Math 2.0

Mechanics of deformable solids Definition

Second moment of area

Builds on Centroid

Definition

Let A⊂ℝ2A \subset \R^2 be a bounded measurable region in the (y,z)(y, z)-plane. The second moments of area of AA about the zz-axis and the yy-axis are Iz=∫Ay2 dA,Iy=∫Az2 dA.I_z = \int_A y^2 \, dA, \qquad I_y = \int_A z^2 \, dA. The product moment of area is Iyz=∫Ayz dAI_{yz} = \int_A y z \, dA, and the polar moment of area about the origin is J=∫A(y2+z2) dA=Iy+IzJ = \int_A (y^2 + z^2) \, dA = I_y + I_z. In beam theory the axes pass through the centroid of the cross-section.

Remarks

Example: for the rectangle ∣y∣≤h/2\abs{y} \le h/2, ∣z∣≤b/2\abs{z} \le b/2, the moment about the centroidal zz-axis is Iz=∫−h/2h/2y2b dy=bh3/12I_z = \int_{-h/2}^{h/2} y^2 b \, dy = bh^3/12. For a disc of radius RR centred at the origin, Iy=Iz=πR4/4I_y = I_z = \pi R^4/4 and J=πR4/2J = \pi R^4/2.

Non-example: the integral ∫Ay dA\int_A y \, dA is the first moment of area; it is 00 about a centroidal axis, so it does not measure resistance to bending.

Let IcI_c be the moment about a centroidal axis and ∣A∣\abs{A} the area. The parallel axis theorem gives I=Ic+d2∣A∣I = I_c + d^2 \abs{A} for a parallel axis at distance dd. The symbol II is used both for this quantity and for the mass moment of inertia, which has the mass density in the integral.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Second_moment_of_area
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DefinesSecond moment of area
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Changed3 November 2026

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