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Principle of Angular Impulse and Momentum

Dynamics · FE Reference Handbook section

Dynamics
4 formulas
10 exam-style examples
~53 min
All Dynamics lectures

Core formulas for this FE topic

Definitions, applicability, units, assumptions and worked examples for each relation.

Worked exam-style examples

The four ways this section is written on the real exam — thoughts first, then equations, then substitution.

Example 1
Perfectly plastic impact — Principle of Angular Impulse and Momentum

A 2 kg mass moving at 18 m/s strikes a stationary 8 kg mass and they move together. Find the common velocity and the energy lost.

Given

  • m1=2kg,v1=18m/sm_{1} = 2 kg, v_{1} = 18 m/s
  • m2=8kg,v2=0m_{2} = 8 kg, v_{2} = 0

Find

v' and ΔKE

Start with the thinking

  • Momentum is conserved in every impact; energy is not.
  • Plastic impact means one common final velocity.

Step-by-step solution

  1. Momentum

    m1v1+m2v2=(m1+m2)v′m_{1}v_{1} + m_{2}v_{2} = (m_{1} + m_{2})v'
  2. Substituting

    2(18)+8(0)=(10)v′2(18) + 8(0) = (10)v'
  3. Solve

    v′=36/10=3.600m/sv' = 36/10 = 3.600 m/s
  4. Initial KE

    ½(2)(18)2=324.0J½(2)(18)^{2} = 324.0 J
  5. Final KE

    ½(10)(3.600)2=64.8J½(10)(3.600)^{2} = 64.8 J
  6. Energy lost — ΔKE = 259.2 J

Answer:

v′ ≈ 3.60 m/s; ΔKE ≈ 259.2 J

Why the other options are there

  • 9.00 m/s (masses assumed equal)
  • ΔKE = 0 (energy assumed conserved)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 2
Angular acceleration of a rotating drum — Principle of Angular Impulse and Momentum

A drum with mass moment of inertia 21.0 kg·m² is driven by a constant torque of 132 N·m from rest. Find α and the angular speed after 5.5 s.

Given

  • I = 21.0 kg·m²

  • M = 132 N·m

  • t=5.5st = 5.5 s

Find

α and ω

Start with the thinking

  • Rotational analogue of F = ma is M = Iα.
  • Constant torque gives constant angular acceleration.

Step-by-step solution

  1. Rotational equation

    M=IαM = I\alpha
  2. Substituting

    α=132/21.0=6.286rad/s2\alpha = 132/21.0 = 6.286 rad/s^{2}
  3. Angular speed — ω = ω₀ + αt

  4. Substituting

    ω=0+6.286(5.5)=34.57rad/s\omega = 0 + 6.286(5.5) = 34.57 rad/s
  5. Convert

    ω=330.1rpm\omega = 330.1 rpm
Answer:

α ≈ 6.29 rad/s²; ω ≈ 34.6 rad/s (330.1 rpm)

Why the other options are there

  • 2,772 rad/s² (multiplied instead of divided)
  • 5.50 rad/s (revolutions confused with radians)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 3
Perfectly plastic impact — Principle of Angular Impulse and Momentum (2)

A 8 kg mass moving at 16 m/s strikes a stationary 9 kg mass and they move together. Find the common velocity and the energy lost.

Given

  • m1=8kg,v1=16m/sm_{1} = 8 kg, v_{1} = 16 m/s
  • m2=9kg,v2=0m_{2} = 9 kg, v_{2} = 0

Find

v' and ΔKE

Start with the thinking

  • Momentum is conserved in every impact; energy is not.
  • Plastic impact means one common final velocity.

Step-by-step solution

  1. Momentum

    m1v1+m2v2=(m1+m2)v′m_{1}v_{1} + m_{2}v_{2} = (m_{1} + m_{2})v'
  2. Substituting

    8(16)+9(0)=(17)v′8(16) + 9(0) = (17)v'
  3. Solve

    v′=128/17=7.529m/sv' = 128/17 = 7.529 m/s
  4. Initial KE

    ½(8)(16)2=1,024J½(8)(16)^{2} = 1,024 J
  5. Final KE

    ½(17)(7.529)2=481.9J½(17)(7.529)^{2} = 481.9 J
  6. Energy lost — ΔKE = 542.1 J

Answer:

v′ ≈ 7.53 m/s; ΔKE ≈ 542.1 J

Why the other options are there

  • 8.00 m/s (masses assumed equal)
  • ΔKE = 0 (energy assumed conserved)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 4
Angular acceleration of a rotating drum — Principle of Angular Impulse and Momentum (2)

A drum with mass moment of inertia 23.5 kg·m² is driven by a constant torque of 31 N·m from rest. Find α and the angular speed after 4.0 s.

