point source is 12 dB lower than at the usual but not very practical measuring
distance of 1 meter.
From a line source like a large electrostat, when auditioned at 4 meters, the loss is
not 12dB but 6 dB only.
An example may clarify this phenomenon:
A good cone-type loudspeaker, behaving as a point source has a “sensitivity of
86dB/watt/1 meter”. At the usual 4-meter distant listening position, the sound level
has dropped to 86 – 12 = 74 dB. A big ESL, when auditioned at the same distance
will produce a sound level of 86 – 6 = 80dB. A 6 dB difference.
The second property of ESL’s is its dipole character. A conventional speaker only
radiates to the front, as the back is usually closed by the box.
An ESL radiates its sound energy both to the front as to the rear and this rear sound
energy will be reflected to the walls and added to the waves coming from the front.
This will contribute to the overall sound level impression of the listener. Were these
two waves in phase, it would lead to an increase of 6dB. But generally this is not
the case of course. An estimation of a 3dB difference is realistic.
Let us sit down again at our listening position at 4 meters of our 86 dB/1 meter/ 1
watt loudspeaker and add the two phenomena as described above together.
The point source will yield (see above) a sound level of 86 – 12 = 74 dB at 4 meters
distance.
The long ESL will yield 86 – 6 + 3dB = 83dB at 4 meters.
This is an important 9 dB of difference at the listening position. Smaller ESL’s are
not an ideal line source, but still are dipoles with their 3 dB advantage. A smaller
ESL/86dB in this context, will yield a sound level at 4 meters of some 86 – 9 + 3 dB
= 80dB, still 6dB ahead of a point source with the same measured 86 db/1 meter/ 1
watt/2.83 volts.
When Final specifies 86 dB/1 meter/1 watt, it is measured with the standardized
method. For large ESLs one has to add 9 db to that figure: it effectively becomes 95
dB equivalent as compared to a point source: a normal cone loudspeaker. For small
ESL’s one has to add 6 dB to that figure: this effectively becomes 92 dB equivalent
in order to get the right impression of the capabilities of ESL’s versus cone
loudspeakers.
The last pitfall in interpreting the measurement results of ESL’s, has –again- to do
with its long, mostly vertical- dimensions.
When assessing the frequency characteristic at the usual distance of 1 meter, there
maybe considerable differences in distances between the microphone and the
different parts of the ESL: from the middle the distance, of course, is 1 meter. But