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Realizing a Full Bandwith Line Array

Full bandwidth line arrays are typically three way systems.

The practice of dividing the band into 3 separate passes is
done to enable the cross-over points to always be substantially
low enough that the radiation from each pass exhibits wave-
lengths that are always longer than the physical device, or driver
spacing. This is relatively easy to achieve for the low frequency
section of any line array and is also easy to achieve for the
mid-band section. 

In mid-band sections the mid range devices are 6 inches

in diameter to 8 inches in diameter. The crossover points are
selected so that the device spacing is always small compared
to the wavelength radiated. The problem for a full bandwidth
line array systems is the high frequency radiation. 

As mentioned earlier, historical line arrays were excellent

in terms of low frequency and mid-band control of the pattern,
but always suffered from polar lobing errors associated with
the device space “B” being greater than the wavelengths being
radiated. A 16 kHz wavelength is on the order of 3/4 of an
inch and as a consequence device spacing must be comparable
to those wavelengths or shorter, if possible. This was always 
a problem in the past because engineering techniques could
not realize spacing closer than the driver diameters themselves.
Even with modern neodymium iron boron based magnetics, 
the diameters were always at least 4 inches or greater (for
large format diaphragm devices). That spacing limited good
performance to below approximately 3 kHz, obviously not a full
bandwidth device.

As a practical example, fmax, the maximum high frequency

control based on the relationship between the spacing of the
devices b and the wavelengths is as follows. For base line
arrays where we are interested in control up to 250 hz, the
spacing needs to be at least 4.5 feet. This is relatively easy 
to do with 15 inch and 12 inch drivers and as a result the real-
ization of bass frequency line arrays is very straightforward. 

For mid-band line arrays, if we are interested in frequencies
between 250 and 1,250 hz, the spacing needs to be 11 inches
or smaller. Again, this is relatively easy to do with 6 inch or 
8-inch drivers, and this is frequently the diameter of mid range
devices in both large format and compact line array systems. 

Figure 27

shows an Electro Voice Hydra™. This device

basically takes the radiation of a compression driver and acts
to produce both equal amplitude and equal phase sources at
the front of the wave-guide. The full drawing in 

Figure 27

is 3

Hydras vertically stacked, thereby generating 21 “point source”
radiating surfaces coupled to a horizontal wave guide with an
included angle varying between 90 and 120 (model dependent).

Figure 28

shows a Hydra without the driver or wave-guide

coupled. Each hydra has 7 output “slots”. The driver is coupled
to the input side of the hydra and the 7 outputs are then
interfaced with a horizontal wave-guide to produce the
required horizontal included angle. The space b for a hydra is
.826 inches, which equates to a wavelength of 16,434 Hz.
Again, it is always best for wavelengths to be longer than that
spacing, so in this implementation, the Hydra presents excel-
lent high frequency control in the 15kHz to 16 kHz range. The
Array Show plot 

Figure 29

shows 21-point sources in a vertical

orientation with the exact spacing provided by a hydra. 

Figure 27

Figure 28

Figure 29

λ

= 16,434 Hz

8

Содержание X-Line Xvls

Страница 1: ...gure 3 that a high frequency horn was employed above that frequency limit in order to achieve appropriate extended bandwidth and fidelity up to and beyond 10 kHz This is a classic embodiment of a limited bandwidth line array and as we shall see in this presen tation only recently have solutions been brought to the state of the art to enable line array technology to truly be full band width and ext...

Страница 2: ... high frequency relates to wavelengths that are much shorter than the dimensions of the radiating source Figure 6 is an Array Show representation of a theoretical simple source As can be seen from this slide the radiation is purely omnidirectional implying that any wavelength radiated is always long compared to the dimensions of the radiating device It is common in sound reinforcement practice to ...

Страница 3: ...lustrate the principles underlying successful application of a continuous line of vertical sources that of a line array Figure 12 is extremely interesting as well as it explains the historical applications where line arrays were limited bandwidth devices such as those referenced in Figure 1 Figure 2 and Figure 3 earlier in this discussion The two point sources continue to be spaced by 12 inches bu...

Страница 4: ...at the lobing pattern begins to suggest that spacings greater than those equal to the radiated wavelength begin producing unacceptable polar lobing errors For this reason successful application of full band with line arrays requires that the spacing always be less than the radiated wavelengths Figure 15 now takes our two point sources and begins to build a continuous vertical orientation of source...

Страница 5: ...e array overall height H must be large compared to the radiated wavelengths The device separation B and line array height H are two key parameters to describe both the high frequency limits fmax and low frequency limits fmin of a line array system The space B helps to determine Fmax the highest frequency of well behaved summing The parameter H defines Fmin the lowest frequency that the line array ...

Страница 6: ...s although producing an improved directivity index would suffer from substantial lobing errors as one walks from the x axis to the y that is walk from the front of the array toward the back of a venue covering the entire included vertical angle of the venue Figure 22 shows an Array Show plot of a point source and compares it to the Array Show plot of the directional improvements in response associ...

Страница 7: ...e velocity of the diaphragm and we generate an addi tional conversion efficiency as a result We have now illustrated two methods of achieving directional radiation that of orientation of simple sources or of coupling a horn to a radiating source An important concept at this point is to introduce the product theorem ρ r ø ρAX r He ø H ø Where He ø is the expression that describes the directional ch...

Страница 8: ... maximum high frequency control based on the relationship between the spacing of the devices b and the wavelengths is as follows For base line arrays where we are interested in control up to 250 hz the spacing needs to be at least 4 5 feet This is relatively easy to do with 15 inch and 12 inch drivers and as a result the real ization of bass frequency line arrays is very straightforward For mid ba...

Страница 9: ... in this paper with regards to vertical stacking It should be remembered by all designers that stacking whether the arrays are horizontal or vertical will always narrow the pattern in the axis that the devices are oriented This brings us back to the mid range devices and low frequency devices in an axis symmetric design These axis symmetric designs are small horizontal arrays Figure 32 shows two e...

Страница 10: ... indirectly the case The actual parameter is the physical height of the array so large format concert level line arrays like the EV X Line certainly require less boxes to get to a particular cut off frequency The important thing to note from Figure 35 is that if we average the 4 multiplier and 5 multiplier we see that a four box system in the case of a compact line array the XLC from Electro Voice...

Страница 11: ...e system Early applications of line arrays consisted of aiming the systems with a laser mounted on the top of the overall array This is very inappropriate as can be seen from any of the figures Figure 37 Figure 38 and Figure 39 Regardless of the shape whether flat symmetrical curved symmetrical or asymmetrical the major lobe always emanates from the physical center of the system and may be steered...

Страница 12: ...re 44 Although the polar pattern is partly compromised the Q is substantially increased The associated gain in directivity index is a very valuable tool for a system designer In Figure 45 shows a typical groundstack A 200 foot long room would exhibit the following performance A flow line array would generate if properly aimed a 1dB to 2 dB variation front to back in the venue described in the exam...

Страница 13: ...atching the SPL coverage versus distance in the venue with the flat array s major lobe for curved arrays the near field behavior is likely between 3dB and 6dB per doubling of distance and is very difficult to quantify It should also be noted that line arrays although offering substantial benefits are not suited for all applications A line array needs proper aiming or sub standard performance will ...

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