A healthy machine is not quiet. Under changing load and speed it produces a rich, variable vibration signal, and the early signature of a failing bearing or a growing imbalance is a small feature buried inside it, not an obvious spike. That is why a single overall vibration level is a poor early alarm: by the time the total energy has risen enough to trip a threshold, the fault is well advanced. The information about what is failing, and how early, lives in the frequency content, not the amplitude.
The physics is what makes diagnosis possible. Each fault mechanism excites vibration at frequencies tied to the machine's geometry — a bearing defect rings at frequencies set by its dimensions and speed, an imbalance shows at once-per-revolution, a gear defect throws sidebands around the tooth-mesh frequency. Spectral and envelope analysis expose those signatures, so a well-processed signal does not just say the machine is worse — it says which part is failing. But the fault frequencies shift with speed, so a machine that changes speed needs order tracking to keep the features from smearing.
None of this survives a poor sensing chain. Where the sensor is mounted, its bandwidth and its noise floor decide whether the small fault feature is even present in the data before any algorithm runs; a badly mounted sensor or too low a sampling rate loses the signature at the source. And because the baseline of normal shifts with load and speed, a fixed threshold either misses faults or floods false alarms — so the honest system models normal per operating point and trends features over time, catching a developing fault rather than reacting to one noisy reading.