Assuming a monopole sound source in free-field, RMS particle velocity $v$ and RMS pressure $p$ are related to each other with (chapter 2 p. 51 from Beranek & Mellow 2012)
$$v(r) = \frac{ p(r) }{Z }\sqrt{1 + (\frac{c}{ 2 \pi f r})^2}$$
with $r$ distance to the source,
$Z $ medium impedance,
$ c $ sound speed,
$ f $ sound frequency.
For distance $r$ far greater than the wave length, particle velocity and pressure are proportional:
$$ v(r) = \frac{p(r)}{Z}$$
As a consequence, as long as your speaker is in the far-field of your insect/microphone ($r >> c/f$), you can monitor the particle-velocity level from the pressure level. If not, it is better to have a pressure-gradient microphone (see SE question How reliable are "particle-velocity" microphones?).