Calculating moments of inertia
Key idea: Find moment of inertia by integrating r² over mass about a stated axis. The parallel-axis theorem shifts a centre-of-mass value by Md²; composite parts must use the same axis.
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Guided lessons · coming soon
Guided lesson
Guided steps
- Predict how equal-width ring masses change with radius.
- Choose mass elements whose points share one distance from the axis.
- Follow the rod integral about its centre.
- Follow the integral with numbers.
- Integrate on paper, then enter the end-axis coefficient as a decimal.
- Explain the mass element and derive the disc’s inertia on paper.
- Check which axis the parallel-axis theorem starts from.
- Shift the disc’s central result to a rim axis.
- Find the rod’s end-axis inertia and show your method.
- Find the centre-of-mass inertia, then shift to the new axis.
- Read how to add parts about the same axis.
- Add the centre-of-mass inertias, then shift using the whole mass.
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ContinueFor a body made of point masses, I = ∑ mᵢrᵢ². A continuous body is made of infinitely many small mass elements, so the sum becomes an integral:
where r is the perpendicular distance of the element dm from the axis. The work is in choosing dm so that every part of it is at the same distance from the axis.
Choose a mass element
Check your understanding 1 Predict first
A uniform disc is cut into thin rings of equal radial width. How does the mass of a ring near the rim compare with the mass of a ring near the centre?
Show answer
More mass. A thin ring of radius r and width dr has area 2π r dr, so at twice the radius it holds twice the mass. That is why a disc cannot be treated as a rod along its radius.
Choosing a mass element
For a uniform thin rod of mass M and length L, the linear density is λ = M/L. A short element has dm = λ dx.
For a uniform thin disc of mass M and radius R, the surface density is σ = M/(π R²). A thin annulus of radius r and radial width dr has area dA = 2π r dr, so dm = 2π rσ dr. The annulus gets heavier as r increases because its circumference increases. Equal radial widths do not contain equal masses.
Illustrative numerical equivalents
The diagrams use schematic widths. These values describe uniform model bodies, not experimental measurements.
| Body and axes | Density | Moment of inertia |
|---|---|---|
| Rod: M = 3 kg, L = 2 m; perpendicular axes | λ = 1.5 kg m⁻¹ | COM: 1.0 kg m²; end: 4.0 kg m² |
| Disc: M = 2 kg, R = 1 m; symmetry axis | σ = 0.637 kg m⁻² | 1.0 kg m² |
For each integral, identify the perpendicular distance, express dm using the correct density, and integrate over the whole body. The limits and the density must describe the same object.
Uniform thin rod about its centre
Choose the axis through the centre and perpendicular to the rod. Put x = 0 at the centre, so -L/2 ≤ x ≤ L/2 and the perpendicular distance is |x|:
Negative coordinates still give positive contributions because the distance is squared.
Worked example 1
Integrating a uniform rod
Problem
Show full solution
Choose the element and limits
Method
dm = 0.50 dx in SI units, with x from -0.60 to + 0.60 m.Reason
The mass is uniform along the rod and the axis passes through its midpoint.Working
Answer
λ = M/L = 0.60/1.2 = 0.50 kg m⁻¹Integrate
Method
I = 0.072 kg m².Reason
Each element contributes x²dm.Working
Answer
I = 0.50∫_(-0.60)^(0.60)x² dx = 0.072 kg m²
Quick check
Check your understanding 2 Derive the end-axis result
On paper, integrate I = ∫ x²λ dx for a uniform rod of mass M and length L about a perpendicular axis through one end, with x from 0 to L. Enter the coefficient of ML² as a decimal; keep the derivation on paper.
Show answer
Compare your limits and density: the element runs over the whole rod from the axis, so the distance is x itself. The result is four times I_cm, because more of the mass is far from the axis.
Uniform disc about its central axis
Every point of an annulus is the same distance r from the disc’s central axis, so the annulus is the right element for a disc. Treating the disc as if its mass were spread evenly along a radius gives the wrong answer.
Spot the mistake 2
A disc is not a rod in the radial direction
Learner claim
A learner models a uniform disc with dm = (M/R)dr and obtains I = MR²/3. Explain why that mass element is wrong and derive the correct central-axis inertia on paper. Compare your reasoning and integral with the solution.
Try this before viewing the solution
Show solution step by step
Use annular area
Method
dm = 2π rσ dr, with σ = M/(π R²).
Reason
A disc has uniform mass per area, rather than per radial distance.
Working
Answer
dA = 2π r drIntegrate the inertia
Method
I = (1/2)MR².Reason
The distance of each annulus from the symmetry axis is r.
