Thanx Issac

.
He's dead, actually.
The membrane accelerates which it needs to do as to generate pulsating air pressure aka sound.
This needs a counterforce aka "actio equals reactio".
The counterforce is, in any and every case, no exception, the accelaration of another bulk of mass aka "force equals mass times acceleration".
Please let this sink in .. .. it is just so.
Regarding your question let's approximately think of two extremes.
(w) The other mass is all of the speaker, except for the membrane and nothing else, floating in space.
(y) The other mass is whole mother earth assumed to be rigid throughout. (Flat earth needs that, right?)
You see, in principal there is no difference, as earth is actually floating (y) as we assume it to be the case with the speaker alone shot into orbit (w).
(y) is easily related to a rigid coupling to the floor, which is rigidly coupled (hope so) to the ground ... down to the iron (audiophile grade) core.
(w) is understood as a weak, soft, wobbley stand; the forces the stand can and will relay to somewhere else are so weak, that they can be neglected. This will be exemplified further.
The relative acceleration of the other mass depends on the proportion of the masses. A heavy bass cone might weigh 100grams,. Calculating it for (w) the according speaker will weigh about 40kilograms. So the ratio is 1 : 400 and so will be the ratio of acceleration.
For the acoustical impact the surface areas have to be taken into account. The surface area of the membrane is about 550cm^2 that of the front baffle 100cm*40cm - cone area = 4000cm^2 - 550cm^2 = 3450cm^2. Related to the cone area this yields a ratio of 6.3 : 1.
Finally relating the acoustical output of cone versus front baffle taking acceleration and surface area into account (expressed in dB): 20*log10(6.3 / 400) = -36dB.
The baffle area's contribution, if and when it obeys to Newton's laws lies 36dB below the cones contribution, altering efficiency or frequency response by not more than 0.1dB (o-point-one).
A second thought may be that the backwall of the speaker radiates the same sound, but counterphase, cancelling the effect out a bit further.
Conclusively, even if you do not couple the speaker to a virtually infinte mass (y) the effect of the speaker moving is utterly neglegible!
So, question is, how to virtually shoot the speaker into orbit? A soft stand, springs, foam the like, but how soft?
Basically this question can be answered by application of very basic high school knowledge. But I won't explicate the calculations, just believe me, nobodies life depends on it.
Get some suspension, a sponge, springs, felt, what have you. If the speaker box, seated on that suspension sinks in by about 1mm, and is still a bit wobbley, then the suspension is sufficiently soft, regardless of the weight of the speaker, to simulate orbital freedom.
Another word of caution. For some mysterious reason audiophiles behave uninformed if they, what they do, use more than three 'spikes'. This makes rattle, necessarily and practically cannot be prevented, whatever one does!
Do we have an agreement that you and others please won't hurt themselves anymore? Don't try to hammer a nail into a wall with the naked fist of audiology.
Thank you so much!
(courtesy of Europe's public education system)