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Anechoic Chamber Free Loudspeaker Test System ---- Type 1600F |
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Technical knowledge
Comparison methods for testing frequency
response of loudspeaker under anechoic chamber free condition.
In principle, the frequency response
of a loudspeaker should be measured in an anechoic chamber. The
anechoic chamber can (1) isolating noise from outside; and (2)
eliminating reflection waves.
Because to construct an anechoic
chamber is very expensive, the following three anechoic chamber-free
methods have been developed :
(1) TDS method; (2) pulse FFT
method; and (3) Special test box method (developed by SUNLIGHT).
Amount them, the TDS method is
obsolete. The principle will not be described here any more because
now this method is seldom used. Here the methods (2) and (3), which
are common used nowadays, are compared.
All other electro-acoustic measuring
instruments use the pulse FFT method. It claims that anechoic chamber
may not be used. However, if measurement is made under free anechoic
chamber condition, a lot of disadvantages comes :
A.
The pure test space should be so large than not practical.
B.
Operator should have deeper technical knowledge. He is able to
make accurate calculation on the reflecting time. These are the basis
for correct operation.
C.
The frequency intervals at low frequencies are too large. For
midrange and woofer loudspeakers, the intervals are larger than
practical requirement. It is only acceptable for the measurement of
tweeter .
D.
Distortion can not be measured under free anechoic chamber
condition.
E.
Results are not stable because it is easy to be influenced by
the environment noise. Results may be different even under very low
background noise.
However, SUNLIGHT 1600F has not the
above shortcomings. The special design of 1600F is originated from
SUNLIGHT. This one of the inventions from SUNLIGHT.
The following description explains why
the pulse FFT method has above five shortcomings.
Pulse FFT method :
In this method, a very short voltage
pulse is fed to the loudspeaker by the instrument. The propagation
time of the direct wave of the pulsed sound from Points P to Q is
about 2.9 ms (0.0029 second). The propagation time of the reflected
wave of the pulsed sound from Points P to M to Q is about 9.2 ms. In
order to avoid the effect of the reflected wave, the sampling time of
the A/D converter must be chosen as 6.3 ms (see lower figure). Then
FFT calculations are made to derive the frequency response curve of
the loudspeaker.
According to the FFT theory, the
frequency interval should be the reciprocal of the sampling time 6.3
ms, i.e. 160 Hz. It means that the measured points which form the
curve have equal frequency interval of 160 Hz. What we know is only
limited to the frequencies of 160 Hz, 320 Hz, 480 Hz, 640 Hz, 800 Hz,
960 Hz... Nobody knows the response below 160 Hz, and at frequencies
between the neighboring points. Exactly to say, the given curve is a
smoothed segment.
To reduce the frequency interval,
the distance of the shortest reflection path (P to M to Q) should be
increased. However, this
distance is limited by the real size of the room, so that it is not
practical in most cases. In other words, the interval is very
difficult to be smaller than 160 Hz.
We can conclude that this method is
suitable only for the measurement of frequent response at higher
frequencies (e.g. > 1 kHz).
Easy to be influenced by noise
: When the
pulse FFT method is used, the pulse fed to the loudspeaker is very
narrow, that means the “Pulse Energy” is very small or the “Pulse
sound energy” generated by the loudspeaker is also very low. This is
why the measured frequency response curve is not accurate under noisy
environment.
In SUNLIGHT 1600F, entirely
different principle is used to reach the free anechoic chamber measurement. There is no above shortcomings. A special
designed test box is used in 1600F. The box isolates environment noise
considerably. With the addition of the “Tracking Filter”, the
influence of environment noise is further eliminated. These measures
ensure that 1600F can be used in noisy production line.
The Test Box 143B in 1600F has
special construction. Together with the software corresponding to the
construction of the box, the free anechoic chamber
test system is formed. Since the characteristics of individual
Test Box could not be exactly the same (e.g. slight difference in the
density of the sound absorbing material), each 143B must be calibrated
and corrected against a large anechoic chamber individually. The
calibrated result is stored in the software so that the disk of one
143B can not be used in other 143B. In other words, each 143B must use
its own attached software. It is true even for two 143Bs manufactured
in the same batch.
SUNLIGHT has a large anechoic
chamber with a height of two floors ( see the
About Us ).
Each Test Box 143B was calibrated carefully against the
anechoic chamber. It makes sure that the measured frequency response
of the loudspeakers is correct.
The frequency
response (including sound pressure sensitivity) of a loudspeaker
measured by SUNLIGHT 1600F is the same (or very close) to that
measured in a large anechoic chamber according to CNS 4784 or JIS 5531
National Standard.
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