Working
Answer
I = 2πσ∫₀^R r³ dr = (1/2)MR²
Common mistake
Check the geometry of dm before integrating. The incorrect model puts too much mass near the centre and therefore gives too small an inertia.
The parallel-axis theorem
The parallel-axis theorem is I = I_cm + Md². Here I_cm refers to a parallel axis through the centre of mass of the whole object, and d is the perpendicular separation of the axes. It does not let you add Md² to an arbitrary non-centroidal inertia.
For the rod’s end axis, d = L/2: I_end = (1/12)ML² + M(L/2)² = (1/3)ML². Within a set of parallel axes, the COM axis gives the smallest inertia because Md² ≥ 0. This comparison keeps the axis direction fixed.
Guided practice 3
A disc about a parallel axis through its rim
Problem
Find a uniform thin disc’s inertia about an axis through a point on its rim and perpendicular to its plane.
Try this before viewing the solution
Hints
Hint 1
identify the centre axis result
Which central-axis result do you need, and how far apart are the two parallel axes?
Show solution step by step
Set the reference
Method
I_cm = (1/2)MR² and d = R.Reason
The rim axis is parallel to and one radius from the symmetry axis.
Working
Answer
I = I_cm + Md²Combine
Method
I = (3/2)MR².Reason
Add the parallel-axis shift MR².Working
Answer
I = (1/2)MR² + MR² = (3/2)MR²
Quick check
Moving to a parallel non-centroidal axis increases the inertia.
Exam-style question 1
A rod rotating about its end
Examination question
Try this before viewing the solution
Show the steps Optional working
Show solution step by step
Find the COM result
1 markMethod
I_cm = 1.0 kg m².Reason
The reference axis passes through the rod’s midpoint.Working
Answer
(3.0)(2.0)²/12 = 1.0Set the separation
1 markMethod
d = 1.0 m.Reason
The end axis is half a rod length from the parallel COM axis.Working
Answer
d = L/2Apply the theorem
1 markMethod
I_end = 4.0 kg m².Reason
Use the full rod mass in the shift term.Working
Answer
I = 1.0 + (3.0)(1.0)² = 4.0 kg m²
Self-mark with the mark scheme
Tick each mark point that your answer includes.
Mark your full written answer against these points.
Check your understanding 3 Can you shift from any parallel axis?
A uniform rod has mass 1.2 kg, length 1.0 m and end-axis inertia 0.40 kg m². A parallel axis lies 0.25 m from its COM. A learner calculates its inertia as 0.40 + 1.2(0.25)². Find the centre-of-mass inertia and the correct inertia, and identify the error. All axes are perpendicular to the rod.
Show the steps Optional working
Show the steps Optional working
Show answer
First recover the COM-axis inertia: I_cm = 0.40-1.2(0.50)² = 0.10 kg m². Then I = 0.10 + 1.2(0.25)² = 0.175 kg m², or 0.18 kg m² to two significant figures. The learner used the end-axis inertia as though it were the COM-axis reference, counting the old shift as well as the new one.
Composite bodies
To find the moment of inertia of a body made of several parts, find each part’s moment of inertia about the same axis and add them. If the parts’ inertias are easier to find about the centre of mass of the whole body, add them about that axis first and then shift the total, using the whole body’s mass.
Always state the axis in full. A disc’s central axis is its symmetry axis, perpendicular to its faces; the rod axes in this lesson are perpendicular to the rod.
Try it yourself 4
Shift the axis of a whole composite body
Problem
Try this before viewing the solution
Show the steps Optional working
Show the steps Optional working
Hints
Hint 1
locate the whole-body COM
Equal end masses preserve symmetry about the midpoint.Show solution step by step
Add inertias about the COM
Method
I_cm = 0.225 kg m² before rounding.Reason
The rod and both masses use the same midpoint axis.Working
Answer
I_cm = 1.2(1.0)²/12 + 2(0.25)(0.50)² = 0.225Shift the whole object
Method
I_end = 0.65 kg m².Reason
The total mass is 1.70 kg and the axis separation is 0.50 m.Working
Answer
I = 0.225 + (1.70)(0.50)² = 0.650 kg m²
Quick check
You will not need the perpendicular-axis theorem or the derivation of a sphere’s moment of inertia. When a question involves a sphere, it gives the moment of inertia and its axis.
Common mistakes
- Using dm = (M/R) dr for a disc. A disc has uniform mass per area, so use the annulus dm = 2π rσ dr.
- Integrating over only half of a rod, or using limits that do not match the density.
- Adding Md² to a moment of inertia that is not about the centre-of-mass axis.
- Using one part’s mass instead of the whole body’s mass in the shift term.
- Adding inertias that are about different axes.
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Syllabus and review details
- GCE A-Level H3 Physics 2027 · 2027
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