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9.5 · Calculate and interpret the product of inertia for an area

Learn to calculate and interpret the product of inertia for an area through clear examples and targeted practice.

University of Alberta ENGG 130: Engineering Mechanics: Statics

Second Moments of Area

Calculate and interpret the signed area integral about specified axes

The product of inertia is an area property that measures how area is distributed relative to two perpendicular axes at the same time. A small patch contributes according to the product of its signed coordinates. Patches in different quadrants can therefore add or cancel. Unlike a second moment of area, which squares one coordinate, this quantity can be positive, negative, or zero. Its value depends on the axes, so a result is incomplete unless those axes are stated. This lesson develops the definition, sign rules, symmetry checks, component addition, and a basic rotation calculation.

What you will learn

  • Define the product of inertia for an area about two specified perpendicular axes.
  • Calculate it by integration or by adding contributions from simple components.
  • Interpret its sign using the area’s position relative to the axes.
  • Explain why changing the axes can change the value.

1. Definition, coordinates, and units

Consider a flat region in the xyxy-plane. Choose perpendicular axes, with positive xx to the right and positive yy upward. A small area patch dAdA at coordinates (x,y)(x,y) contributes xy dA. Integrating over the entire region gives the product of inertia about these axes.
The coordinates are signed. In the first and third quadrants, xyxy is positive; in the second and fourth quadrants, xyxy is negative. Thus, the total depends on the balance of positive and negative contributions. The area element is always positive.
If coordinates are measured in metres, the product has units of m4\mathrm{m^4}: the coordinate product contributes two powers of length and area contributes two more. With millimetres, the units are mm4\mathrm{mm^4}. This is an area property, not a force or a moment of a force.
Ixy=∫Axy dAI_{xy}=\int_A xy\,dA
  • Use signed coordinates in the integrand.
  • The sign depends on both coordinates and on the selected axes.
  • Report the axes and use units of length to the fourth power.

2. Symmetry and component addition

Symmetry can establish a zero value without integration. If the area is symmetric about the selected xx-axis, every patch at (x,y)(x,y) has a matching patch at (x,−y)(x,-y). Their coordinate products have equal magnitudes and opposite signs, so they cancel. Symmetry about the selected yy-axis works in the same way. Symmetry about some other line does not by itself guarantee a zero value for the chosen axes.
For a composite area, split the region into simple, non-overlapping pieces. For each piece, use its product of inertia about centroidal axes parallel to the reference axes, its area, and its centroid coordinates measured from the reference axes. Add the translated contributions. For a rectangle whose sides are parallel to the axes, the centroidal product is zero because it is symmetric about each of its centroidal axes.
A useful calculation sketch shows the area boundary, the positive axis directions, and the dimensions or centroid locations used. Keep one common reference-axis pair throughout the component sum.
Ixy=∑i(Ix′y′,i+Aixˉiyˉi)I_{xy}=\sum_i\left(I_{x'y',i}+A_i\bar{x}_i\bar{y}_i\right)
  • Symmetry about either selected axis makes the product zero.
  • Use non-overlapping pieces and common reference axes.
  • An axis-aligned rectangle has zero product about its centroidal axes.

3. Axis orientation and interpretation

The same area can have different products of inertia for different axis orientations. Let perpendicular axes u,vu,v pass through the same point as x,yx,y. Rotate the positive uu-axis counterclockwise by angle θ\theta from the positive xx-axis. The coordinate relations are x=ucos⁡θ−vsin⁡θx=u\cos\theta-v\sin\theta and y=usin⁡θ+vcos⁡θy=u\sin\theta+v\cos\theta. Multiplying them and integrating gives a way to calculate the product in the xyxy axes from integrals in the uvuv axes.
For an area symmetric about both uu and vv, the integral of uvuv is zero. The remaining terms depend on the difference between the integrals of u2u^2 and v2v^2. For example, a rectangle aligned with its centroidal side axes has zero product in those axes, but rotating the axes can give a nonzero value if the side lengths differ.
A positive result means the positive coordinate-product contributions outweigh the negative ones for the stated axes; a negative result means the reverse. Neither sign is an intrinsic label for the area. State the axis location and orientation whenever reporting the value.
Ixy=sin⁡θcos⁡θ(∫Au2 dA−∫Av2 dA)I_{xy}=\sin\theta\cos\theta\left(\int_Au^2\,dA-\int_Av^2\,dA\right)
  • Changing axis orientation can change the value or sign.
  • Define the rotation direction before using a rotation relation.
  • Interpret the sign as the net of signed area contributions.

