Lewis,
Without presuming too much technical knowledge of my own, I suspect that the opposite happens. Since the dispersion pattern of the Ohms is always (nearly) omnidirectional, there is a sense of "continuousness" to the speakers. Whatever discontinuity that might be a result of your observation seems to be subsumed by this effect. At least to my ear.
Also, I would guess that the transition may be gradual, with some frequencies being partially reproduced by both bending and pistonic motion. Such an arrangement would be akin to very low order (presumably well less than first order) crossover. Such schemes usually mask transitional issues, although they can certainly introduce other artifacts. By the time response is primarily pistonic, you may well be at a frequency low enough that most listener's sensitivity is reduced. Similarly, BTW, the cross to the tweeter is so high in frequency that -IME- most listeners will be relatively insensitive to that hand-off.
Maybe John S can comment further.
Without presuming too much technical knowledge of my own, I suspect that the opposite happens. Since the dispersion pattern of the Ohms is always (nearly) omnidirectional, there is a sense of "continuousness" to the speakers. Whatever discontinuity that might be a result of your observation seems to be subsumed by this effect. At least to my ear.
Also, I would guess that the transition may be gradual, with some frequencies being partially reproduced by both bending and pistonic motion. Such an arrangement would be akin to very low order (presumably well less than first order) crossover. Such schemes usually mask transitional issues, although they can certainly introduce other artifacts. By the time response is primarily pistonic, you may well be at a frequency low enough that most listener's sensitivity is reduced. Similarly, BTW, the cross to the tweeter is so high in frequency that -IME- most listeners will be relatively insensitive to that hand-off.
Maybe John S can comment further.