Reject a circular path that needs a pulling surface
At the top of a convex circular support, inward points downward toward the circle center. A 2 kg point has gravity downward and a surface normal upward. The term centripetal force names the inward resultant needed for circular motion; it is not a third interaction to add to gravity and normal.
Learning outcome: Compare speeds 4,6,8 m/s at R=4 m. Draw the two actual interaction forces, then calculate the inward resultant. Keep failed required normal separate from actual force and state what is not predicted after separation.
Starting recap
Draw recipient-specific interactions, resolve signed components and identify the domain of each force/contact model before substituting.
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At R=4 m, the zero-normal speed is√40≈6.32456 m/s. A prescribed6 m/s state remains feasible, whereas8 m/s does not follow the circular-support model.
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A negative required normal at a convex crest means:
Experiment
Compare speeds 4,6,8 m/s at R=4 m. Draw the two actual interaction forces, then calculate the inward resultant. Keep failed required normal separate from actual force and state what is not predicted after separation.
Test whether a circular crest can supply its required force
Worked teaching model · synthetic values · A 2 kg point is at the top of a convex circular support, gravity 10 m/s². Normal force is upward, desired inward direction downward. Contact cannot pull inward. Failure means circular constraint invalid; no road-speed or ride-safety recommendation.
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Required circular-contact normal
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: conditional equation, negative means failure (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Required circular-contact normal
conditional equation, negative means failure
| speed (m/s) | required upward normal (N) |
|---|---|
| 0 | 20 |
| 0.2 | 19.98 |
| 0.4 | 19.92 |
| 0.6 | 19.82 |
| 0.8 | 19.68 |
| 1 | 19.5 |
| 1.2 | 19.28 |
| 1.4 | 19.02 |
| 1.6 | 18.72 |
| 1.8 | 18.38 |
| 2 | 18 |
| 2.2 | 17.58 |
| 2.4 | 17.12 |
| 2.6 | 16.62 |
| 2.8 | 16.08 |
| 3 | 15.5 |
| 3.2 | 14.88 |
| 3.4 | 14.22 |
| 3.6 | 13.52 |
| 3.8 | 12.78 |
| 4 | 12 |
| 4.2 | 11.18 |
| 4.4 | 10.32 |
| 4.6 | 9.42 |
| 4.8 | 8.48 |
| 5 | 7.5 |
| 5.2 | 6.48 |
| 5.4 | 5.42 |
| 5.6 | 4.32 |
| 5.8 | 3.18 |
| 6 | 2 |
| 6.2 | 0.78 |
| 6.4 | -0.48 |
| 6.6 | -1.78 |
| 6.8 | -3.12 |
| 7 | -4.5 |
| 7.2 | -5.92 |
| 7.4 | -7.38 |
| 7.6 | -8.88 |
| 7.8 | -10.42 |
| 8 | -12 |
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.
| Quantity | Value | Unit |
|---|---|---|
| Required circular inward acceleration | 9 | m/s² |
| Required upward normal | 2 | N |
| Actual contact normal | 2 | N |
| Actual instantaneous downward acceleration | 9 | m/s² |
| Circular contact branch feasible | 1 | flag |
| Critical speed for zero normal | 6.32456 | m/s |
Gravity minus the support force supplies the inward resultant at the crest.
At the top, mg−N=mv²/R. Centripetal force names that inward resultant, not a third interaction to add to gravity and normal. Equality N=0 is a marginal instantaneous contact boundary; beyond it actual free-flight acceleration is g, not v²/R constrained to the surface. No full post-separation trajectory is computed.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Gravity minus the support force supplies the inward resultant at the crest.
At the top, mg−N=mv²/R. Centripetal force names that inward resultant, not a third interaction to add to gravity and normal. Equality N=0 is a marginal instantaneous contact boundary; beyond it actual free-flight acceleration is g, not v²/R constrained to the surface. No full post-separation trajectory is computed.
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Why does changing from crest to valley change the signs in the radial balance?
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