Handbook for Sound Engineers

(Wang) #1
Loudspeakers 637

requiring less woofer excursion for a given acoustic
output in the lowest portion of its usable bandwidth. In
general, a sealed system will have more highly damped
low-frequency transient response when compared to a
vented system with the same cutoff frequency. This effect
is most noticeable for frequencies in the neighborhood of
the system lower cutoff frequency.
The design and modeling of vented and sealed
woofer enclosures has been greatly simplified in recent
years due to the ready availability of computer software
developed specifically for the purpose. The following
Thiele-Small (in honor of A. N. Thiele and Richard
Small) loudspeaker parameters are required as
minimum input to an enclosure design program:


  1. QT is the total loudspeaker Q.

  2. FS is the free-air cone resonance of the loudspeaker.

  3. VAS is the equivalent volume compliance of the
    suspension.

  4. Xmax is the maximum linear excursion.

  5. Pmax is the maximum thermal power handling.


Most manufacturers provide the above parameters as
per Audio Engineering Society (AES) recommended
practice on loudspeaker specifications.


Loudspeaker enclosures can have resonances, or
standing waves, caused by internal reflections. The
characteristic frequencies (fb) of these standing waves
are given by:


(17-26)

where,
x, y, and z are the three box dimensions,
l is the designated dimension of the box,
n takes on all possible integer values (n = 0, 1, 2, 3,...).

If the lowest modal frequency found by setting n=0
for all but the longest box dimension is above the band
of use, there will be no standing waves inside the enclo-
sure. In the more common case of a woofer being used
above the first mode frequency, acoustic absorption can
be added to damp these unwanted resonances. It should
be understood that the addition of large amounts of
damping material can have an adverse effect on the
box/port tuning, so a balance must often be struck
between control of standing waves and optimal low
frequency response alignment.

17.10.2.3 Measurement of Thiele-Small Parameters

The most accurate way of determining fS is by observa-
tion of a Lissajous pattern on an oscilloscope of voltage
versus current with the speaker in free air. When the
pattern collapses to a straight diagonal line, the phase of
the impedance is zero, which indicates resonance. Once
this condition has been achieved, the frequency should
be measured with a frequency counter that is accurate to
0.1 Hz or better.
VAS may be determined with the loudspeaker
suspended in free air as follows:


  1. Find total moving mass (m) by attaching an extra
    mass (MX) to the cone (as close to the voice coil as
    possible) and observing the new resonant frequency,
    fSX. MX can be putty or clay; measure mX accurately.
    The total mass can then be found by the equation


(17-27)


  1. The suspension spring constant is then


(17-28)


  1. From the effective diaphragm area of the loud-
    speaker, SD, VAS is given by


(17-29)

One means for determining the effective diaphragm
area is to excite the woofer near its resonant frequency
and observe its motion using a strobe light tuned almost,
but not exactly, to the frequency of excitation. The
resulting apparent slow motion of the woofer will allow
an accurate determination of the portion of the cone that
is moving.
QT may be found using the following procedure:


  1. Determine the impedance of the woofer, Zmax, at its
    resonant frequency. This is simply the applied
    voltage divided by the current in the coil.

  2. Identify the frequencies, f+ and f–, above and below
    fs, respectively, at which the magnitude of the
    applied voltage divided by the magnitude of the
    current in the coil is equal to.

  3. Mechanical Q is given by


(17-30)


  1. The total Q is then


fn c
2

---

nx
lx
©¹§·---- -

(^2) ny
ly
©¹§·-----
(^2) nz
lz
©¹§·----
2
= ++
mc
Mx
fS
fSX




©¹
§·
2
1–
=------------------------
k= 2 Sfs^2 mc
VAS
U 0 c^2 SD^2
k
--------------------=
Qm
f 0
f+–f


©¹
̈ ̧
§·Zmax
Re
= -----------

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