Angular Momentum Examples in Physics

Start with the recap, study the fully worked examples, then use the practice problems to check your understanding of Angular Momentum.

This page combines explanation, solved examples, and follow-up practice so you can move from recognition to confident problem-solving in Physics.

Concept Recap

The rotational equivalent of linear momentum, measuring the quantity of rotational motion in a spinning or orbiting object.

A spinning skater pulling their arms in spins faster β€” they're conserving angular momentum.

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How to Use These Examples

  • Read the first worked example with the solution open so the structure is clear.
  • Try the practice problems before revealing each solution.
  • Use the related concepts and background knowledge badges if you feel stuck.

What to Focus On

Core idea: Angular Momentum works by defining the interacting system and comparing motion before and after the interaction.

Common stuck point: Students often know a formula related to angular momentum but skip the recognition step: Is the interaction short, collision-like, or rotational, and have I checked whether external forces or torques can be ignored? That leads to a correct-looking substitution attached to the wrong physical model.

Sense of Study hint: Ask: Is the interaction short, collision-like, or rotational, and have I checked whether external forces or torques can be ignored?

Worked Examples

Example 1

medium
A skater has I1=8 kg\cdotpm2I_1 = 8\,\text{kgΒ·m}^2, Ο‰1=1.5 rad/s\omega_1 = 1.5\,\text{rad/s}. They tuck in to I2=3 kg\cdotpm2I_2 = 3\,\text{kgΒ·m}^2. Find Ο‰2\omega_2.

Answer

Ο‰2=4Β rad/s\omega_2 = 4 \text{ rad/s}

First step

1
Conserve LL: I1Ο‰1=I2Ο‰2I_1 \omega_1 = I_2 \omega_2.

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Example 2

hard
Show that if KE is conserved when a skater pulls in their arms (II halves), then LL cannot be conserved. (Reach a contradiction.)

Practice Problems

Try these problems on your own first, then open the solution to compare your method.

Example 1

easy
A disk has moment of inertia I=4 kg\cdotpm2I = 4\,\text{kgΒ·m}^2 and spins at Ο‰=3 rad/s\omega = 3\,\text{rad/s}. Find its angular momentum.

Example 2

easy
A 2 kg mass moves at 5 m/s5\,\text{m/s} in a circle of radius 3 m3\,\text{m}. Find its angular momentum about the center.

Example 3

easy
Angular momentum L=18 kg\cdotpm2/sL = 18\,\text{kgΒ·m}^2/\text{s} and Ο‰=6 rad/s\omega = 6\,\text{rad/s}. Find the moment of inertia.

Example 4

easy
A spinning skater pulls in their arms, reducing II. What happens to their spin rate Ο‰\omega (no external torque)?

Example 5

easy
Is angular momentum a vector or a scalar?

Example 6

easy
A skater has I=2 kg\cdotpm2I = 2\,\text{kgΒ·m}^2 spinning at 4 rad/s4\,\text{rad/s}. Find their angular momentum.

Example 7

easy
If no external torque acts on a system, what happens to its total angular momentum?

Example 8

easy
A 0.5 kg ball whirls at 2 m/s2\,\text{m/s} on a string of radius 4 m4\,\text{m}. Find its angular momentum.

Example 9

medium
A skater spins at 2 rad/s2\,\text{rad/s} with I=6 kg\cdotpm2I = 6\,\text{kgΒ·m}^2, then pulls in arms to I=2 kg\cdotpm2I = 2\,\text{kgΒ·m}^2. Find the new spin rate.

Example 10

medium
A merry-go-round (I=100 kg\cdotpm2I = 100\,\text{kgΒ·m}^2) spins at 1 rad/s1\,\text{rad/s}. A child adds I=25 kg\cdotpm2I = 25\,\text{kgΒ·m}^2 by stepping on at the rim. Find the new angular speed.

Example 11

medium
A ball on a string moves at 4 m/s4\,\text{m/s} at radius 2 m2\,\text{m}. The string is pulled in to radius 1 m1\,\text{m}. Find the new speed (conserve L=mvrL = mvr).

Example 12

medium
A 3 kg point mass at r=2 mr = 2\,\text{m} rotates at Ο‰=5 rad/s\omega = 5\,\text{rad/s}. Find its angular momentum (I=mr2I = mr^2).

Example 13

medium
Two disks: one spinning (I=4 kg\cdotpm2I = 4\,\text{kgΒ·m}^2 at 6 rad/s6\,\text{rad/s}) drops onto a stationary one (I=2 kg\cdotpm2I = 2\,\text{kgΒ·m}^2); they couple. Find the common angular speed.

Example 14

medium
A planet at perihelion moves at 60 km/s60\,\text{km/s} at r=1r = 1 unit; at aphelion r=4r = 4 units. Find its aphelion speed (conserve L=mvrL = mvr).

