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Springs in series/parallel oscillations

Intermediate

Equivalent stiffness changes the frequency.

Effective stiffness changes the frequency: parallel k = k₁ + k₂ (higher f), series 1/k = 1/k₁ + 1/k₂ (lower f).

Worked example

Two 20 N/m springs in parallel: ω rises by √2.

Common mistake

Check how the springs are connected to the mass.

In more detail

Springs in series or parallel change the effective spring constant, which changes the oscillation frequency. Parallel springs stiffen the system, and series springs soften it.

Real-world uses

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Frequently asked questions

Which increases frequency?

Springs in parallel, because the effective spring constant is larger.

How do I find the effective constant?

Add the constants for parallel springs, and use reciprocal sums for series springs.

How do combined springs change the frequency?

Stiffer combinations give a higher frequency, while softer ones give a lower frequency, since the frequency depends on the square root of the stiffness.

Related topics in Oscillations & SHM

Phasor representation · Mass–spring system · Vertical spring · Simple pendulum · Small-angle approximation · Pendulum at large amplitude

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