
The peak axial displacement is 0.03 and the displacement in the stem is 0.01. The mode is normalized so that the maximum total displacement is 1. The displacements are shown in the figures below.

The tabletop surface will act as a large loudspeaker diaphragm. The motion is much smaller than the transverse motion of the prongs, but it has the potential to set the large flat tabletop in motion - a surface that is a far better emitter of sound than the thin prongs of a tuning fork. When you hold the stem of the tuning fork to a table, an axial motion in the stem connects to the tabletop. You can hear it, but it is not a very efficient conversion of the mechanical vibration into acoustic pressure. The pressure waves in the air propagate as sound.

When you hold a vibrating tuning fork in your hand, the bending motion of the prongs sets the air around them in motion.

As it turns out, the explanation behind this mystery can be boiled down to nonlinear solid mechanics. When you strike a tuning fork and hold it against a tabletop, it seems to double in frequency. In a recent video on YouTube from standupmaths, science enthusiasts Matt Parker and Hugh Hunt discuss and demonstrate the “mystery” of a tuning fork. In this blog post, we explain the tuning fork mystery using simulation and provide some fun facts about tuning forks along the way. When a tuning fork is struck, and held against a tabletop, the peak frequency of the emitted sound doubles - a mysterious behavior that has left many people baffled.
