Moment of Inertia of an I-Beam

Formula and worked example in mm and inches

An I-beam puts most of its area in the flanges, as far from the neutral axis as possible. That gives a high moment of inertia for little steel, which is why it is the standard shape for steel beams.

Formula

Worked example (millimetres)

Given

  • Flange width b_f = 200 mm
  • Flange thickness t_f = 15 mm
  • Web thickness t_w = 10 mm
  • Overall depth h = 400 mm

Steps

  1. Clear web height: h_w = h − 2t_f = 400 − 2 × 15 = 370 mm.
  2. Closed form: Iₓ = (b_f × h³ − (b_f − t_w) × h_w³) / 12 = (200 × 400³ − 190 × 370³) / 12 = 264,660,833 mm⁴ (26,466.1 cm⁴).
  3. Check by parallel axis — each flange: b_f × t_f³ / 12 + b_f × t_f × d², with d = (h − t_f) / 2 = 192.5 mm, gives 111,225,000 mm⁴.
  4. Web: t_w × h_w³ / 12 = 42,210,833 mm⁴. Total: 2 × 111,225,000 + 42,210,833 = 264,660,833 mm⁴, the same answer.
  5. Section modulus: Zₓ = Iₓ / (h/2) = 1,323,304 mm³; radius of gyration rₓ = √(Iₓ / A) = 165.2 mm.
Section properties for the mm example
Area, A9,700 mm²
Moment of inertia, Iₓ264,660,833 mm⁴
Section modulus, Zₓ1,323,304 mm³
Radius of gyration, rₓ165.2 mm

Worked example (inches)

Given

  • Flange width b_f = 8 in
  • Flange thickness t_f = 0.5 in
  • Web thickness t_w = 0.3 in
  • Overall depth h = 12 in

Steps

  1. Clear web height: h_w = h − 2t_f = 12 − 2 × 0.5 = 11 in.
  2. Closed form: Iₓ = (b_f × h³ − (b_f − t_w) × h_w³) / 12 = (8 × 12³ − 7.7 × 11³) / 12 = 297.9 in⁴.
  3. Check by parallel axis — each flange: b_f × t_f³ / 12 + b_f × t_f × d², with d = (h − t_f) / 2 = 5.75 in, gives 132.3 in⁴.
  4. Web: t_w × h_w³ / 12 = 33.28 in⁴. Total: 2 × 132.3 + 33.28 = 297.9 in⁴, the same answer.
  5. Section modulus: Zₓ = Iₓ / (h/2) = 49.66 in³; radius of gyration rₓ = √(Iₓ / A) = 5.13 in.
Section properties for the in example
Area, A11.3 in²
Moment of inertia, Iₓ297.9 in⁴
Section modulus, Zₓ49.66 in³
Radius of gyration, rₓ5.13 in

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Frequently asked questions

How do you calculate the moment of inertia of an I-beam?
Treat it as the outer rectangle b_f × h minus the two empty rectangles beside the web: Iₓ = (b_f × h³ − (b_f − t_w) × h_w³) / 12, where h_w = h − 2t_f. The parallel-axis theorem on the two flanges and the web gives the same result.
Why does an I-beam have a high moment of inertia?
Moment of inertia weights each bit of area by the square of its distance from the axis. The flanges sit at the top and bottom, so they contribute most of Iₓ while the thin web adds little weight.
Does this match the values in steel section tables?
Closely, but tabulated rolled sections include the fillet radii where web meets flange, so their Iₓ is slightly higher than this idealised plate calculation.

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