Fine Points of Aiming One-box Line Arrays — II

by Richard Honeycutt

Fine Points of Aiming One-box Line Arrays – Richard Honeycutt looks at practical aiming considerations.

The directionality of any sound source changes with the distance from the source. Close to the source — in the “near field” — the directivity does not match the simple approximations we usually use to predict coverage; these approximations are valid only in the “far field”. In the near field, SPL drops off at a lower rate than the 6 dB per doubling of distance we see in the far field (assuming anechoic conditions). The transition from near-field to far-field behavior is frequency-dependent, and occurs at a distance given by r > or =8a2/λ, where r is the distance from the source, a is the width (for horizontal directivity considerations) or height (for vertical directivity) of the source, and λ is the wavelength. [Introduction to Electroacoustics and Audio Amplifier Design, by W. Marshall Leach, Jr., Kendall/Hunt Publishers, 1998, p. 37]. Beranek adds that r must be a minimum of 3 times the source diameter [Acoustics, McGraw-Hill, 1954, p. 100.]

Pat Brown gives more thorough discussion in http://www.synaudcon.com/site/author/pat-brown/far-field-criteria-for-loudspeaker-balloon-data/.

For a 15″ speaker, these conditions indicate the transition to far field is the greater of about 45″ (Beranek condition); or 23.3″ ( Leach equation at 100 Hz), 19.4′ ( Leach equation at 1 kHz), or 194′ ( Leach equation at 10 kHz). Pat’s article includes a convenient table to allow you to avoid calculations. Using the table, we see that for a 4′ one-box line array, the vertical directivity settles to far-field conditions at about 30′ for frequencies of 4.2 kHz and below.

Two types of one-box line arrays provide reduced effective dimensions for the source at higher frequencies. The Bessel array uses LC circuits to taper the response from full-range in the center to only low frequencies at the ends. Most steerable arrays perform the same sort of frequency tapering by internal digital filtering. This reduces the transition distance.

The bottom line is that you can’t count on actual devices matching the theoretical performance if the listeners are close to the line array. Or in somebody’s words (the experts disagree as to whose words): in theory, theory and practice should be the same, but in practice, they’re not. This fact shows up in the shape of the level graph for a Renkus-Heinz IC16 at 1 kHz (Figure 1), which does not smooth out until the distance reaches about 40′.

Figure 1: Renkus-Heinz IC-16 Single Beam at 1 kHz

Figure 1: Renkus-Heinz IC-16 Single Beam at 1 kHz

Another fine point about line arrays that is not always appreciated is that the frequency response varies with distance from the array. This makes sense if you remember that the SPL variation with distance changes with frequency. Figures 2 and 3 illustrate this variation for an SLS LS-8695. (The vertical axis is marked in 5-dB increments; the horizontal axis, in 1/3-octave increments.)

Figure 2: SLS LS-8695 Frequency Response at 23' on Axis

Figure 2: SLS LS-8695 Frequency Response at 23′ on Axis

Figure 3: SLS LS8695 Frequency Response 48' on Axis

Figure 3: SLS LS8695 Frequency Response 48′ on Axis

In a closed room, this variation will be less noticeable than it looks, since the wide horizontal coverage of the line array ensures abundant sidewall reflections so that the reflections and reverberation even out some of the gaps that show in the direct field at great distances.

In Part III of this blog series, we’ll look at some unintended consequences of beam steering and at the interaction between choice of aiming and the architecture of the room.