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SCIENCE · INVESTIGATE AND EXPLAIN

Change force branches at a stopping event

A 2 kg object starts sliding right with speed v0 on a level plane. Gravity is 10 m/s², μk=0.3 and μs=0.5. A constant rightward drive F lies between 0 and 10 N. During rightward slip kinetic friction is 6 N leftward, so acceleration is (F−6)/2 m/s².

Learning outcome: Compare F=0,4,6,10 N at v0=2 m/s. Predict whether a stop exists and whether it lies in the 2 s interval. Retain the position and velocity at the event before evaluating the final state.

Starting recap

Draw recipient-specific interactions, resolve signed components and identify the domain of each force/contact model before substituting.

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Try

With F=4 N and v0=2 m/s, acceleration is−1 m/s² and the stop occurs exactly at 2 s after 2 m. Immediately after stopping, static friction balances4 N rather than retaining the 6 N sliding value.

Open the experiment

Predict

After a stop with drive below static capacity, continuing the old sliding formula would:

Experiment

Compare F=0,4,6,10 N at v0=2 m/s. Predict whether a stop exists and whether it lies in the 2 s interval. Retain the position and velocity at the event before evaluating the final state.

Stop a sliding object without inventing reverse friction

Worked teaching model · synthetic values · A 2 kg object slides right on a level plane with g=10, mu_k=.3 and mu_s=.5. Drive stays between 0 and 10 N. Observe 2 s; after any stop the available static friction can balance the drive. No reversed kinetic branch is imposed.

Reset keeps your prediction, captures and practice history.

Velocity with stop-and-stick event

rightward velocity (m/s)time (s)0220

Unlike graph quantities rescale independently; read units and values, not screen angles. 1: admissible velocity (solid). Joined curves show the supplied model, not additional observations.

Equivalent numerical coordinates for Velocity with stop-and-stick event

admissible velocity

time (s)rightward velocity (m/s)
02
0.051.9
0.11.8
0.151.7
0.21.6
0.251.5
0.31.4
0.351.3
0.41.2
0.451.1
0.51
0.550.9
0.60.8
0.650.7
0.70.6
0.750.5
0.80.4
0.850.3
0.90.2
0.950.1
10
1.050
1.10
1.150
1.20
1.250
1.30
1.350
1.40
1.450
1.50
1.550
1.60
1.650
1.70
1.750
1.80
1.850
1.90
1.950
20

At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.

Calculated quantities under the declared measurement model
QuantityValueUnit
Initial sliding acceleration-2m/s²
Stop time in continued sliding model1s
Position after 2 s1m
Velocity after 2 s0m/s
Stopped by interval end1flag
Static capacity after a stop10N
Friction magnitude at interval end2N

The friction law changes at zero slip; an extrapolated negative velocity is not the next state here.

Before a stop, kinetic friction is 6 N leftward. If F<6 N, the stop time is v0/((6−F)/2). Afterward static friction balances F because F≤10 N, so the object stays at rest. If F=6 N it keeps its initial speed; larger drive accelerates it rightward. This is not a physical stopping-distance or traction guarantee.

Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.

The friction law changes at zero slip; an extrapolated negative velocity is not the next state here.

Before a stop, kinetic friction is 6 N leftward. If F<6 N, the stop time is v0/((6−F)/2). Afterward static friction balances F because F≤10 N, so the object stays at rest. If F=6 N it keeps its initial speed; larger drive accelerates it rightward. This is not a physical stopping-distance or traction guarantee.

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

Understand

Define the recipient and model

A 2 kg object starts sliding right with speed v0 on a level plane. Gravity is 10 m/s², μk=0.3 and μs=0.5. A constant rightward drive F lies between 0 and 10 N. During rightward slip kinetic friction is 6 N leftward, so acceleration is (F−6)/2 m/s².

Build the algebraic relationship

When F<6 N, solve v0+(F−6)t/2=0 to locate the stop. The root is an event boundary, not permission to continue the same friction direction into negative velocity. Once slip ceases, static friction can balance any selected drive because its capacity is 10 N. The object therefore remains at rest after the stop.

Check the changed state

For F=2 N and v0=2 m/s, initial acceleration is−2 m/s², stop time is 1 s and displacement to the stop is 1 m. At t=2 s the object is still there with zero velocity. Extending the old parabola to 2 s would return it to its starting point, an invented reverse motion that is inconsistent with the new contact state.

Interpret evidence and limits

If F=6 N, the object maintains its nonzero initial speed because net force is zero. If F>6 N, it accelerates rightward and never reaches a stopping event in this model. A stop exactly at the 2 s observation endpoint contributes no reverse segment. This ideal coefficient model is not a transport stopping-distance or braking-safety rule.

Worked original packet

With F=4 N and v0=2 m/s, acceleration is−1 m/s² and the stop occurs exactly at 2 s after 2 m. Immediately after stopping, static friction balances4 N rather than retaining the 6 N sliding value.

Bounded investigation

Compare F=0,4,6,10 N at v0=2 m/s. Predict whether a stop exists and whether it lies in the 2 s interval. Retain the position and velocity at the event before evaluating the final state.

Changed-case numerical practice

Try the changed case before feedback

A 2 kg object starts at 3 m/s rightward, with 6 N kinetic friction leftward and no applied drive. If static balance holds after the stop, how far does it travel in the first2 s, in metres?

This practice is public and unsaved. A matching number does not verify understanding. Retain your explanation, assumptions and changed-case evidence in the separate course workspace.

Sources and boundaries

Original prose, data and diagrams checked 30 October 2026 against OpenStax College Physics 2e. This is an algebra-based virtual evidence exercise, not a physical experiment, equipment certification, transport recommendation or independent mastery result. Save assumptions and a competing explanation with the course evidence; supervised practical requirements remain external.

Apply

After a stop with drive below static capacity, continuing the old sliding formula would:

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

Why does a force law need a domain as well as a numerical coefficient?

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