Given

  • I = 23.5 kg·m²

  • M = 31 N·m

  • t=4.0st = 4.0 s

Find

α and ω

Start with the thinking

  • Rotational analogue of F = ma is M = Iα.
  • Constant torque gives constant angular acceleration.

Step-by-step solution

  1. Rotational equation

    M=IαM = I\alpha
  2. Substituting

    α=31/23.5=1.319rad/s2\alpha = 31/23.5 = 1.319 rad/s^{2}
  3. Angular speed — ω = ω₀ + αt

  4. Substituting

    ω=0+1.319(4.0)=5.28rad/s\omega = 0 + 1.319(4.0) = 5.28 rad/s
  5. Convert

    ω=50.4rpm\omega = 50.4 rpm
Answer:

α ≈ 1.32 rad/s²; ω ≈ 5.3 rad/s (50 rpm)

Why the other options are there

  • 728.5 rad/s² (multiplied instead of divided)
  • 0.84 rad/s (revolutions confused with radians)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 5
Perfectly plastic impact — Principle of Angular Impulse and Momentum (3)

A 4 kg mass moving at 7 m/s strikes a stationary 8 kg mass and they move together. Find the common velocity and the energy lost.

Given

  • m1=4kg,v1=7m/sm_{1} = 4 kg, v_{1} = 7 m/s
  • m2=8kg,v2=0m_{2} = 8 kg, v_{2} = 0

Find

v' and ΔKE

Start with the thinking

  • Momentum is conserved in every impact; energy is not.
  • Plastic impact means one common final velocity.

Step-by-step solution

  1. Momentum

    m1v1+m2v2=(m1+m2)v′m_{1}v_{1} + m_{2}v_{2} = (m_{1} + m_{2})v'
  2. Substituting

    4(7)+8(0)=(12)v′4(7) + 8(0) = (12)v'
  3. Solve

    v′=28/12=2.333m/sv' = 28/12 = 2.333 m/s
  4. Initial KE

    ½(4)(7)2=98.0J½(4)(7)^{2} = 98.0 J
  5. Final KE

    ½(12)(2.333)2=32.7J½(12)(2.333)^{2} = 32.7 J
  6. Energy lost — ΔKE = 65.3 J

Answer:

v′ ≈ 2.33 m/s; ΔKE ≈ 65 J

Why the other options are there

  • 3.50 m/s (masses assumed equal)
  • ΔKE = 0 (energy assumed conserved)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 6
Angular acceleration of a rotating drum — Principle of Angular Impulse and Momentum (3)

A drum with mass moment of inertia 21.5 kg·m² is driven by a constant torque of 99 N·m from rest. Find α and the angular speed after 5.0 s.

Given

  • I = 21.5 kg·m²

  • M = 99 N·m

  • t=5.0st = 5.0 s

Find

α and ω

Start with the thinking

  • Rotational analogue of F = ma is M = Iα.
  • Constant torque gives constant angular acceleration.

Step-by-step solution

  1. Rotational equation

    M=IαM = I\alpha
  2. Substituting

    α=99/21.5=4.605rad/s2\alpha = 99/21.5 = 4.605 rad/s^{2}
  3. Angular speed — ω = ω₀ + αt

  4. Substituting

    ω=0+4.605(5.0)=23.02rad/s\omega = 0 + 4.605(5.0) = 23.02 rad/s
  5. Convert

    ω=219.9rpm\omega = 219.9 rpm
Answer:

α ≈ 4.60 rad/s²; ω ≈ 23.0 rad/s (219.9 rpm)

Why the other options are there

  • 2,129 rad/s² (multiplied instead of divided)
  • 3.66 rad/s (revolutions confused with radians)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 7
Perfectly plastic impact — Principle of Angular Impulse and Momentum (4)

A 3 kg mass moving at 11 m/s strikes a stationary 10 kg mass and they move together. Find the common velocity and the energy lost.

Given

  • m1=3kg,v1=11m/sm_{1} = 3 kg, v_{1} = 11 m/s
  • m2=10kg,v2=0m_{2} = 10 kg, v_{2} = 0

Find

v' and ΔKE

Start with the thinking

  • Momentum is conserved in every impact; energy is not.
  • Plastic impact means one common final velocity.

