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Area Moment of Inertia — Formulas, Units & Cross-Section Reference

Area moment of inertia (also called the second moment of area) is the geometric quantity that determines a beam\'s resistance to bending. This page lists the closed-form formulas for circle, rectangle, I-beam, T-beam, and pipe sections, gives the parallel-axis theorem for composite shapes, summarises the units in use (in⁴, mm⁴, m⁴), and walks through a worked beam example using AISC W-shape data. Reviewed by a licensed PE.

AREA MOMENT OF INERTIA · DEFINITION x y dA y x arbitrary cross-section A integrate DEFINITION Iₓ = ∫ y²·dA Iᵧ = ∫ x²·dA units: length⁴ Stiffness in bending grows with the SQUARE of distance from the bending axis
Figure 1 — Definition: each differential area element dA contributes y²·dA to the moment of inertia; integrate over the section.

Area moment inertia calculator

For built-up cross-sections (assemblies of rectangles, I-shapes, plates, and round bars) the composite-centroid / inertia calculator computes I_x, I_y, J, and the centroid coordinates for any combination. For single primitive shapes (circle, rectangle, I-beam, pipe) the dedicated moment-of-inertia tool covers the closed-form formulas. Both calculators include the parallel-axis correction automatically.

→ Open the composite centroid & inertia calculator  ·  → Open the single-shape inertia calculator

Area moment of inertia formulas

Eq. 01 — Definition (general integral) SI
Ix=Ay2dA,Iy=Ax2dAI_x = \int_A y^2 \, dA, \qquad I_y = \int_A x^2 \, dA
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I_x, I_y = second moments about the x- and y- axes (length⁴)
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dA = differential area element
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y, x = perpendicular distance from the corresponding axis to dA
Eq. 02 — Solid circle (diameter D) SI
I=πD464I = \frac{\pi D^4}{64}
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I = area moment of inertia about any centroidal axis
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D = diameter
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Same value for every centroidal axis (rotational symmetry)
Eq. 03 — Rectangle (b × h, centroidal axis) SI
Ix=bh312,Iy=hb312I_x = \frac{b h^3}{12}, \qquad I_y = \frac{h b^3}{12}
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b = width, h = height (h is measured along the bending axis)
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For a square b = h, both axes give I = b⁴/12
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About the base, not centroid: I = bh³/3
Eq. 04 — I-beam (B × H outer, b × h inner cavity) SI
Ix=BH3bh312I_x = \frac{B H^3 - b h^3}{12}
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B = full flange width; H = full depth
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b = (B − web thickness); h = clear web height between flanges
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Subtraction works because both rectangles share the centroidal axis
Eq. 05 — Hollow tube / pipe (outer D, inner d) SI
I=π(D4d4)64I = \frac{\pi (D^4 - d^4)}{64}
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D = outside diameter, d = inside diameter
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Subtract the inner solid I from the outer solid I
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Closed-section torsion uses the polar form J = π(D⁴ − d⁴)/32
Eq. 06 — Parallel-axis theorem (Huygens) SI
I=Icentroid+Ad2I = I_{centroid} + A \cdot d^2
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I_centroid = inertia of sub-area about its own centroid
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A = sub-area
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d = perpendicular distance from sub-area centroid to the composite neutral axis

Standards and authoritative sources

Standard / sourceScope
AISC Steel Construction Manual (16th ed.)Part 1 lists I_x, I_y, S, Z, r for every US W-, S-, HP-, HSS-, C-, MC-, L-shape (in⁴ units)
AISC 360-22Specification for structural steel buildings — uses I in flexural strength (Chapter F) and deflection checks (Chapter L)
EN 10365 / Eurocode product tablesEuropean IPE, HEA, HEB, UPN section properties in mm⁴
ANSI/AWC NDS-2018National Design Specification for Wood Construction — moment of inertia tables for sawn lumber and engineered wood
ASCE 7-22Loading standard whose deflection limits (L/360, L/240) consume the I value
ISO 80000-3SI units and quantities — defines moment of inertia symbols and units

Reference: I_x for common cross-sections

ShapeDimensionsI_x (in⁴)I_x (mm⁴ ×10⁶)
Solid circleD = 4 in (100 mm)12.574.91
Hollow pipe (Sched 40)4 in NPS (D = 4.5, t = 0.237)7.233.01
Solid square4 × 4 in (100 × 100 mm)21.338.33
HSS rectangularHSS 6 × 4 × 1/420.98.70
W-shape (steel I)W12×2620484.9
W-shape (steel I)W18×35510212
W-shape (steel I)W24×621 550645
IPE (Eurocode)IPE 30019883.6
Wood joist (NDS)2 × 12 (1.5 × 11.25 in)177.9874.1
  1. Identify the cross-section shape and axis Pick the shape (circle, rectangle, I-beam, T-beam, pipe) and the bending axis (usually the strong axis x–x for beams). For composite sections, list each rectangular sub-shape and its centroid offset from the overall neutral axis.
  2. Apply the closed-form formula For a solid circle of diameter D: I = πD⁴ / 64. For a rectangle b × h: I = bh³/12 about the centroidal axis. For an I-beam: I = (B·H³ − b·h³) / 12 where B,H are outer flange/depth and b,h are the open web cavity. Pull from the section table for standard W-, HSS-, IPE-shapes.
  3. Add parallel-axis correction for off-centroid pieces Huygens' parallel-axis theorem: I = I_centroid + A · d², where d is the distance from each sub-area's own centroid to the composite section's neutral axis. Apply once per sub-piece, then sum. Without this step composite sections are systematically under-strength.
  4. Convert units if needed I has units of length⁴ — in⁴ (US), mm⁴ (metric SI), m⁴ (large structures). Conversions: 1 in⁴ = 416 231 mm⁴ = 4.162 × 10⁻⁷ m⁴. The AISC manual lists I in in⁴; Eurocode tables in mm⁴.
  5. Check against bending stress Compute σ = M·c / I, where M is the bending moment, c is the distance from neutral axis to extreme fiber. The whole point of computing I is so this stress check works. If σ exceeds Fy/Ω (ASD) or φFy (LRFD), the section is undersized.

Worked example — built-up T-beam

Compute I_x for a built-up T-beam: top flange 6 in × 1 in plate, web 1 in × 8 in plate. The T is symmetric left-right but not top-bottom; you must first locate the centroid before applying the inertia formulas.

  1. Sub-areas: A₁ (flange) = 6 × 1 = 6 in²; A₂ (web) = 1 × 8 = 8 in². Total A = 14 in².
  2. Centroid from the top fibre: ȳ = (6 × 0.5 + 8 × 5.0) / 14 = 3.07 in.
  3. Centroidal I of each rectangle: I₁ = 6·1³/12 = 0.5 in⁴; I₂ = 1·8³/12 = 42.7 in⁴.
  4. Distances to overall neutral axis: d₁ = 3.07 − 0.5 = 2.57 in; d₂ = 5.0 − 3.07 = 1.93 in.
  5. Parallel-axis additions: 6·2.57² = 39.6 in⁴; 8·1.93² = 29.8 in⁴.
  6. Total I_x: 0.5 + 42.7 + 39.6 + 29.8 = 112.6 in⁴.

The same answer drops out of the composite-centroid calculator in two clicks — but doing it by hand once is the only way to internalise why the parallel-axis correction matters.

Area moment of inertia vs. mass moment of inertia vs. polar moment

PropertySymbolUnitsUsed for
Area moment of inertiaI, I_x, I_ylength⁴ (in⁴, mm⁴)Bending stress / deflection of beams
Polar (are