Dear Duke,
I share your view that the exact measurement method for sensitivity specifications is crucial, and you haven’t misunderstood me. Let me address this step by step and elaborate, based on standardized acoustic principles.
First, regarding sensitivity measurement: Nominal values (e.g., 95 dB/1W/1m) are typically determined axially (i.e., in the main radiation direction) at a distance of 1 meter, often with an input voltage of 2.83 V (corresponding to 1 W at 8 ohms). The level is measured as an average over a frequency range (e.g., 250 Hz to 4 kHz), assuming hemispherical radiation (solid angle 2π sr, directivity index Q=2). Manufacturers ( Of course, assuming the manufacturer actually conducts these measurements and is willing to publish them).rarely inflate these values artificially, as they are standardized according to norms like IEC 60268-5 – the contribution of room reflections is explicitly excluded to ensure comparable conditions. In practice, this leads to deviations in a real room, as reflections influence the overall level at the listening position.
This is precisely where the point about reflections comes into play, which you so aptly addressed: With the same axial level (e.g., 95 dB for the horn vs. 98 dB for the cone loudspeaker), a conventional cone/box loudspeaker indeed has a broader radiation pattern (often nearly omnidirectional in the midrange), leading to stronger diffuse reflections. These reflections add to the direct sound and increase the measured level at the listening position – theoretically by up to 6 dB in a typical room (depending on distance and room geometry), as sound pressure in rooms decays less rapidly than in free-field conditions. However, this “additional level” often doesn’t translate into a pure loudness increase but rather as a diffuse “veil” that reduces clarity: Early reflections (under 50 ms) can cause phase shifts, while later ones blur transient contrast.
With horn loudspeakers, it’s different: Their directivity (narrower radiation angle, often 60–90° horizontally) focuses the sound more toward the listening position and excites the room less – fewer diffuse reflections mean less “background noise.” As a result, the pure direct sound level achieves a subjectively higher presence and clarity, making the horn appear louder and more detailed despite its lower nominal sensitivity. In a real listening room, this can even outperform a cone loudspeaker with a 3 dB higher rating, as the listener contends less with room reverberation.
And yes, you hit the nail on the head with dynamic contrast! Increased reflections often behave like masking noise, obscuring quiet passages and subjectively reducing the overall dynamic range (typically 60–120 dB in music) – similar to a concert hall, where controlled, spectrally correct reflections (e.g., from the ceiling) preserve contrast, but diffuse wall reflections diminish it. Horns minimize these uncontrolled contributions, making them particularly advantageous in acoustically challenging rooms (e.g., with hard surfaces). Of course, this depends on the specific horn design (e.g., Constant Directivity vs. classic) and room acoustics – a measurement with an SPL meter or REW software would best demonstrate this.
Beat Regards S.