Step-by-step solution

  1. Momentum

    m1v1+m2v2=(m1+m2)v′m_{1}v_{1} + m_{2}v_{2} = (m_{1} + m_{2})v'
  2. Substituting

    3(11)+10(0)=(13)v′3(11) + 10(0) = (13)v'
  3. Solve

    v′=33/13=2.538m/sv' = 33/13 = 2.538 m/s
  4. Initial KE

    ½(3)(11)2=181.5J½(3)(11)^{2} = 181.5 J
  5. Final KE

    ½(13)(2.538)2=41.9J½(13)(2.538)^{2} = 41.9 J
  6. Energy lost — ΔKE = 139.6 J

Answer:

v′ ≈ 2.54 m/s; ΔKE ≈ 139.6 J

Why the other options are there

  • 5.50 m/s (masses assumed equal)
  • ΔKE = 0 (energy assumed conserved)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 8
Angular acceleration of a rotating drum — Principle of Angular Impulse and Momentum (4)

A drum with mass moment of inertia 30.0 kg·m² is driven by a constant torque of 170 N·m from rest. Find α and the angular speed after 5.5 s.

Given

  • I = 30.0 kg·m²

  • M = 170 N·m

  • t=5.5st = 5.5 s

Find

α and ω

Start with the thinking

  • Rotational analogue of F = ma is M = Iα.
  • Constant torque gives constant angular acceleration.

Step-by-step solution

  1. Rotational equation

    M=IαM = I\alpha
  2. Substituting

    α=170/30.0=5.667rad/s2\alpha = 170/30.0 = 5.667 rad/s^{2}
  3. Angular speed — ω = ω₀ + αt

  4. Substituting

    ω=0+5.667(5.5)=31.17rad/s\omega = 0 + 5.667(5.5) = 31.17 rad/s
  5. Convert

    ω=297.6rpm\omega = 297.6 rpm
Answer:

α ≈ 5.67 rad/s²; ω ≈ 31.2 rad/s (297.6 rpm)

Why the other options are there

  • 5,100 rad/s² (multiplied instead of divided)
  • 4.96 rad/s (revolutions confused with radians)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 9
Perfectly plastic impact — Principle of Angular Impulse and Momentum (5)

A 6 kg mass moving at 15 m/s strikes a stationary 7 kg mass and they move together. Find the common velocity and the energy lost.

Given

  • m1=6kg,v1=15m/sm_{1} = 6 kg, v_{1} = 15 m/s
  • m2=7kg,v2=0m_{2} = 7 kg, v_{2} = 0

Find

v' and ΔKE

Start with the thinking

  • Momentum is conserved in every impact; energy is not.
  • Plastic impact means one common final velocity.

Step-by-step solution

  1. Momentum

    m1v1+m2v2=(m1+m2)v′m_{1}v_{1} + m_{2}v_{2} = (m_{1} + m_{2})v'
  2. Substituting

    6(15)+7(0)=(13)v′6(15) + 7(0) = (13)v'
  3. Solve

    v′=90/13=6.923m/sv' = 90/13 = 6.923 m/s
  4. Initial KE

    ½(6)(15)2=675.0J½(6)(15)^{2} = 675.0 J
  5. Final KE

    ½(13)(6.923)2=311.5J½(13)(6.923)^{2} = 311.5 J
  6. Energy lost — ΔKE = 363.5 J

Answer:

v′ ≈ 6.92 m/s; ΔKE ≈ 363.5 J

Why the other options are there

  • 7.50 m/s (masses assumed equal)
  • ΔKE = 0 (energy assumed conserved)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

Example 10
Angular acceleration of a rotating drum — Principle of Angular Impulse and Momentum (5)

A drum with mass moment of inertia 23.5 kg·m² is driven by a constant torque of 69 N·m from rest. Find α and the angular speed after 9.5 s.

Given

  • I = 23.5 kg·m²

  • M = 69 N·m

  • t=9.5st = 9.5 s

Find

α and ω

Start with the thinking

  • Rotational analogue of F = ma is M = Iα.
  • Constant torque gives constant angular acceleration.

Step-by-step solution

  1. Rotational equation

    M=IαM = I\alpha
  2. Substituting

    α=69/23.5=2.936rad/s2\alpha = 69/23.5 = 2.936 rad/s^{2}
  3. Angular speed — ω = ω₀ + αt

  4. Substituting

    ω=0+2.936(9.5)=27.89rad/s\omega = 0 + 2.936(9.5) = 27.89 rad/s
  5. Convert

    ω=266.4rpm\omega = 266.4 rpm
Answer:

α ≈ 2.94 rad/s²; ω ≈ 27.9 rad/s (266.4 rpm)

Why the other options are there

  • 1,622 rad/s² (multiplied instead of divided)
  • 4.44 rad/s (revolutions confused with radians)

Reference: FE Reference Handbook — Dynamics → Principle of Angular Impulse and Momentum

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