Example 15

medium
A wheel slows from Ο‰=10 rad/s\omega = 10\,\text{rad/s} to rest in 5 s5\,\text{s} with I=2 kg\cdotpm2I = 2\,\text{kgΒ·m}^2. Find the average torque applied.

Example 16

medium
A disk with I=5 kg\cdotpm2I = 5\,\text{kgΒ·m}^2 spins at 4 rad/s4\,\text{rad/s}, then a brake changes its inertia arrangement so I=10 kg\cdotpm2I = 10\,\text{kgΒ·m}^2 (mass moved outward, no external torque). Find the new angular speed.

Example 17

medium
A 4 kg point mass moves at 3 m/s3\,\text{m/s} along a line passing 2 m2\,\text{m} from a reference point (perpendicular distance). Find its angular momentum about that point.

Example 18

challenge
A 0.5 kg bug lands on the rim of a spinning disk (I=1.5 kg\cdotpm2I = 1.5\,\text{kgΒ·m}^2, Ο‰=4 rad/s\omega = 4\,\text{rad/s}) at radius r=2 mr = 2\,\text{m}. Find the new angular speed after the bug sticks.

Example 19

challenge
A rod (I=3 kg\cdotpm2I = 3\,\text{kgΒ·m}^2) spins at Ο‰=8 rad/s\omega = 8\,\text{rad/s}. A torque of 6 N\cdotpm6\,\text{NΒ·m} opposes it. How long until it stops?

Example 20

challenge
A child (mass 30 kg30\,\text{kg}) runs at 4 m/s4\,\text{m/s} tangent to the rim of a stationary merry-go-round (I=200 kg\cdotpm2I = 200\,\text{kgΒ·m}^2, radius 2 m2\,\text{m}) and jumps on. Find the resulting angular speed.

Example 21

easy
A wheel has I=5 kg\cdotpm2I = 5\,\text{kgΒ·m}^2 and spins at Ο‰=4 rad/s\omega = 4\,\text{rad/s}. Find LL.

Example 22

easy
A 1 kg1\,\text{kg} point mass orbits at r=2 mr = 2\,\text{m} with v=3 m/sv = 3\,\text{m/s}. Find LL.

Example 23

easy
True/false: external torque is needed to change a system's angular momentum.

Example 24

easy
A hoop of mass 2 kg2\,\text{kg} and radius 0.5 m0.5\,\text{m} rolls so its center moves at Ο‰=10 rad/s\omega = 10\,\text{rad/s}. Find LspinL_{spin}. (Ihoop=MR2I_{hoop} = MR^2.)

Example 25

easy
A solid disk has I=12MR2I = \tfrac12 M R^2. For M=4 kgM = 4\,\text{kg}, R=0.5 mR = 0.5\,\text{m}, Ο‰=8 rad/s\omega = 8\,\text{rad/s}, find LL.

Example 26

easy
If Ο‰=5 rad/s\omega = 5\,\text{rad/s} and L=20 kg\cdotpm2/sL = 20\,\text{kgΒ·m}^2/\text{s}, find II.

Example 27

easy
A planet's angular momentum about the Sun is approximately conserved. True or false?

Example 28

medium
A solid disk (M=6 kgM = 6\,\text{kg}, R=0.4 mR = 0.4\,\text{m}, Ο‰=5 rad/s\omega = 5\,\text{rad/s}) is suddenly joined by a coaxial 4 kg4\,\text{kg} disk of the same radius initially at rest. Find the new Ο‰\omega.

Example 29

medium
Earth has Iβ‰ˆ8.0Γ—1037 kg\cdotpm2I \approx 8.0 \times 10^{37}\,\text{kgΒ·m}^2 and rotates at Ο‰β‰ˆ7.3Γ—10βˆ’5 rad/s\omega \approx 7.3 \times 10^{-5}\,\text{rad/s}. Estimate Earth's spin angular momentum.

Example 30

medium
A neutron star forms when a stellar core of radius 7Γ—105 km7 \times 10^5\,\text{km} collapses to 10 km10\,\text{km}, keeping MM constant (I∝R2I \propto R^2 for a uniform sphere). If it spun at one rev/month before, find its new period.

Example 31

medium
A merry-go-round of I=200 kg\cdotpm2I = 200\,\text{kgΒ·m}^2 is at rest. A 50 kg50\,\text{kg} child runs tangentially at 3 m/s3\,\text{m/s} and jumps on at radius 2 m2\,\text{m}. Find the new angular speed.

