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Study Guide: AP Physics – Moment of Inertia and Rotational Kinetic Energy
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AP Physics – Moment of Inertia and Rotational Kinetic Energy

By Fatskills Exam Guides Team — the exam nerds behind 28,500+ quizzes and 2.1M practice questions across 500+ global exams.

⏱️ ~6 min read

AP Physics – Moment of Inertia and Rotational Kinetic Energy

AP Physics: Moment of Inertia & Rotational Kinetic Energy – Exam-Ready Study Guide


What This Is

Moment of inertia (I) measures an object’s resistance to rotational motion—just like mass resists linear motion. Rotational kinetic energy (K_rot) is the energy an object has due to its rotation. These concepts are critical on the AP Physics exam because they appear in problems involving rolling objects, angular momentum, and energy conservation. Real-world example: A figure skater pulls their arms in to spin faster—this works because reducing their moment of inertia increases their angular velocity (conservation of angular momentum). Without understanding I and K_rot, you can’t explain why!


Key Terms & Concepts

  • Moment of Inertia (I): Resistance to rotational motion; depends on mass distribution relative to the axis of rotation. Units: kg·m².
  • Formula: I = ?m?r?² (for point masses) or I = ?r² dm (for continuous objects).
  • Key idea: More mass farther from the axis-larger I-harder to rotate.

  • Rotational Kinetic Energy (K_rot): Energy due to rotation.

  • Formula: K_rot = ½I?², where ? = angular velocity (rad/s).

  • Parallel Axis Theorem: If you know I about an axis through the center of mass (I_cm), you can find I about a parallel axis.

  • Formula: I = I_cm + Md², where M = total mass, d = distance between axes.

  • Common Moments of Inertia (memorize these!):

  • Point mass at distance r: I = mr²
  • Solid cylinder/disk (axis through center): I = ½mr²
  • Hollow cylinder (axis through center): I = mr²
  • Solid sphere (axis through center): I = ?mr²
  • Thin rod (axis through center): I = ?mL²
  • Thin rod (axis through end): I = mL²

  • Torque (?): Rotational equivalent of force; causes angular acceleration.

  • Formula: ? = I?, where ? = angular acceleration (rad/s²).

  • Work-Energy Theorem (Rotational): Work done by torque changes rotational kinetic energy.

  • Formula: W = ?K_rot = ½I?_f²-½I?_i²

  • Rolling Without Slipping: A special case where v_cm = r? (linear speed = radius × angular speed).

  • Total kinetic energy: K_total = K_trans + K_rot = ½mv² + ½I?²

  • Angular Momentum (L): Rotational equivalent of linear momentum.

  • Formula: L = I? (for rigid bodies).

  • Conservation of Angular Momentum: If net external torque = 0, L is conserved.

  • Example: Skater spins faster when arms are pulled in (?I-??).

Step-by-Step / Process Flow

How to Solve Moment of Inertia & Rotational Energy Problems

  1. Identify the axis of rotation – Is it through the center of mass, an end, or another point? This determines which I formula to use.
  2. Determine if energy is conserved – If no non-conservative forces (e.g., friction) do work, use K_i + U_i = K_f + U_f, including K_rot if the object is rotating.
  3. For rolling objects, relate v and ? – Use v_cm = r? for rolling without slipping.
  4. Apply torque or energy equations
  5. If torque is involved: ? = I? or W = (work = torque × angular displacement).
  6. If energy is involved: K_rot = ½I?² or K_total = ½mv² + ½I?².
  7. Check unitsI must be in kg·m², ? in rad/s, and ? in rad/s².

Example Problem: A solid sphere (mass m, radius r) rolls down a ramp from rest. What is its speed at the bottom?
1. Energy conservation: mgh = ½mv² + ½I?²
2. For a solid sphere: I = ?mr²
3. Rolling without slipping: v = r?-? = v/r
4. Substitute: mgh = ½mv² + ½(?mr²)(v²/r²) = ½mv² + ?mv² = ?mv²
5. Solve for v: v = ?(10gh/7)


Common Mistakes

  • Mistake: Forgetting that I depends on the axis of rotation.
  • Correction: Always specify the axis! A rod’s I is different if rotated about its center vs. its end.

