Drag a spring to explore force, displacement and elastic potential energy.
Drag handle ↔
Force stays fixed when stiffness changes.
N/m
N
Display
F = kx● Current state
Applied force F
N
Displacement x
m
Stiffness k
N/m
Elastic potential energy U
J
Restoring force: 0.0 N
What is happening
At zero applied force, the spring has its natural length and stores no elastic energy. Try dragging the handle.
Drag a spring to explore force, displacement and elastic potential energy.Model notes
Ideal massless springs in static equilibrium: applied force F = kx and restoring force Fᵣ = −kx.
No oscillation, inertia, friction or gravity. Dragging passes through equilibrium states.
Hooke’s law applies within the elastic limit. Permanent deformation and breakage are not simulated.
x is displacement from the system’s natural length of 1.5 m; compression is negative. U = ½kx² is nonnegative.
Thicker drawn wire symbolizes greater stiffness; it is not a law for wire dimensions or material. All modes use the same force scale; an arrow beyond the frame has a break mark and the numerical reading stays exact. The energy column uses a fixed 0–200 J scale, and a pinned reference keeps the value at pinning.