Page 211 - The Master Handbook Of Acoustics
P. 211

186   CHAPTER NINE



                                   bothersome reflections from walls and other surfaces to arrive at the
                                   measuring position. If the pulse is short enough, the time gate can be
                                   opened only for the desired sound pulse, shutting out the interfering
                                   pulses. This  tone-burst method can be used to measure the sound-
                                   absorption coefficient of a material at any desired angle of incidence.
                                      Such an arrangement is illustrated in principle in Fig. 9-5. The
                                   source-microphone system is calibrated at distance x as shown in Fig.
                                   9-5A. The geometry of Fig. 9-5B is then arranged so that the total path
                                   of the pulse reflected from the material to be tested is equal to this
                                   same distance x. The strength of the reflected pulse is then compared
                                   to that of the unreflected pulse at distance x to determine the absorp-
                                   tion coefficient of the sample.
                                      A recent surge of interest in the influence of individual reflections
                                   on the timbre of sound is a new and promising development in
                                   acoustics. In this new field specific normal reflections, called “early
                                   sound,” are of special interest. Although random-incidence coeffi-
                                   cients are still of interest in room reverberation calculations, for these
                                   image control problems normal-incident reflection coefficients are
                                   generally required. Thus, interest may be returning to normal (right-
                                                              angle) coefficients obtained by the reso-
                                                              nance-tube method. There may even be a
                                                              renewed interest in the old “quarter-wave-
                                                       A      length rule” in which the porous absorber
                                                              for normal incidence must be at least a
                                                              quarter wavelength thick at the frequency
                                       x
                                                              of interest. For example, for a frequency of
                                                              1 kHz, the minimum absorber thickness
                                                              should be about 3.4″.
                                     Barrier
                                                              Mounting of Absorbents

                                   x        x
                                   2        2          B      The method of mounting the test sample
                          Sample                              on the reverberation chamber floor is
                                                              intended to mimic the way the material is
                     FIGURE 9-5                               actually used in practice. Table 9-1 lists
                                                              the standard mountings, both in the old
                   Determining the absorption coefficients of materials
                   by a tone-burst method. The source-microphone sys-  form and in the ASTM form that will be
                   tem is calibrated at distance X as shown in (A).  used in the future.
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