The Vox Olympian is a 4-way horn-loaded satellite: midbass horn, midrange horn, high-frequency horn, and a super tweeter horn. When paired with the optional Vox Elysian sub-bass units (each with dual 12" drivers front-loaded by a 4.6 m folded exponential horn), the system becomes effectively a 5-way all-horn design. By contrast, the Trio G3 is a 3-way horn satellite, with optional bass modules that can be horn-loaded (Basshorns/SpaceHorns) or conventional (Sub 231). The claim that the Olympian has “only two horn-loaded ways” is incorrect, and it’s equally misleading to imply the Trio always uses “conventional” bass , it depends entirely on the bass module selected.
Hello Kozak, very interesting.
To be honest, I didn’t know that a 460 cm folded ‘horn’ is being used here.
I have a few comments about that
In acoustic horn design, the geometry of the flare (the way the cross-section expands along the horn axis) is critical for predictable sound radiation and efficiency.
Exponential law of area growth. In a true exponential horn, the cross-sectional area follows
S(x) = S_0 \, e^{mx}
where S_0 is the throat area, m the flare constant, and x the distance along the horn length.
For a horn of 460 cm length, the area expansion is continuous and smooth from throat to mouth. This ensures that the acoustic impedance gradually transforms from the driver to free air.
Impedance matching and cutoff frequency.The exponential profile produces a well-defined cutoff frequency f_c = \frac{m c}{2\pi}, below which the horn loses efficiency.
A straight-line approximation (polygonal flare) introduces discontinuities in the rate of expansion. These act as acoustic mismatches, generating reflections inside the horn. As a result, the effective cutoff becomes less precise and resonances may occur.
Reduction of internal reflections. Every sharp change in flare angle (as occurs when substituting curved walls with flat boards) creates partial reflections.
In a 460 cm long horn, even small reflections accumulate, producing standing waves and colorations in the mid-bass and lower midrange. The exponential curve minimizes this problem by ensuring continuous impedance transition.
Frequency response and directivity
A true exponential curve yields a smoother low-frequency roll-off and a more predictable radiation pattern.
Straight-line segments approximate the exponential law only roughly; this causes ripples in frequency response and less controlled directivity, especially around the horn’s cutoff region (which, for a 460 cm horn, is typically in the range of ~18–25 Hz depending on flare constant).
Perceptual effect
To the listener, a horn with the correct exponential contour delivers cleaner bass, reduced coloration, and higher efficiency.
A straight-panel approximation may still produce strong output, but with audible irregularities: boominess, uneven tonal balance, or “honkiness.”
In summary: A true exponential 460 cm horn ensures smooth acoustic impedance transformation, minimizes reflections, and produces a cleaner, more natural sound compared to a horn that only imitates the exponential shape with flat, straight segments.
In light of these facts, the sonic result that is delivered should be rated even higher.