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 experimentPredict
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.
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Net torque history
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 |
| 0.2 | 0.08 |
| 0.25 | 0.3125 |
| 0.3 | 0.53 |
| 0.35 | 0.7325 |
| 0.4 | 0.92 |
| 0.45 | 1.0925 |
| 0.5 | 1.25 |
| 0.55 | 1.3925 |
| 0.6 | 1.52 |
| 0.65 | 1.6325 |
| 0.7 | 1.73 |
| 0.75 | 1.8125 |
| 0.8 | 1.88 |
| 0.85 | 1.9325 |
| 0.9 | 1.97 |
| 0.95 | 1.9925 |
| 1 | 2 |
| 1.05 | 1.9925 |
| 1.1 | 1.97 |
| 1.15 | 1.9325 |
| 1.2 | 1.88 |
| 1.25 | 1.8125 |
| 1.3 | 1.73 |
| 1.35 | 1.6325 |
| 1.4 | 1.52 |
| 1.45 | 1.3925 |
| 1.5 | 1.25 |
| 1.55 | 1.0925 |
| 1.6 | 0.92 |
| 1.65 | 0.7325 |
| 1.7 | 0.53 |
| 1.75 | 0.3125 |
| 1.8 | 0.08 |
| 1.85 | -0.1675 |
| 1.9 | -0.43 |
| 1.95 | -0.7075 |
| 2 | -1 |
Integrated angular momentum
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 |
| 1.65 | 0.025375 |
| 1.7 | 0.057 |
| 1.75 | 0.078125 |
| 1.8 | 0.088 |
| 1.85 | 0.085875 |
| 1.9 | 0.071 |
| 1.95 | 0.042625 |
| 2 | 0 |
| Quantity | Value | Unit |
|---|---|---|
| Net angular impulse | 2 | N m s |
| Final angular momentum | 0 | kg m²/s |
| Final angular velocity | 0 | rad/s |
| Average net torque | 1 | N m |
| Angular displacement over interval | -1 | rad |
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.
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Which data would be required to reconstruct angle if rotational inertia varied with time?
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