Comparing EMC to shock and vibe (the mechanical equivalent) is interesting.
Normally, EMC does:
- Susceptibility sweep (single frequency with modulation, applied to cables, and with antennas, as appropriate)
- Surges (on applicable power input or load connections)
- Spikes (on cables and pins)
- ESD (anywhere it can touch)
And also checking emissions.
Nothing is measured during the susceptibility tests, and it is assumed that the instruments are calibrated to deliver their specified waveforms into a suitable dummy load (or in the case of the susceptibility sweep, it's usually measured at the final amplifier, but not at the coupling network to, or in the space around, the EUT). In general, one wouldn't expect significant nonlinearity to occur, so the frequencies the EUT is subjected to will be largely what's given.
Shock and vibe does fully body acceleration, in three axes each:
- Sine wave sweep (low level, no modulation -- somewhat akin to an EMC emissions sweep, even though this uses an external source)
- Sine wave sweep (at specified level -- stress test)
- Surges (usually X acceleration for Y ms, N cycles)
- Random noise (some RMS acceleration, for specified duration)
Acceleration sensors are attached to the shake table and EUT; acceleration is calibrated at the table, but measured in as many locations as desired.
What you see on the readout during the high level sweep (and in the averaged FT view of the random test) is similar to the peaks and valleys of the low level sweep, but depending on construction, those features can be expected to appear flatter (lower peaks, higher valleys), or shifted somewhat higher in frequency, due to the harmonic generation and frequency mixing action (and yes, even parametric oscillators) of wobbly materials shaking and sliding and slapping around.
What you see on the transient readout, is similar to the input pulses, but with much more 'crashing' behavior -- high frequency content that wasn't there before, and which dies down in an inconsistent fashion, as energy sloshes between different axes (only one of which is being measured) and between different degrees of freedom (like how a square plate has spacially orthogonal, but spectrally identical, resonant modes; which are normally independent, but can be coupled together by a nonuniformity, for example a screw near the corner).
So, as poor a grasp as us EEs have on modeling our circuits, my heart goes out to those few MEs who have to delve into the nitty gritty, multidimensional, manifestly coupled, highly nonlinear and inconsistent systems they have to work with. Which fortunately isn't all that many, but when every gram counts -- aerospace for example -- you have to take the time to optimize resonant modes to require the least amount of damping and such.
Tim