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SCIENCE · INVESTIGATE AND EXPLAIN

Reconstruct angular momentum from a torque history

Integrate signed torque in time and test its derivative against the momentum record.

Learning outcome: Use A=3,B=1 and then A=3,B=2. Predict signed areas and final momenta. Differentiate your reconstructed L at t=0,1,2 and compare with the torque function. Integrate omega independently and explain why zero net impulse does not imply zero torque at every instant.

Starting recap

State the reference axis and system, distinguish time and angle integrals, and verify an accessible and supported motion branch.

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Try

For A=3 and B=1, impulse is 2 N m s. Starting at L=−2 gives Lf=0 and omega_f=0, but theta(2)=−1 rad. The average net torque is 1 N m; it is not the instantaneous torque at every time.

Open the experiment

Predict

What does the slope of a signed angular-momentum-versus-time graph represent?

Experiment

Use A=3,B=1 and then A=3,B=2. Predict signed areas and final momenta. Differentiate your reconstructed L at t=0,1,2 and compare with the torque function. Integrate omega independently and explain why zero net impulse does not imply zero torque at every instant.

Integrate net torque into angular momentum

Worked teaching model · synthetic values · Fixed I=2 kg m²,omega0=−1 rad/s,theta0=0. Net torque A t(2−t)−B over 0–2 s with dimensional2 s. Torque and momentum share the same fixed axis.

Reset keeps your prediction, captures and practice history.

Net torque history

torque (N m)time (s)022-1

Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.

Net torque history: numerical coordinates
time (s)torque (N m)
0-1
0.05-0.7075
0.1-0.43
0.15-0.1675
0.20.08
0.250.3125
0.30.53
0.350.7325
0.40.92
0.451.0925
0.51.25
0.551.3925
0.61.52
0.651.6325
0.71.73
0.751.8125
0.81.88
0.851.9325
0.91.97
0.951.9925
12
1.051.9925
1.11.97
1.151.9325
1.21.88
1.251.8125
1.31.73
1.351.6325
1.41.52
1.451.3925
1.51.25
1.551.0925
1.60.92
1.650.7325
1.70.53
1.750.3125
1.80.08
1.85-0.1675
1.9-0.43
1.95-0.7075
2-1

Integrated angular momentum

angular momentum (kg m²/s)time (s)020.088-2.088

Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.

Integrated angular momentum: numerical coordinates
time (s)angular momentum (kg m²/s)
0-2
0.05-2.04263
0.1-2.071
0.15-2.08588
0.2-2.088
0.25-2.07813
0.3-2.057
0.35-2.02537
0.4-1.984
0.45-1.93362
0.5-1.875
0.55-1.80888
0.6-1.736
0.65-1.65712
0.7-1.573
0.75-1.48438
0.8-1.392
0.85-1.29663
0.9-1.199
0.95-1.09987
1-1
1.05-0.900125
1.1-0.801
1.15-0.703375
1.2-0.608
1.25-0.515625
1.3-0.427
1.35-0.342875
1.4-0.264
1.45-0.191125
1.5-0.125
1.55-0.066375
1.6-0.016
1.650.025375
1.70.057
1.750.078125
1.80.088
1.850.085875
1.90.071
1.950.042625
20
Calculated values under the declared model
QuantityValueUnit
Net angular impulse2N m s
Final angular momentum0kg m²/s
Final angular velocity0rad/s
Average net torque1N m
Angular displacement over interval-1rad

Angular impulse is a time integral; angular work is an angle integral.

L=L0+integral tau dt, then omega=L/I. Integrating omega gives theta=−t+A(t³/6−t⁴/24)−Bt²/4. A zero net angular impulse can still contain nonzero torques and intermediate angular-momentum changes.

Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.

Angular impulse is a time integral; angular work is an angle integral.

L=L0+integral tau dt, then omega=L/I. Integrating omega gives theta=−t+A(t³/6−t⁴/24)−Bt²/4. A zero net angular impulse can still contain nonzero torques and intermediate angular-momentum changes.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Keep the reference axis fixed

For the selected fixed-axis system, net external torque equals dL/dt. Its signed time integral is angular impulse: J_L=integral tau dt=Lf−Li. Individual external torques can deliver nonzero impulses even when their sum cancels. A torque-time graph gives angular impulse through signed area; the slope of an angular-momentum-time graph gives net torque.

Integrate with the initial condition

Here I=2 kg m², omega0=−1 rad/s, so L0=−2 kg m²/s. The stipulated net torque is A t(2−t)−B from 0 to 2 s, with coefficients in consistent SI units. Integrating gives L(t)=−2+A(t²−t³/3)−Bt. The total angular impulse is 4A/3−2B. Dividing the result by I gives omega only because I is constant.

A second integral describes angle

With theta0=0, theta(t)=−t+A(t³/6−t⁴/24)−Bt²/4. Angular impulse and displacement are different integrals: at 2 s theta=−2+2A/3−B. A body can have zero final angular momentum yet have undergone a nonzero angle and nonzero intermediate torques. If I changed, integrate L first and use omega(t)=L(t)/I(t), rather than treating tau=I alpha with constant I.

Predict the graph before checking

At an instant where torque is negative, L has negative slope, regardless of whether L itself is positive or negative. At a zero of torque, the slope vanishes; this need not mean L=0. Compare a flat momentum segment with a momentum curve crossing zero. Only the first establishes zero net torque throughout that segment.

Worked original case

For A=3 and B=1, impulse is 2 N m s. Starting at L=−2 gives Lf=0 and omega_f=0, but theta(2)=−1 rad. The average net torque is 1 N m; it is not the instantaneous torque at every time.

Investigation

Use A=3,B=1 and then A=3,B=2. Predict signed areas and final momenta. Differentiate your reconstructed L at t=0,1,2 and compare with the torque function. Integrate omega independently and explain why zero net impulse does not imply zero torque at every instant.

Public numerical transfer practice

Try a new practice case

A system starts with angular momentum −3 kg m²/s and receives constant net torque 2 N m for 4 s. What is final signed angular momentum in kg m²/s?

This public, unsaved check is not a secure assessment. Explain the derivative, integral or boundary in the retained course evidence workspace.

Sources and evidence boundary

Original derivations and assigned numerical cases checked 30 October 2026 against the official AP Physics C Mechanics framework and OpenStax angular momentum. These are supplied or generated records, not physical measurements or performed laboratory time. Do not construct rotating equipment, release loads or conduct launch experiments. Public feedback and retained self-reports do not certify independent mastery.

Apply

What does the slope of a signed angular-momentum-versus-time graph represent?

Public practice checks a specific claim. It does not establish independent mastery.

Which data would be required to reconstruct angle if rotational inertia varied with time?

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