| Line Array Principles – for the Mathematically Minded |
| By Engineering Director Bill Webb Early in 2002, Martin Audio entered the competitive line array market with the W8L. One year on, its compact sibling — the W8LC is about to enter production. This article explains how, in parallel with actual product development, the Engineering Department at Martin have been developing mathematical tools that can predict line array performance and give a greater insight into how line arrays really work in practice. WHAT IS A LINE ARRAY?
The principle of configuring a
vertical column made up of closely-spaced loudspeakers has been around
for decades. Because of increased coupling, line arrays increase directivity
in the vertical plane and produce a narrow vertical beam, while the horizontal
coverage remains the same as for a single device.
The increased coupling is due to:
1. Much smaller distances between
each element (either horn or direct radiator), and
2. Much flatter wavefronts produced
by those elements.
To illustrate this, the difference
between three closely spaced horns and three horns spaced 1m apart is
shown in Figs 1a and 1b.
![]() Fig 1a: W8L 3 x 1” HF
at 8kHz (vertical dispersion)
![]() Fig 1b: Three 30º horns
1m apart at 8kHz (vertical dispersion)
In straight line arrays, this increased
directivity can result in coverage angles of less than 1 degree at high
frequencies. Whilst this narrow beam might be fine for aiming voice announcements
in transportation facilities, it is of little use in live performance
applications where both the audience and tour manager demand high quality
sound in every seat.
To achieve the wider vertical pattern
required to cover an audience area, practical line arrays are nearly always
physically curved in the vertical plane. Curving the array in this manner
has very important implications for the design and use of practical systems,
and challenges some of the simplistic ideas associated with first generation
line arrays.
3dB OR 6dB PER DOUBLING
OF DISTANCE?
In line array folklore, much has
been made of the notion that a line array produces a cylindrical wavefront
with an output that falls off at 3dB per doubling of distance rather than
the 6dB associated with a spherical wavefront. The increased throw gained
by extending the ‘cylindrical’ nearfield out to a greater
distance has been promoted as one of the key benefits of line array technology.
There are two problems with this
notion. The first is that, if it were true, a cylindrical wavefront would
require a floor to ceiling column in a typical stadium to cover both the
floor and the highest seat.
The second is that only an infinitely tall line could produce such a cylindrical wavefront. The wavefront produced by a line source with a finite length will only approach ‘cylindrical’ for a certain distance, after which it will disperse in the vertical plane. This distance will depend on the length of the line and the frequency. Theoretically, with a continuous array 3m high the transition from 3dB to 6dB will occur at the following distances:
100Hz 500Hz 1kHz 5kHz
10kHz
1.3m....6.5m
...13m.. 65m..
130m
While perhaps of academic interest, this effect is largely useless as it only really comes into play at high frequencies. Also, if we remember that in a straight line array the vertical coverage may be less than 1 degree, it is clear that only a very few members of the audience could ever benefit from such a narrow beam. In fact, whilst many believe it to be a key feature of line array, the cylindrical wavefront notion has little or no practical value.
CURVING THE ARRAY
Given that the line array must be curved in the vertical plane to cover the entire audience, we needed a way of determining exactly what shape of curvature was necessary to achieve the desired coverage for a particular venue. Since this question was much too
complex to be answered by simple reasoning alone, we embarked on the development
of a computer model, incorporating the acoustic and electro-mechanical
characteristics of each individual low, mid and HF element and with each
element driven by a virtual crossover. The phenomenon of air absorption
of high frequencies over distance was also taken into account.
To validate the model 12 WL8HF
horns were arranged in a line with zero splay between them as shown in
Fig 2. The SPL
was measured every 20cm on a 12m path normal to the line positioned at
the centre and the measured and predicted responses compared. Fig
3 shows that the response predicted by the mathematical model
correlates very well with the measured response.
Fig 2: Validation set-up
Fig 3: Comparison of model
prediction vs measured response
With this model, it was possible
to predict the frequency response curves at various points in the audience
and use the results to optimise the curvature of the array. In nearly
all cases, the computer model yielded a progressive curvature array profile
(Fig 4), where the curvature increases
gently and gradually going down the array. This produces a more consistent
frequency response from front to rear seats than J-shaped arrays (Fig
5), having a straight section at the top and
a curved lower section.
Fig 4: Progressive Curvature Array
Fig 5: J-Shaped Array
FRONT OR REAR HINGE?
Not only is it important to curve
the array correctly in order to achieve consistent frequency response
at any point in the audience, the position of the hinge point is also
important. The W8L and W8LC hinge points are at the front of the cabinet
which keeps the spacing between each cabinet the same, irrespective of
splay angle. This makes a significant difference as splay angle increases,
usually toward the bottom of an array (Fig
6). With a hinge point at the rear, as in some
first generation line array systems, noticeable drops in output occur
towards the upper end of the frequency spectrum when the listener is in-between
cabinets (Fig 7).