Example 32

medium
A child of mass 30 kg30\,\text{kg} stands on a I=150 kg\cdotpm2I = 150\,\text{kgΒ·m}^2 turntable spinning at Ο‰=2 rad/s\omega = 2\,\text{rad/s} at r=3 mr = 3\,\text{m}. They walk to r=1 mr = 1\,\text{m}. Find the new Ο‰\omega.

Example 33

medium
A net torque of Ο„=4 N\cdotpm\tau = 4\,\text{NΒ·m} acts on a disk for 3 s3\,\text{s}. Find the change in LL.

Example 34

medium
A flywheel of I=25 kg\cdotpm2I = 25\,\text{kgΒ·m}^2 initially at rest reaches Ο‰=40 rad/s\omega = 40\,\text{rad/s} in 10 s10\,\text{s}. Find the average torque applied.

Example 35

medium
A particle moves at constant velocity along a straight line that does NOT pass through point OO. Is its angular momentum about OO constant?

Example 36

medium
A 0.4 kg0.4\,\text{kg} puck on a frictionless air hockey table moves at 5 m/s5\,\text{m/s} along a line 2 m2\,\text{m} from the table's center. Find its angular momentum about the center.

Example 37

medium
A 200 kg200\,\text{kg} flywheel disk of radius 1 m1\,\text{m} stores L=5000 kg\cdotpm2/sL = 5000\,\text{kgΒ·m}^2/\text{s}. Find its spin rate. (I=12MR2I = \tfrac12 M R^2.)

Example 38

hard
A bullet (m=0.05 kgm = 0.05\,\text{kg}, v=400 m/sv = 400\,\text{m/s}) embeds in the rim of a stationary disk (M=5 kgM = 5\,\text{kg}, R=0.5 mR = 0.5\,\text{m}, I=12MR2I = \tfrac12 M R^2). Find the disk's angular speed after.

Example 39

hard
A rod of length L=1 mL = 1\,\text{m}, mass M=2 kgM = 2\,\text{kg}, pivots at its center. A 0.1 kg0.1\,\text{kg} clay ball at 10 m/s10\,\text{m/s} hits the rod's end and sticks. Find the angular speed after. (Irod,center=112ML2I_{rod,center} = \tfrac{1}{12}M L^2.)

Example 40

hard
A spinning bicycle wheel (LspinL_{spin} along its axle, horizontal) is held by a person on a stationary turntable. The person flips the wheel 180∘180^\circ. What is the person+turntable's final LL if their I=8 kg\cdotpm2I = 8\,\text{kgΒ·m}^2 and the wheel's Lspin=4 kg\cdotpm2/sL_{spin} = 4\,\text{kgΒ·m}^2/\text{s}?

Example 41

hard
Two skaters on ice, each of mass 60 kg60\,\text{kg}, hold a 4 m4\,\text{m} pole and rotate about its center at Ο‰=1.2 rad/s\omega = 1.2\,\text{rad/s}. They pull together so they are now 1 m1\,\text{m} apart. Find the new Ο‰\omega (treat them as point masses, pole massless).

Example 42

hard
A comet's perihelion (closest approach) is 0.5 AU0.5\,\text{AU} at speed 60 km/s60\,\text{km/s}. At aphelion it is 50 AU50\,\text{AU} from the Sun. Find its aphelion speed.

Example 43

hard
A 3 m3\,\text{m} uniform rod (M=4 kgM = 4\,\text{kg}) lies on frictionless ice. A 0.2 kg0.2\,\text{kg} puck moving at 8 m/s8\,\text{m/s} strikes it perpendicularly 1 m1\,\text{m} from the center and sticks. Find the angular speed of the rod+puck about their new center of mass. (Irod,CM=112ML2I_{rod,CM} = \tfrac{1}{12}M L^2.)

Example 44

challenge
A figure skater spins at 1.0 rev/s1.0\,\text{rev/s} with arms out (I=5 kg\cdotpm2I = 5\,\text{kgΒ·m}^2). She tucks to I=1 kg\cdotpm2I = 1\,\text{kgΒ·m}^2. Find her new rotational KE and the work she did.

Example 45

challenge
A solid sphere (I=25MR2I = \tfrac25 M R^2, M=2 kgM = 2\,\text{kg}, R=0.1 mR = 0.1\,\text{m}) rolls without slipping at v=3 m/sv = 3\,\text{m/s}. Find its total angular momentum about a point on the ground directly below its current center.

Example 46

challenge
A platform (Ip=100 kg\cdotpm2I_p = 100\,\text{kgΒ·m}^2) rotates at Ο‰0=2 rad/s\omega_0 = 2\,\text{rad/s}. A 50 kg50\,\text{kg} person stands at rim r=2 mr = 2\,\text{m}. They jump off radially outward. Find the platform's new angular speed.

Related Concepts

Background Knowledge

These ideas may be useful before you work through the harder examples.

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