for me, as in what each term represents. What I wrote originally, is it correct or incorrect?
I wonder whether there has to be a connection except in the common form of the formula.
 
Thank you but I'd really appreciate if you could confir, or correct each of the assumptions above??

Cheers
 
In statics, the second moment of area is sometimes called, confusingly, the moment of inertia.
(MOI is technically the second moment of mass.)
Similarly, the first moment of area is sometimes called the moment of mass.

First moment of area -- Used to find centroid of a plane figure, for example
Second moment of area -- A beam cross section's resistance to bending
First moment of mass -- Used to find an object's center of gravity
Second moment of mass -- Resistance to angular acceleration
 

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