INGENIA

CIV-08

Parallel-axis (Steiner) theorem

I = Icm + A d² about a parallel axis.

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Section propertiesHuygens–SteinerEN 1993-1-1

Governing equation

I=Icm+Ad2I = I_{\mathrm{cm}} + A d^2

d∈[0,800]d \in \left[0, 800\right]

where

b
Width (mm)
h
Height (mm)
d
Offset of axis (mm)
I_{\mathrm{cm}}
Centroidal I (cm⁴)
I
I about axis (cm⁴)

The figure, part by part

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CIV-08 · beam
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①

Governing law — red

I=Icm+Ad2I = I_{\mathrm{cm}} + A d^2

d∈[0,800]d \in \left[0, 800\right]

d=0d = 0Icm=1.07×105I_{\mathrm{cm}} = 1.07\times 10^{5}

②

Domain of the variable — blue

dmin⁡=0,dmax⁡=800d_{\min} = 0,\quad d_{\max} = 800

d∈[0,800]d \in \left[0, 800\right]

d=0d = 0d=0d = 0

③

Response curve — green

I=Icm+Ad2I = I_{\mathrm{cm}} + A d^2

d∈[0,800]d \in \left[0, 800\right]

d=0d = 0Icm=1.07×105I_{\mathrm{cm}} = 1.07\times 10^{5}

④

Rate of change — amber

dIcmdd\frac{\mathrm{d}I_{\mathrm{cm}}}{\mathrm{d}d}

d∈[0,800]d \in \left[0, 800\right]

d=5.031d = 5.031Icm′=80.5I_{\mathrm{cm}}^{\prime} = 80.5

Lecture brief

Historical brief

From Euler’s 1744 elastica and Navier’s beam theory to Mohr’s circle and transformed-section RC, structural mechanics grew as a closed-form craft before finite elements. The lab keeps those governing lines for buckling, flexure, joints and influence. This sheet (CIV-08 — Parallel-axis (Steiner) theorem) is the form associated with Huygens–Steiner · EN 1993-1-1. Working symbols: bb, hh, dd →\rightarrow IcmI_{\mathrm{cm}}, II. Shifting the origin of the second-moment integral by d adds the Steiner term A d²; it is the workhorse of composite-section design.

Purpose

Purpose: compute IcmI_{\mathrm{cm}}, II from bb, hh, dd in Structural & civil via I=Icm+Ad2I = I_{\mathrm{cm}} + A d^2 I = Icm + A d² about a parallel axis. Use it when a real structural & civil question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given b=200.000 mmb = 200.000\,\mathrm{mm}, h=400.000 mmh = 400.000\,\mathrm{mm}, d=250.000 mmd = 250.000\,\mathrm{mm}, the governing relation I=Icm+Ad2I = I_{\mathrm{cm}} + A d^2 yields Icm=106666.667 cm4I_{\mathrm{cm}} = 106666.667\,\mathrm{cm⁴}, I=606666.667 cm4I = 606666.667\,\mathrm{cm⁴}. One rectangle shifted from its centroid. Units mm. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Centroidal I I_{\mathrm{cm}}106666.667 cm⁴
  • I about axis I606666.667 cm⁴
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CIV-08 · beam
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Narration of this film

One rectangle shifted from its centroid. Units mm.

Shifting the origin of the second-moment integral by d adds the Steiner term A d²; it is the workhorse of composite-section design.

Reading speed

Watch on YouTube