Moment of Inertia Calculator

Select a cross-section shape (Rectangle, Circle, Triangle, I-Beam, Hollow Rectangle, or Annulus), enter its dimensions, and get the second moment of area (Ix, Iy), section modulus, and centroid — all the key geometric properties structural engineers rely on.

Select the shape of the cross-section you want to analyse.

mm

Outer width of the section (used for Rectangle, Hollow Rectangle, Triangle, I-Beam flange).

mm

Outer height of the section (used for Rectangle, Hollow Rectangle, Triangle, I-Beam).

mm

Inner void width — for Hollow Rectangle only.

mm

Inner void height — for Hollow Rectangle only.

mm

Outer radius — for Circle and Annulus.

mm

Inner radius — for Annulus only.

mm

Top/bottom flange width — for I-Beam only.

mm

Thickness of each flange — for I-Beam only.

mm

Thickness of the web — for I-Beam only.

Results

Moment of Inertia Ix (about x-axis)

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Moment of Inertia Iy (about y-axis)

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Section Modulus Sx

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Section Modulus Sy

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Centroid ȳ (from bottom)

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Cross-Sectional Area

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Section Properties Overview

Frequently Asked Questions

What is the area moment of inertia (second moment of area)?

The area moment of inertia — also called the second moment of area — is a purely geometric property that describes how a cross-section's area is distributed relative to a given axis. It has units of length to the fourth power (e.g. mm⁴ or m⁴) and is widely used in structural and mechanical engineering to predict how a beam will resist bending and deflection.

What is the difference between Ix and Iy?

Ix is the second moment of area about the horizontal centroidal x-axis, and Iy is the second moment of area about the vertical centroidal y-axis. Ix governs bending resistance in the vertical plane (the most common loading direction for beams), while Iy governs resistance to lateral bending.

How do I calculate the moment of inertia of a rectangle?

For a solid rectangle of width b and height h, Ix = (b × h³) / 12 and Iy = (h × b³) / 12, both measured about the centroidal axes. The centroid lies at h/2 from the bottom and b/2 from the side. These are among the most commonly used formulas in structural engineering.

How do I calculate the moment of inertia about any axis using the parallel axis theorem?

The parallel axis theorem states that I = I_c + A × d², where I_c is the moment of inertia about the centroidal axis, A is the cross-sectional area, and d is the perpendicular distance between the centroidal axis and the new axis. This allows you to combine individual shapes into composite sections.

How do I find the moment of inertia of a composite (built-up) shape?

Divide the composite shape into simple sub-shapes (rectangles, circles, etc.) whose individual moments of inertia are known. Find the centroid of the whole section, then apply the parallel axis theorem to shift each sub-shape's Ix or Iy to the overall centroidal axis, and sum them all up. Subtract the inertia of any void or hole regions.

What is the section modulus and why does it matter?

The section modulus S = I / y_max, where y_max is the distance from the centroid to the extreme fibre. It directly relates bending moment to bending stress via σ = M / S. A larger section modulus means the cross-section can carry higher bending moments before reaching the material's allowable stress.

What is the moment of inertia of a circle with radius r?

For a solid circle of radius r, Ix = Iy = π × r⁴ / 4. For a hollow circular annulus with outer radius r and inner radius r_i, Ix = Iy = π × (r⁴ − r_i⁴) / 4. Circular sections are commonly used for columns, shafts, and pipes where bending may occur in any direction.

What are typical engineering applications of the moment of inertia?

Engineers use the second moment of area to design beams, columns, floor joists, and structural members so they resist bending without excessive stress or deflection. It is also essential when selecting standard steel sections (I-beams, channels, hollow sections) from design tables, and when verifying compliance with structural codes such as Eurocode 3 or AISC.

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