  • Mistake: Using K = ½mv² for rolling objects without adding K_rot.

  • Correction: Rolling objects have both translational and rotational kinetic energy. Use K_total = ½mv² + ½I?².

  • Mistake: Confusing ? (angular velocity) with v (linear velocity).

  • Correction: ? is in rad/s, v is in m/s. For rolling without slipping, v = r?.

  • Mistake: Applying ? = I? when torque isn’t constant.

  • Correction: ? = I? only works for constant torque. For variable torque, use energy methods.

  • Mistake: Misapplying the parallel axis theorem.

  • Correction: The theorem only works for parallel axes. If the axis isn’t parallel, you can’t use it!

AP Exam Insights

  • Frequently tested:
  • Calculating I for point masses or standard shapes (disks, rods, spheres).
  • Energy conservation problems with rolling objects (e.g., spheres, cylinders, hoops).
  • Comparing speeds of different objects rolling down a ramp (e.g., hoop vs. solid sphere).

  • Tricky distinctions:

  • Moment of inertia vs. mass: I depends on mass distribution, not just total mass.
  • Rolling with slipping vs. without slipping: If slipping occurs, v-r? and energy isn’t conserved (friction does work).
  • Torque vs. work: Torque (? = rF sin?) causes rotation; work (W = ) changes rotational energy.

  • FRQ traps:

  • Not including K_rot in energy problems (e.g., forgetting a rolling object has both K_trans and K_rot).
  • Mixing up I formulas (e.g., using I = mr² for a solid sphere instead of I = ?mr²).
  • Forgetting to convert degrees to radians (AP always uses radians for ? and ?).

  • Multiple-choice traps:

  • Questions where two objects have the same mass but different I (e.g., a hoop and a disk).
  • Problems where an object is both translating and rotating (e.g., a yo-yo unwinding).

Quick Check Questions

1. Multiple Choice

A hollow cylinder and a solid cylinder of the same mass and radius roll down an incline without slipping. Which reaches the bottom first? (A) The hollow cylinder (B) The solid cylinder (C) They arrive at the same time (D) Not enough information

Answer: (B) The solid cylinder. Explanation: The solid cylinder has a smaller I (½mr² vs. mr²), so more of its energy goes into translational motion, giving it a higher speed.


2. Free-Response (Short)

A thin rod of mass M and length L is pivoted at one end. What is its moment of inertia about this pivot?

Answer: I = ML² Explanation: For a thin rod rotated about its end, the moment of inertia is I = ML² (memorize this!).


3. Multiple Choice

A figure skater with arms extended has a moment of inertia I and angular velocity ?. When she pulls her arms in, her moment of inertia decreases to I/2. What is her new angular velocity? (A) ?/2 (B) ? (C) 2? (D) 4?

Answer: (C) 2? Explanation: Angular momentum is conserved (L = I?), so if I halves, ? must double to keep L constant.


Last-Minute Cram Sheet

  1. Moment of inertia (I) = resistance to rotation; depends on mass and distribution.
  2. Rotational KE = ½I?² (like ½mv² but for rotation).
  3. Parallel axis theorem: I = I_cm + Md² (only for parallel axes!).
  4. Rolling without slipping: v = r? (linear speed = radius × angular speed).
  5. Total KE for rolling objects: K = ½mv² + ½I?².
  6. Solid sphere I: I = ?mr² (axis through center).
  7. Hollow cylinder I: I = mr² (axis through center).
  8. Thin rod I (center): I = ?mL²; (end): I = mL².
  9. Energy conservation: Include K_rot for rolling objects!
  10. Units: I = kg·m², ? = rad/s, ? = rad/s².