Typical horn-loaded PA tops run Q = 10 to 30, i.e. DI = +10 to +15 dB on-axis.
DI is frequency-dependent: low frequencies stay near omni, high frequencies beam, so DI rises with pitch.
Rough rule: Q approx 25000 / (H x V), with H and V the -6 dB coverage angles in degrees.
Speed of sound = 343 m/s in air at 20 C; 10 kHz wavelength is 3.43 cm, so HF beams hardest.
Doubling acoustic power = +3 dB; perceived 'twice as loud' needs about +10 dB. Higher DI = more on-axis dB per watt.
How it works
Drive speaker with a known power; measure sound intensity on-axis at fixed distance.
Average the intensity over a full sphere around the speaker (the total power spread everywhere).
Q = on-axis intensity divided by that spherical-average intensity.
DI = 10 x log10(Q): convert the ratio into decibels.
Higher Q/DI = energy crammed into a narrow beam; lower = spread wide and even.
Real examples
Omni mic/point source: Q = 1, DI = 0 dB, sound goes everywhere equally.
PA top in a 90 x 60 horn: roughly DI +9 to +11 dB, beam aimed at the crowd.
Subwoofer at 50 Hz: nearly omni, DI near 0 dB, which is why bass leaks behind the stage.
Line array: stacks boxes to raise vertical DI, throwing level to the back rows, not the ceiling.
A speaker tucked into a wall corner gains DI for free from boundary loading (Q jumps to 4 or 8).
How it helps in live sound
Pick boxes by DI/coverage: a 90 x 40 horn over 60 x 40 puts more dB on the audience, less on walls = less feedback.
Aim high-DI tops at ear height of the back of the crowd, not the empty ceiling, to claw back gain-before-feedback.
Subs are low-DI (near omni): place them where rear spill won't matter, or build a cardioid sub array.
Higher DI = more direct-to-reverberant ratio = clearer speech in boomy rooms (halls, gyms, churches).
Read the spec sheet: look for the DI/Q vs frequency plot, not just the nominal coverage angle.
Tight HF beaming means a step off-axis can drop you -6 dB or more, so cover the whole crowd, don't over-narrow.
Everyday analogy
A bare light bulb (DI = 0 dB, lights the whole room) versus a torch beam (high DI, throws a tight column of light far down the field).
Watch out
Myth: one DI number describes the whole speaker. Truth: DI rises with frequency, so the box that's tight at 8 kHz can be nearly omni at 200 Hz.
Fun fact
Putting a speaker flush in a wall doubles its directivity for free: half-space loading sends Q from 1 to 2, a clean +3 dB on-axis with zero extra power.
Key takeaways
DI (dB) = 10 x log10(Q); omni = Q1 = 0 dB; every Q doubling = +3 dB.
High DI = tight beam = more level on the crowd, less on walls and ceiling.
High DI raises direct-to-reverberant ratio = clarity + more gain-before-feedback.
DI climbs with frequency: HF beams, LF/subs stay near omni.
Boundary loading (wall/corner) boosts DI for free: half +3, quarter +6, eighth +9 dB.
Choose and aim speakers by coverage angle/DI to match the audience shape.