Moment of Inertia Calculator
Area moment of inertia (Iₓ, I_y), centroid, section modulus and radius of gyration for 9 cross-sections — rectangles, circles, I-beams, T/L sections and standard AISC W-shapes.
Section properties
Iₓ — strong axis
I_y — weak axis
Area (A)
Polar moment (J = Iₓ + I_y)
Section modulus Sₓ
Section modulus S_y
Radius of gyration rₓ
Radius of gyration r_y
Centroid location (from base / corner)
Strong vs weak axis: Iₓ is bending about the horizontal axis (vertical beam orientation); I_y is bending about the vertical axis. For asymmetric T and L sections the centroid is offset from the geometric centre — use the parallel-axis theorem when transforming to a different axis.
Why moment of inertia matters in structural design
The area moment of inertia (I) is the geometric property that quantifies how the cross-section resists bending. A larger I means less deflection under load, less bending stress at the extreme fiber, and a higher critical buckling load.
A 2×8 floor joist has Iₓ ≈ 47.6 in⁴ (strong axis, on edge) vs 5.4 in⁴ on the flat — 9× stiffer simply by orienting the cross-section to put material away from the neutral axis. This is why beams are tall and narrow, and why I-beams are dramatically more efficient than rectangular bars of the same area.
Section modulus and radius of gyration
Section modulus S = I / c where c is the distance from the centroid to the extreme fiber. Allowable bending moment is M = S × Fb, so S is what you compare against the design moment in a flexural check.
Radius of gyration r = √(I / A) is the effective radius at which the area could be concentrated to give the same moment of inertia. Slenderness ratio (KL / r) determines buckling capacity of compression members.
Cross-section formulas
| Shape | Iₓ | A |
|---|---|---|
| Solid Rectangle (b × h) | b·h³ / 12 | b·h |
| Hollow Rectangle (B,H outer; b,h inner) | (B·H³ − b·h³) / 12 | B·H − b·h |
| Solid Circle (Ø D) | π·D⁴ / 64 | π·D² / 4 |
| Hollow Circle (D outer, d inner) | π·(D⁴ − d⁴) / 64 | π·(D² − d²) / 4 |
| I-Beam | (bf·H³ − (bf−tw)·hw³) / 12 | 2·bf·tf + hw·tw |
| Triangle (b base, h height) | b·h³ / 36 (centroid) | b·h / 2 |
T and L sections require first computing the centroid, then applying the parallel-axis theorem to each rectangular sub-part — the calculator does this automatically.
Worked examples
Solid Rectangle 4 × 8 in (strong axis vertical)
- Iₓ = (4 × 8³) / 12 = 170.67 in⁴
- I_y = (8 × 4³) / 12 = 42.67 in⁴
- A = 4 × 8 = 32 in²
- Iₓ / I_y = 4× — meaningful but not as dramatic as an I-beam
Solid Circle Ø 4 in
- I = π × 4⁴ / 64 = 12.566 in⁴
- A = π × 4² / 4 = 12.566 in²
- r = √(12.566 / 12.566) = 1.0 in
- Iₓ = I_y by symmetry; J = 2·I = 25.13 in⁴
AISC W8×10 (lookup)
- A = 2.96 in²
- Iₓ = 30.8 in⁴ (strong axis)
- I_y = 2.09 in⁴ (weak axis)
- Sₓ = 7.81 in³
- Iₓ / I_y ≈ 15× — the value of the I-beam shape