Series and parallel springs explained

In mechanics, two or more springs are said to be in series when they are connected end-to-end or point to point, and it is said to be in parallel when they are connected side-by-side; in both cases, so as to act as a single spring:

align=center Seriesalign=center Parallel
align=center align=center

More generally, two or more springs are in series when any external stress applied to the ensemble gets applied to each spring without change of magnitude, and the amount strain (deformation) of the ensemble is the sum of the strains of the individual springs. Conversely, they are said to be in parallel if the strain of the ensemble is their common strain, and the stress of the ensemble is the sum of their stresses.

Any combination of Hookean (linear-response) springs in series or parallel behaves like a single Hookean spring. The formulas for combining their physical attributes are analogous to those that apply to capacitors connected in series or parallel in an electrical circuit.

Formulas

Equivalent spring

The following table gives formula for the spring that is equivalent to a system of two springs, in series or in parallel, whose spring constants are

k1

and

k2

.[1] (The compliance

c

of a spring is the reciprocal

1/k

of its spring constant.)
QuantityIn SeriesIn Parallel
Equivalent spring constant
1
keq

=

1
k1

+

1
k2

keq=k1+k2

Equivalent compliance

ceq=c1+c2

1
ceq

=

1
c1

+

1
c2

Deflection (elongation)

xeq=x1+x2

xeq=x1=x2

Force

Feq=F1=F2

Feq=F1+F2

Stored energy

Eeq=E1+E2

Eeq=E1+E2

Partition formulas

QuantityIn SeriesIn Parallel
Deflection (elongation)
x1
x2

=

k2
k1

=

c1
c2

x1=x2

Force

F1=F2

F1
F2

=

k1
k2

=

c2
c1

Stored energy
E1
E2

=

k2
k1

=

c1
c2

E1
E2

=

k1
k2

=

c2
c1

Derivations of spring formula (equivalent spring constant)

See also

Notes and References

  1. Keith Symon (1971), Mechanics. Addison-Wesley.