Fig 6: Front hinge, 8 cabinets 5.6kHz ![]() Fig 7: Rear hinge, 8 cabinets
5.6kHz
POPULAR MISCONCEPTIONS
–
WAVEFRONT CURVATURE AND STEP DISTANCE BETWEEN DRIVERS As well as the cylindrical/spherical
argument, which has little or no practical value in real-world line arrays,
other ideas which have found their way into line array folklore include
so-called criteria for wavefront curvature and the step distance between
sources.
Contrary to popular belief, a perfectly
flat wavefront is not essential and can indeed cause problems in curved
arrays where the situation is complex and important trade-offs have to
be made.
Too much wavefront curvature will adversely affect coupling and therefore output at the top of the array where there is typically very little or no splay between each cabinet. No wavefront curvature will give noticeable high frequency hot-spots where inter-cabinet splay angles are large, typically in the short throw region at the bottom of the array. This is made much worse when the hinge point is at the rear of the cabinet. The acoustic devices within the W8L and W8LC generate low curvature wavefronts, which, together with the advantages of a front hinge point, provide a combination of excellent projection over distance and smooth coverage right up close to the array. The other so-called ‘criteria’ regarding what constitutes a line array calls for the step distance between drivers to be less than a wavelength at the highest frequencies. This is one area where the performance of horns
and direct radiators differ: a horn can be driven by drivers which are
greater than one wavelength apart at the highest frequency that they
reproduce and still produce a low curvature wavefront, as shown in Fig
8. ![]() Fig 8: W8L mid horn –
measured wavefront curvature @ 2.5kHz
Using specially-designed toroidal
phase bungs (patent pending), which act in conjunction with the shape
of the horn flare, the W8L mid horn produces a low curvature wavefront
in the vertical plane, all the way to the upper end of its passband. Note
the curvature from left to right is due to the 90º horizontal dispersion
of the horn.
VIEWPOINT
Fig 9: ViewPoint During the summer of 2002, the
progressive curvature rules established by the mathematical model were
built into ViewPoint (Fig 9),
a proprietary Martin Audio optimisation programme. Venue dimensions and
number of cabinets are entered into ViewPoint, which will automatically
optimise the curvature of the array to suit the venue. Designs can be
saved to disk and printed out ready to give to the crew assembling the
array.
AIR ABSORPTION AND BAND
ZONING
Whilst line arrays have greater high frequency output capabilities than cluster based systems, all sound systems are still limited by the phenomenon of air absorption, which is a function of temperature, humidity, atmospheric pressure and frequency (Fig 10). The relationship between these quantities is quite complex, but losses always increase as frequency rises and distance from the source increases. Note this effect is in addition to the overall SPL loss as distance increases. For instance, weather conditions
can attenuate output at 8kHz by 12dB at a distance of only 50m from thesource.
On another day the same system could throw over 200m!
![]() Fig 10: Temperature and humidity
effects
To offset the affects of air absorption,
progressively more EQ is required as the distance from the array increases.
Since air absorption primarily affects high frequencies, it is of most
benefit to split the drive to the HF devices into a number of separate
channels (typically three) so that optimal EQ can be added to suit the
requirements of the short, medium and long throw sections of an array.
By using this ‘HF band zoning’,
people near the front don’t have to listen to the extra EQ that
the people at the back must have in order for them to hear high frequencies
adequately. This simple technique helps to deliver remarkably consistent
sound quality over the whole audience (Fig
11).
Fig 11: HF band zoning accurately compensates for air absorption CONTROLLER PRESETS
Up to now, it has been common practice
to use a single digital controller preset or analogue crossover for a
particular loudspeaker system, with users adding their own preferred EQ
and crossover tweaks.
Whilst the simplicity of this approach may have some appeal, line arrays benefit greatly from specific controller presets that take into account variables such as line length and degree of curvature. Using our mathematical model, we
have determined a family of presets that are optimised for different array
configurations, curvatures and also take into account the highly variable
effect of air absorption.
The presets are called up by ViewPoint
during the array design process and ensure consistent sound quality over
the whole audience whatever the size or shape of the array and atmospheric
conditions prevailing on the day.
SUMMARY
The
development of a mathematical model that will predict line array performance
has brought a greater insight into the ways that real-world, touring line
arrays actually work. It has also provided the basis for everyday, practical
tools such as ViewPoint and the band zoning techniques that enable
users to get consistently good performance out of the W8L and W8LC in
all configurations and atmospheric conditions.
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