(a) Series Combination
As shown in Fig. spring S1 and S2 are joined in series. A mass hanging from the combination is stretched y distance downwards and left, then the working force on both the springs is same; where as the increase in lengths is y1 and y2 respectively (suppose) are different. The restoring force for spring Si in this combination is;
F1 = -K1 y1
Fig: Series combination of the springs
and restoring force in the spring S2 is;
F2 = -k2y2
Since, the tension on both the springs is same hence the working restoring force on the body.
where, k is the effective spring constant of combination. If n springs of spring constant k1 = k2 = k3 =….= k’ are joined in series, then k will be the effective spring constant of combination.
(b) Parallel Combination
Two springs having spring constant k1 and k2 are combined in parallel from same base and mass m is hanged from the free end of the springs together. The weight is given y displacement from the equilibrium position, then both springs are extended equally in length; where as the restoring force on both the springs is different.
Hence the restoring force working on both the springs is;
F1 = -k1y
and F2 = -k2 y respectively;
The effective restoring force on the combination in this position is;
F = F1 + F2
– ky = -k1y – k2y
and effective spring constant k = k1 + k2
Fig: Series combination of the springs
Time period of oscillating body;
\(T = 2 \pi \sqrt{\frac{m}{k}}\)
where, effective spring constant
k = k1 + k2