Rotational Motion – Stage 1 (Page 7)
Parallel Axis Theorem & Perpendicular Axis Theorem
Often, moment of inertia is required about an axis that does not pass through the center of mass. To handle such cases easily, we use axis theorems.
1. Parallel Axis Theorem
The moment of inertia of a body about any axis is equal to the moment of inertia about a parallel axis passing through the center of mass plus M d².
I = Icm + M d²
where
Icm = M.I. about center of mass
M = mass of body
d = distance between axes
2. Conditions for Applying Parallel Axis Theorem
✔ Axes must be parallel
✔ One axis must pass through center of mass
✔ Body must be rigid
3. Example (Very Common in Exams)
Moment of inertia of a rod about one end:
Iend = Icm + M(L/2)²
= ML²/12 + ML²/4
= ML²/3
4. Perpendicular Axis Theorem
For a planar lamina, the moment of inertia about an axis perpendicular to the plane is equal to the sum of the moments of inertia about two perpendicular axes in the plane.
Iz = Ix + Iy
5. Conditions for Perpendicular Axis Theorem
✔ Applicable only to planar bodies
✔ All three axes must pass through same point
✔ Axes must be mutually perpendicular
6. Why These Theorems Are Powerful
✔ Convert difficult axis problems into easy ones
✔ Avoid lengthy integration
✔ Save time in competitive exams
⚠ Common Student Mistakes
❌ Using perpendicular axis theorem for 3D bodies ❌ Forgetting d² term in parallel axis theorem ❌ Confusing axes directions
IIT-JEE Insight
IIT problems often combine both theorems. Recognizing which theorem applies first is the key skill.
Next: Stage 1 – Page 8
Rotational Kinetic Energy & Work–Energy Theorem
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