6.2.4Energy and Momentum of Rotating Systems
Angular Impulse Graphs — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 9 parts Lesson 7 of 13 1 quiz
Lesson summary
6.2.4 Angular Impulse Graphs — AP PHYSICS 1 notes: Interpret torque–time and angular momentum–time graphs, finding angular impulse from areas and torque from gradients.Area — the area under a net torque–time graph equals the angular impulse, which equals ΔL.Sign — areas above the…
- Rectangle (constant torque)
- Straight line
- Horizontal line
- Curve with increasing gradient
- Constant I
- Gradient of ω–t
Section 1 of 9Torque–time graphs
1Area
- Area the area under a net torque–time graph equals the angular impulse, which equals ΔL.
2Sign
- Sign areas above the axis are positive and below are negative.
3Rectangle (constant torque)
- τΔt.
4Triangle
- ½ × base × height.
5Trapezium
- ½(a + b) × width.
6Total
- Total add areas of simple shapes and subtract those below the axis.
Section 2 of 9Angular momentum–time graphs
Angular momentum–time graphs
Gradient
- Gradient equals the net torque, since τ = ΔL/Δt.
Straight line
- Straight line constant torque.
Horizontal line
- Horizontal line zero net torque, so L is conserved.
Curve with increasing gradient
- Curve with increasing gradient growing torque.
Relation
- Relation the τ–t graph is the gradient of the L–t graph and the L–t graph is built from the area under the τ–t graph.
Section 3 of 9Angular velocity from graphs
Constant I
- ω = L/I, so an L–t graph has the shape of an ω–t graph scaled by 1/I.
Gradient of ω–t
- α = τ/I.
Final ω
- Final ω find the area (ΔL), divide by I, and add the initial ω.
Example
- Example a triangle of 15 N·m·s and a rectangle of −10 N·m·s give ΔL = 5 N·m·s;
- with I = 5.0 kg·m2 and ω0 = −2.0 rad/s, ω = −1.0 rad/s.
Section 4 of 9Reading graphs carefully
Axes and units
- Axes and units check them before computing areas.
Force graph
- Force graph multiply by the lever arm to get torque.
Irregular shapes
- Irregular shapes count squares and convert using the value of one square.
Below the axis
- Below the axis the torque reverses and ΔL reduces.
Torque returning to zero
- Torque returning to zero the object then keeps ω constant.
Section 5 of 9Impulse versus work graphs
| Graph | Horizontal axis | Area gives |
|---|---|---|
| τ against t | Time | Angular impulse ΔL |
| τ against θ | Angle | Work |
Check
- Check read the axis label to tell which is shown.
Analogy
- Analogy area under F–t gives Δp; area under τ–t gives ΔL.
Section 6 of 9Sketching from a description
1Steady torque for 3.0 s then coasting
- τ–t is a rectangle ending at 3.0 s; L–t rises linearly then becomes horizontal.
2With constant opposing friction
- L rises more gently during the push, then falls with a small negative gradient.
3Check
- Check positive area minus negative area equals the final ΔL; equal areas return L to zero.
4Labels
- Labels label axes with quantities and units, and mark key times.
Section 7 of 9More from the specification
More from the specification
Rotation
- Motion in which an object turns about an axis.
Collision
- Short interaction with large internal forces.
Newton
- Unit of force, kg m s-2.
Rotational inertia
- Resistance to angular acceleration, I = Σmr2.
Average torque
- Constant torque giving the same angular impulse in the same time.
External torque
- Torque produced by a force from outside the system.
Rigid system
- System that holds its shape while rotating.
Velocity
- Rate of change of displacement.
Inertia
- Resistance of an object to changes in its motion.
Distance
- Total length of path travelled, a scalar.
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Torque–time graph | Graph whose area gives the angular impulse. |
| Gradient | Slope of a graph; on an L–t graph it is the net torque. |
| Area under a curve | Product of the two axis quantities. |
| Angular impulse | τΔt, equal to the change in angular momentum. |
| Constant torque | Horizontal line on a τ–t graph, sloped line on an L–t graph. |
Section 9 of 9Exam technique
1
Taking the gradient of a torque–time graph instead of the area to find ΔL.
2
Mixing the meaning of the area under τ–t (impulse) and τ–θ (work).
3
Forgetting to subtract areas below the axis.
4
Using the maximum torque instead of the average for a varying torque.
5
Not dividing by I to convert ΔL to Δω.
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