The Spring-Mass System
How spring constant k and mass m determine the time period — and what changes when springs are combined.
The spring-mass system is the prototype of SHM. Every result here applies — with appropriate substitution — to pendulums, LC circuits, and molecular vibrations.
The time period
Newton's second law + Hooke's law:
Heavier mass → slower oscillation
. Quadrupling mass doubles the period.
Light mass ( kg):
SpringMass amplitude 60 k 100 m 1
Show spring block wall graph-x readouts
Hide energy displacement-arrow velocity-arrow acceleration-arrow equilibrium
Heavy mass ( kg, same spring):
SpringMass amplitude 60 k 100 m 4
Show spring block wall graph-x readouts
Hide energy displacement-arrow velocity-arrow acceleration-arrow equilibrium
Watch the x(t) graph — cycles are twice as wide. T displayed in the readout confirms it.
Stiffer spring → faster oscillation
. Quadrupling stiffness halves the period.
Soft spring ( N/m):
SpringMass amplitude 60 k 50 m 1
Show spring block wall graph-x readouts
Hide energy displacement-arrow velocity-arrow acceleration-arrow equilibrium
Stiff spring ( N/m, same mass):
SpringMass amplitude 60 k 200 m 1
Show spring block wall graph-x readouts
Hide energy displacement-arrow velocity-arrow acceleration-arrow equilibrium
Springs in series
Two springs end-to-end. Same force stretches both — displacements add:
Effective stiffness is less than either spring. Period is longer.
Springs in parallel
Two springs side by side. Same displacement — forces add:
Effective stiffness is greater. Period is shorter.
Cutting a spring
A spring of constant cut to of its length has constant .
Fewer coils → each coil must stretch more per unit force → stiffer.
| Configuration | ||
|---|---|---|
| Single | ||
| Series | longer | |
| Parallel | shorter | |
| Cut to |