Polar Moment of Inertia Calculator
Calculate the polar second moment of area for solid circular, hollow circular, and rectangular cross-sections.
About polar moment of inertia
Polar moment examples
The same formulas apply at any consistent length scale.
| Cross-section | Polar moment | Use |
|---|---|---|
| Solid circle, diameter 0.10 m | 9.817 × 10⁻⁶ m⁴ | Centroidal polar moment for a solid round shaft. |
| Hollow circle, outer 0.10 m, inner 0.05 m | 9.204 × 10⁻⁶ m⁴ | Removing central material causes a relatively small reduction. |
| Rectangle, width 0.10 m, height 0.20 m | 8.333 × 10⁻⁵ m⁴ | This is Ix plus Iy, not the rectangle's torsional constant. |
How to use the calculator
- Select Solid Circle, Hollow Circle, or Rectangle.
- Measure the required cross-section dimensions and convert them to metres.
- Enter diameter values for circles or width and height for a rectangle.
- Select Calculate J and interpret the result according to the selected shape.
Polar moment of inertia FAQ
What units does polar moment of inertia use?
It uses length to the fourth power, such as m⁴ or mm⁴. The calculator expects metres and therefore displays m⁴.
Is polar moment of inertia the same as mass moment of inertia?
No, polar area moment depends only on cross-sectional geometry and uses length-to-the-fourth units. Mass moment of inertia describes rotational mass distribution and includes mass units.
Why are hollow shafts efficient?
Material far from the axis contributes strongly because diameter appears to the fourth power. Removing lightly contributing central material can reduce mass without a proportional loss of circular-shaft torsional stiffness.
Can I use the rectangle result in the circular shaft twist formula?
Not directly in general, because a rectangle warps and its Saint-Venant torsional constant differs from its polar area moment. Use a noncircular torsion formula for twist and stress.
Which axis does this calculator use?
It uses the centroidal axis perpendicular to the cross-section. Results about another point require the parallel-axis theorem before summing the planar moments.