Separate changes in speed from changes in direction
A vector derivative can be nonzero even when a scalar speed derivative is zero.
Learning outcome: Vary u at fixed b and then b at fixed u. Reconstruct dot and cross products, verify the component-square identity and explain the equal-scale path.
Starting recap
Read derivatives as local rates and integrals as signed accumulation. Review power and chain rules, vector components, units and initial conditions where used.
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Try
At u=3,b=1,t=2, speed=sqrt13, tangential acceleration2/sqrt13 and normal3/sqrt13. Their squared sum is1 m²/s⁴.
Open the experimentPredict
For nonzero velocity, a·v divided by speed gives:
Experiment
Vary u at fixed b and then b at fixed u. Reconstruct dot and cross products, verify the component-square identity and explain the equal-scale path.
Resolve acceleration along and across the trajectory
Worked teaching model · synthetic values · Parametric trajectory r=(u t,b t²/2), t from0 to4 s; evaluation at2 s. Positive u,b ensure nonzero speed and defined tangent/normal. Curvature is geometry, not proof of a particular force.
Reset keeps your prediction, captures and practice history.
Parametric path with equal spatial scales
Spatial axes use the same pixels per physical unit, preserving geometry. 1: r(t),0–4 s (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Parametric path with equal spatial scales
r(t),0–4 s
| east position (m) | north position (m) |
|---|---|
| 0 | 0 |
| 0.1 | 0.00125 |
| 0.2 | 0.005 |
| 0.3 | 0.01125 |
| 0.4 | 0.02 |
| 0.5 | 0.03125 |
| 0.6 | 0.045 |
| 0.7 | 0.06125 |
| 0.8 | 0.08 |
| 0.9 | 0.10125 |
| 1 | 0.125 |
| 1.1 | 0.15125 |
| 1.2 | 0.18 |
| 1.3 | 0.21125 |
| 1.4 | 0.245 |
| 1.5 | 0.28125 |
| 1.6 | 0.32 |
| 1.7 | 0.36125 |
| 1.8 | 0.405 |
| 1.9 | 0.45125 |
| 2 | 0.5 |
| 2.1 | 0.55125 |
| 2.2 | 0.605 |
| 2.3 | 0.66125 |
| 2.4 | 0.72 |
| 2.5 | 0.78125 |
| 2.6 | 0.845 |
| 2.7 | 0.91125 |
| 2.8 | 0.98 |
| 2.9 | 1.05125 |
| 3 | 1.125 |
| 3.1 | 1.20125 |
| 3.2 | 1.28 |
| 3.3 | 1.36125 |
| 3.4 | 1.445 |
| 3.5 | 1.53125 |
| 3.6 | 1.62 |
| 3.7 | 1.71125 |
| 3.8 | 1.805 |
| 3.9 | 1.90125 |
| 4 | 2 |
| 4.1 | 2.10125 |
| 4.2 | 2.205 |
| 4.3 | 2.31125 |
| 4.4 | 2.42 |
| 4.5 | 2.53125 |
| 4.6 | 2.645 |
| 4.7 | 2.76125 |
| 4.8 | 2.88 |
| 4.9 | 3.00125 |
| 5 | 3.125 |
| 5.1 | 3.25125 |
| 5.2 | 3.38 |
| 5.3 | 3.51125 |
| 5.4 | 3.645 |
| 5.5 | 3.78125 |
| 5.6 | 3.92 |
| 5.7 | 4.06125 |
| 5.8 | 4.205 |
| 5.9 | 4.35125 |
| 6 | 4.5 |
| 6.1 | 4.65125 |
| 6.2 | 4.805 |
| 6.3 | 4.96125 |
| 6.4 | 5.12 |
| 6.5 | 5.28125 |
| 6.6 | 5.445 |
| 6.7 | 5.61125 |
| 6.8 | 5.78 |
| 6.9 | 5.95125 |
| 7 | 6.125 |
| 7.1 | 6.30125 |
| 7.2 | 6.48 |
| 7.3 | 6.66125 |
| 7.4 | 6.845 |
| 7.5 | 7.03125 |
| 7.6 | 7.22 |
| 7.7 | 7.41125 |
| 7.8 | 7.605 |
| 7.9 | 7.80125 |
| 8 | 8 |
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 |
|---|---|---|
| East velocity | 2 | m/s |
| North velocity | 2 | m/s |
| Speed | 2.828427 | m/s |
| Tangential acceleration | 0.7071068 | m/s² |
| Normal acceleration magnitude | 0.7071068 | m/s² |
| Curvature | 0.08838835 | 1/m |
| Radius of curvature | 11.31371 | m |
Acceleration can change speed and direction simultaneously.
v=(u,bt), acceleration=(0,b). The dot product a·v divided by speed gives tangential acceleration; the cross-product magnitude |v×a| divided by speed gives normal acceleration. Curvature=|v×a|/|v|³ and an=v² curvature. These relations require nonzero speed; the controls deliberately exclude the zero-speed singularity.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Acceleration can change speed and direction simultaneously.
v=(u,bt), acceleration=(0,b). The dot product a·v divided by speed gives tangential acceleration; the cross-product magnitude |v×a| divided by speed gives normal acceleration. Curvature=|v×a|/|v|³ and an=v² curvature. These relations require nonzero speed; the controls deliberately exclude the zero-speed singularity.
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Why does a radius of curvature describe local geometry rather than the force law?
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