Centroids of Composite Areas

The centroid of a composite area is the area-weighted average of the centroids of its parts: x̄ = ΣAᵢx̄ᵢ / ΣAᵢ and ȳ = ΣAᵢȳᵢ / ΣAᵢ. Split the shape into rectangles, triangles and circles whose centroids you know, treat holes as negative areas, and sum the table.

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What the centroid is

The centroid is the geometric centre of an area: the point where it would balance if it were cut from a thin, uniform plate. For a plate of uniform thickness and density it is also the centre of gravity. For a beam cross-section it is where the neutral axis passes in bending, which is why every bending stress and deflection calculation starts by finding it.

Any axis of symmetry contains the centroid. A shape with two axes of symmetry has its centroid where they cross, so you only need to compute the coordinate that symmetry does not give you.

The composite-area table

Set up one row per part with columns for A, x̄ᵢ, ȳᵢ, Aᵢx̄ᵢ and Aᵢȳᵢ. Measure every x̄ᵢ and ȳᵢ from the same reference axes, chosen at a corner or edge so most coordinates are positive.

From the centroid to the moment of inertia

The second moment of area about the centroidal axis uses the same table: add each part’s own I to Aᵢdᵢ², where dᵢ is the distance from the part’s centroid to the composite centroid. That is the parallel axis theorem. The moment of inertia calculator shows both steps for standard sections, so you can check a hand table against it.

Key formulas

Formulas used on this page, with the textbook each is cited from
FormulaExpressionWhereCited from
Centroid of a composite areax̄ = ΣAᵢx̄ᵢ / ΣAᵢ, ȳ = ΣAᵢȳᵢ / ΣAᵢAᵢ = area of part i (mm²), negative for holes; x̄ᵢ, ȳᵢ = coordinates of the centroid of part i from the reference axes (mm)Hibbeler, Engineering Mechanics: Statics
Centroid of a semicircleȳ = 4r / (3π)r = radius (mm); ȳ measured from the diameterBeer & Johnston, Vector Mechanics for Engineers: Statics
Parallel axis theorem (areas)I = Σ(Īᵢ + Aᵢdᵢ²)Īᵢ = second moment of part i about its own centroidal axis (mm⁴), dᵢ = distance from that axis to the composite centroidal axis (mm)Meriam & Kraige, Engineering Mechanics: Statics
Rectangle about its centroidal axisĪ = b·h³ / 12b = width parallel to the axis (mm), h = depth perpendicular to it (mm)Hibbeler, Engineering Mechanics: Statics

Worked examples

Example: Centroid and moment of inertia of a T-section

Given

  • A T-section made of a 120 mm wide × 20 mm thick flange on top of a 20 mm wide × 100 mm deep web, centred on the web. Total depth 120 mm.
  • Reference axis at the bottom of the web.

Find

  • The height of the centroid ȳ above the bottom, and the moment of inertia about the horizontal centroidal axis.

Solution

  1. The vertical axis of symmetry contains the centroid, so only ȳ is needed. Part areas and centroid heights:Web: A₁ = 20 × 100 = 2000 mm², ȳ₁ = 50 mm; Flange: A₂ = 120 × 20 = 2400 mm², ȳ₂ = 100 + 10 = 110 mm
  2. Sum the table:ΣA = 4400 mm², ΣAȳ = 2000(50) + 2400(110) = 364 000 mm³
  3. Centroid height:ȳ = 364 000 / 4400 = 82.73 mm above the bottom (37.27 mm below the top)
  4. Distances from each part’s centroid to the composite centroid:d₁ = 82.73 − 50 = 32.73 mm, d₂ = 110 − 82.73 = 27.27 mm
  5. Parallel axis theorem, part by part:Web: 20(100)³/12 + 2000(32.73)² = 1.667 × 10⁶ + 2.142 × 10⁶; Flange: 120(20)³/12 + 2400(27.27)² = 0.080 × 10⁶ + 1.785 × 10⁶
  6. Add the four terms:I = 5.674 × 10⁶ mm⁴

Answer: ȳ = 82.73 mm above the bottom of the web, on the axis of symmetry, and I = 5.67 × 10⁶ mm⁴ about the horizontal centroidal axis. The centroid sits in the web, close to the heavier flange. The bending stress lesson uses this section.

Example: A bracket plate with a triangular extension and a hole

Given

  • A plate made of a 160 mm wide × 120 mm tall rectangle with its lower-left corner at the origin.
  • A right triangle attached to its right edge: vertical leg 120 mm along x = 160 mm, base 60 mm along the bottom edge from x = 160 to 220 mm.
  • A 50 mm diameter hole centred at (60 mm, 70 mm).

Find

  • The coordinates (x̄, ȳ) of the centroid of the plate.

Solution

  1. Rectangle:A₁ = 160 × 120 = 19 200 mm², x̄₁ = 80 mm, ȳ₁ = 60 mm
  2. Triangle (centroid one third of the base from the vertical leg, one third of the height from the base):A₂ = ½ × 60 × 120 = 3600 mm², x̄₂ = 160 + 60/3 = 180 mm, ȳ₂ = 120/3 = 40 mm
  3. Hole, as a negative area:A₃ = −π(25)² = −1963.5 mm², x̄₃ = 60 mm, ȳ₃ = 70 mm
  4. Total area:ΣA = 19 200 + 3600 − 1963.5 = 20 836.5 mm²
  5. First moments:ΣAx̄ = 1 536 000 + 648 000 − 117 810 = 2 066 190 mm³; ΣAȳ = 1 152 000 + 144 000 − 137 445 = 1 158 555 mm³
  6. Divide by the total area:x̄ = 2 066 190 / 20 836.5 = 99.16 mm, ȳ = 1 158 555 / 20 836.5 = 55.60 mm

Answer: The centroid is at (99.16 mm, 55.60 mm). The triangle pulls it right of the rectangle’s centre (80 mm), and the hole, above and to the left of that centre, pulls it further right and down.

Common mistakes

In industry

Frequently asked questions

Is the centroid the same as the centre of mass?

For a plate of uniform thickness and density, yes. If density or thickness varies, weight each part by its mass instead of its area.

Can the centroid be outside the shape?

Yes. The centroid of an L-shape, a ring or a channel can fall in empty space. It is a point of balance, not necessarily a point on the material.

Why use negative areas instead of splitting around the hole?

It is much simpler. A plate with a circular hole would need curved pieces otherwise; subtracting a full circle gives the same answer.

How many decimal places should I keep?

Keep at least four significant figures in the table and round at the end. The parallel axis terms use d², so rounding the centroid early magnifies the error in I.

Keep learning

All Statics lessons · All engineering subjects

See also

Sources

  1. R. C. Hibbeler, Engineering Mechanics: Statics, Pearson
  2. F. P. Beer, E. R. Johnston, D. F. Mazurek, Vector Mechanics for Engineers: Statics, McGraw Hill
  3. J. L. Meriam, L. G. Kraige, Engineering Mechanics: Statics, Wiley

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