4. A reliable calculation routine

First identify the complete area and the two perpendicular axes. Set positive directions and check whether symmetry settles the result. If it does not, choose a direct integral or divide the area into simple pieces. For an integral, describe the limits so every point is included once. For a component sum, measure each centroid from the same reference axes.
After calculating, check the sign against the area’s locations, check that the units are length to the fourth power, and name the axes. These checks do not replace the calculation, but they often reveal a mistaken sign, omitted offset, or unit conversion.
  • Define the axes before calculating.
  • Use signed coordinates or signed centroid locations consistently.
  • Check sign, units, and axis description.

Worked example

A right triangle about its legs

A right-triangular area has vertices (0,0)(0,0), (b,0)(b,0), and (0,h)(0,h). Find its product of inertia about the two legs, which lie on the positive xx- and yy-axes.
  1. Describe the region
    Use vertical strips. At each xx from zero to bb, the upper boundary decreases linearly from height hh to zero. This gives limits that cover the triangle exactly once.
    0≤x≤b,0≤y≤h(1−xb)0\le x\le b,\qquad 0\le y\le h\left(1-\frac{x}{b}\right)
  2. Integrate the coordinate product
    Every point is in the first quadrant, so each patch contributes positively. Integrate xyxy over the vertical strip and then over the base.
    Ixy=∫0b∫0h(1−x/b)xy dy dx=b2h224I_{xy}=\int_0^b\int_0^{h(1-x/b)}xy\,dy\,dx=\frac{b^2h^2}{24}
  3. Check sign and units
    The positive result agrees with xy>0xy>0 throughout the region. Since both dimensions are lengths, the result has four powers of length.
    [Ixy]=L4[I_{xy}]=L^4
Answer: About the two legs, Ixy=b2h224I_{xy}=\frac{b^2h^2}{24}.
Check: The integrand is positive throughout the triangle, and the result has units of length to the fourth power.

Worked example

An L-shaped area from two rectangles

An L-shaped area consists of a horizontal rectangle spanning 0≤x≤40\le x\le4 and 0≤y≤10\le y\le1, and a vertical rectangle spanning 0≤x≤10\le x\le1 and 1≤y≤41\le y\le4. Find IxyI_{xy} about the bottom and left edges, using metres.
  1. Find each centroid
    The horizontal rectangle has area 4 m24\,\mathrm{m^2} and centroid (2,0.5) m(2,0.5)\,\mathrm{m}. The vertical rectangle has area 3 m23\,\mathrm{m^2} and centroid (0.5,2.5) m(0.5,2.5)\,\mathrm{m}. Their centroidal products are zero because each rectangle is aligned with the axes and symmetric about its centroidal axes.
    A1=4 m2,(xˉ1,yˉ1)=(2,0.5) m;A2=3 m2,(xˉ2,yˉ2)=(0.5,2.5) mA_1=4\,\mathrm{m^2},\quad(\bar{x}_1,\bar{y}_1)=(2,0.5)\,\mathrm{m};\quad A_2=3\,\mathrm{m^2},\quad(\bar{x}_2,\bar{y}_2)=(0.5,2.5)\,\mathrm{m}
  2. Translate and add
    For each rectangle, use its area times the product of its centroid coordinates. Both contributions are positive because both centroid coordinates are positive.
    Ixy=4(2)(0.5)+3(0.5)(2.5)=7.75 m4I_{xy}=4(2)(0.5)+3(0.5)(2.5)=7.75\,\mathrm{m^4}
  3. Interpret the total
    The entire area lies in the first quadrant relative to the stated corner axes, so all patches have positive coordinate products. The result has the expected units.
    Ixy>0I_{xy}>0
Answer: About the bottom and left edges, Ixy=7.75 m4I_{xy}=7.75\,\mathrm{m^4}.
Check: The component contributions are 4 m44\,\mathrm{m^4} and 3.75 m43.75\,\mathrm{m^4}, which add to 7.75 m47.75\,\mathrm{m^4}.

