Read turning points and force directions from potential energy
For a conservative one-particle model with total mechanical energy E, kinetic energy at position x is K=E−U(x). A position is accessible only when E≥U there. Where E=U, speed is zero; such positions can be turning points. Where E<U, a negative number is an energy deficit, not a physical negative kinetic energy.
Learning outcome: Compare total energies 2,4 and 8 J. Locate turning points from the intersection condition before reading them. At E=2 J, test x=0 to produce a forbidden position; explain why the model withholds speed. Use graph slopes to identify force directions on both sides of the minimum.
Starting recap
Review signed force components, graph areas, speed squared and system boundaries. Distinguish an interaction force from an energy store or transfer.
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Try
With E=4 J, turning points satisfy 2|x−2|=4, so x=0 and 4 m. At x=1 m, U=2 J and K=2 J. For mass 2 kg, speed is√2≈1.41 m/s. The object could be moving either right or left there. At the minimum x=2, K=4 J and speed 2 m/s.
Open the experimentPredict
If you raise both the potential-energy curve and total-energy line by 10 J, should any turning position move?
Experiment
Compare total energies 2,4 and 8 J. Locate turning points from the intersection condition before reading them. At E=2 J, test x=0 to produce a forbidden position; explain why the model withholds speed. Use graph slopes to identify force directions on both sides of the minimum.
Test accessible positions in a potential landscape
Worked teaching model · synthetic values · A 2 kg particle has potential U(x)=2|x−2| J for all x. This idealized V-shaped well has a sharp cusp at x=2; force is not uniquely defined exactly at the cusp. Position choices with E<U are rejected, not assigned imaginary speed. Direction of motion is not determined by energy alone.
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Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Total mechanical energy | 4 | J |
| Potential energy at selected position | 2 | J |
| Available E minus U | 2 | J |
| Position accessible | 1 | 0 no / 1 yes |
| Speed magnitude | 1.41421 | m/s |
| Left turning position | 0 | m |
| Right turning position | 4 | m |
Accessible plot coordinates
| position (m) | energy (J) |
|---|---|
| -3 | 10 |
| -2.5 | 9 |
| -2 | 8 |
| -1.5 | 7 |
| -1 | 6 |
| -0.5 | 5 |
| 0 | 4 |
| 0.5 | 3 |
| 1 | 2 |
| 1.5 | 1 |
| 2 | 0 |
| 2.5 | 1 |
| 3 | 2 |
| 3.5 | 3 |
| 4 | 4 |
| 4.5 | 5 |
| 5 | 6 |
| 5.5 | 7 |
| 6 | 8 |
| 6.5 | 9 |
| 7 | 10 |
| position (m) | energy (J) |
|---|---|
| -3 | 4 |
| -2.5 | 4 |
| -2 | 4 |
| -1.5 | 4 |
| -1 | 4 |
| -0.5 | 4 |
| 0 | 4 |
| 0.5 | 4 |
| 1 | 4 |
| 1.5 | 4 |
| 2 | 4 |
| 2.5 | 4 |
| 3 | 4 |
| 3.5 | 4 |
| 4 | 4 |
| 4.5 | 4 |
| 5 | 4 |
| 5.5 | 4 |
| 6 | 4 |
| 6.5 | 4 |
| 7 | 4 |
K=E−U gives a speed magnitude, not its direction.
The solid curve is U and dashed line is E. Turning points satisfy U=E. Force points toward lower potential on each side (negative slope gives positive force); the cusp is an idealization. Adding the same constant to U and E changes no prediction.
K=E−U gives a speed magnitude, not its direction.
The solid curve is U and dashed line is E. Turning points satisfy U=E. Force points toward lower potential on each side (negative slope gives positive force); the cusp is an idealization. Adding the same constant to U and E changes no prediction.
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Sketch a smooth hill instead of a well. Explain why its top can be an equilibrium point but not a stable one.
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