Below is the observation when the pendulum A is set to vibration.
The lengths of the pendulums A and D are equal and hence their frequencies are equal. The length of pendulum C is greater than that of B is less than the lengths of A and D. If the pendulum A is set to vibration, then these vibrations reach the other pendulums also through the string XY. Hence, a periodic force of frequency equal to that of pendulum A begins to act upon other pendulums. It is observed that the pendulums C and B whose natural frequencies are different from frequency of A, are set into forced vibrations of very small amplitude, while the amplitude of vibrations of D increases slowly, and it becomes much larger than that of any other.
This is only due to resonance, since the frequencies of D and A are equal due to their equal length.
Resonance occurs when a system is able to store and easily transfer energy between two or more different storage modes (such as kinetic energy and potential energy in the case of a pendulum). However, there are some losses from cycle to cycle, called damping. When damping is small, the resonant frequency is approximately equal to the natural frequency of the system, which is a frequency of unforced vibrations. Some systems have multiple, distinct, resonant frequencies.