Worked example

A centred rectangle with rotated axes

A rectangle has side lengths a=120 mma=120\,\mathrm{mm} along uu and b=60 mmb=60\,\mathrm{mm} along vv, with its centre at the origin. Find IxyI_{xy} when the positive uu-axis is rotated 30∘30^\circ counterclockwise from the positive xx-axis.
  1. Use the side-aligned axes
    The rectangle is symmetric about both centroidal side axes, so its product in the u,vu,v axes is zero. Direct integration of the squared coordinates gives the two integrals needed in the rotation relation.
    ∫Au2 dA=ba312,∫Av2 dA=ab312\int_Au^2\,dA=\frac{ba^3}{12},\qquad \int_Av^2\,dA=\frac{ab^3}{12}
  2. Apply the rotation relation
    For the specified counterclockwise rotation, the integral involving u2u^2 is larger because the side along uu is longer. Substitution gives a positive product for the stated x,yx,y axes.
    Ixy=sin⁡30∘cos⁡30∘(ba312−ab312)=2.81×106 mm4I_{xy}=\sin30^\circ\cos30^\circ\left(\frac{ba^3}{12}-\frac{ab^3}{12}\right)=2.81\times10^6\,\mathrm{mm^4}
  3. Check the scale
    Both integrals have units of length to the fourth power, and the trigonometric factor is dimensionless. The reported units are therefore consistent.
    [Ixy]=mm4[I_{xy}]=\mathrm{mm^4}
Answer: For the specified axes, Ixy≈2.81×106 mm4I_{xy}\approx2.81\times10^6\,\mathrm{mm^4}.
Check: The squared-coordinate integrals are 8.64×106 mm48.64\times10^6\,\mathrm{mm^4} and 2.16×106 mm42.16\times10^6\,\mathrm{mm^4}. Their difference times sin⁡30∘cos⁡30∘\sin30^\circ\cos30^\circ gives approximately 2.81×106 mm42.81\times10^6\,\mathrm{mm^4}.

Common mistakes and how to avoid them

Using x2x^2 or y2y^2 instead of xyxy.
Correction: The product of inertia uses both signed coordinates. Squared coordinates describe different area integrals.
Assuming the answer must be positive.
Correction: Patches in the second and fourth quadrants contribute negatively.
Adding only the component centroidal products.
Correction: Translate each component to the common reference axes by including its area and centroid offset.
Assuming any symmetry makes the product zero.
Correction: For the chosen axes, symmetry about either selected coordinate axis guarantees cancellation; symmetry about another line alone does not.
Giving a product value without identifying the axes.
Correction: State the axes’ location and orientation because the value depends on them.

Lesson summary

  • The product of inertia is Ixy=∫Axy dAI_{xy}=\int_Axy\,dA about specified perpendicular axes.
  • Signed coordinates determine whether each area patch contributes positively or negatively.
  • Symmetry about either selected axis makes the product zero for that axis pair.
  • For composite areas, add centroidal products and centroid-offset contributions about common axes.
  • Rotating the axes can change the value and its sign; the units are length to the fourth power.

Check your understanding

Question 1

An area is symmetric about the selected xx-axis. What is its product of inertia about the selected x,yx,y axes?
  1. Ixy=0I_{xy}=0
  2. IxyI_{xy} must be positive
  3. IxyI_{xy} must be negative
  4. It depends on the area’s thickness
Show answer and explanation
Ixy=0I_{xy}=0
Each patch above the xx-axis has a matching patch below it with the opposite yy coordinate, so their contributions cancel.

Question 2

A small patch is located at x<0x<0 and y>0y>0. What is the sign of its contribution to IxyI_{xy}?
  1. Positive
  2. Negative
  3. Zero
  4. It depends only on the patch area
Show answer and explanation
Negative
The coordinate product is negative, and the area patch is positive, so its contribution is negative.

Question 3

What are the units of IxyI_{xy} when coordinates are measured in millimetres?
  1. mm2\mathrm{mm^2}
  2. mm3\mathrm{mm^3}
  3. mm4\mathrm{mm^4}
  4. N mm2\mathrm{N\,mm^2}
Show answer and explanation
mm4\mathrm{mm^4}
The coordinate product contributes two powers of length, and the area element contributes two more.

Key terms

Product of inertia
An area property found by integrating the product of signed coordinates over a plane area about specified perpendicular axes.
Centroidal axes
Axes that pass through the area’s centroid; their orientation must also be stated.
Composite area
An area divided into simpler, non-overlapping pieces for calculation.
Coordinate rotation
A change in axis orientation that changes the coordinates used in the area integral.

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