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Experiment A: Schematic of the reverberation chamber containing the suspended Aluminium plate. TSEA subsystem numbers are shown in brackets.

Experiment A: Schematic of the reverberation chamber containing the suspended Aluminium plate. TSEA subsystem numbers are shown in brackets.

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This paper forms the second part of two companion papers on the use of Transient Statistical Energy Analysis (TSEA) to predict maximum time-weighted sound pressure and vibration levels in built-up structures. It focuses on experimental validation of the TSEA modelling procedures defined in Part 1. Two experimental designs are used to ensure the val...

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... wo-subsystem TSEA model is formed by a4 .8 mm thick Aluminium plate (subsystem 1) that wass uspended by elastic cord in the centre of a1 22 m 3 reverberation chamber (subsystem 2).As chematic of the experimental set-up is shown in Figure 1w ith details for the twos ubsystems giveni n Table I. These twos ubsystems were chosen as theyb oth had very lowinternal loss factors which could be systematically increased by the application of damping material onto the plate and the placement of absorptive material into the room. ...
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... is nowp ossible to investigate the effect of different damping conditions on the response of the subsystems in Experiment Aa ss hown on Figure 10. Fort he three different room damping conditions there is close agreement between maximum velocity levels predicted using TSEA and the average measured values. ...
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... stage of the validation concerns TSEA prediction of the maximum sound pressure leveli nar everberant room due to ap late that is mechanically excited by at ransient force. Forexperiments Aand B, the measured and TSEA predicted maximum sound pressure levels are shown in one-third octave bands in Figure 11 and Figure 12 respectively. From Experiment A, Figure 11 shows the measured and TSEA predicted maximum sound pressure levels in the partially damped room (subsystem 2b)w ith excitation of the partially damped Aluminium plate (subsystem 1b). ...
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... stage of the validation concerns TSEA prediction of the maximum sound pressure leveli nar everberant room due to ap late that is mechanically excited by at ransient force. Forexperiments Aand B, the measured and TSEA predicted maximum sound pressure levels are shown in one-third octave bands in Figure 11 and Figure 12 respectively. From Experiment A, Figure 11 shows the measured and TSEA predicted maximum sound pressure levels in the partially damped room (subsystem 2b)w ith excitation of the partially damped Aluminium plate (subsystem 1b). ...
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... Aand B, the measured and TSEA predicted maximum sound pressure levels are shown in one-third octave bands in Figure 11 and Figure 12 respectively. From Experiment A, Figure 11 shows the measured and TSEA predicted maximum sound pressure levels in the partially damped room (subsystem 2b)w ith excitation of the partially damped Aluminium plate (subsystem 1b). The results showg ood agreement (i.e. ...
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... agreement occurred with other combinations of damping conditions. From Experiment B, Figure 12 shows similarly close agreement between TSEA and measurements for the 140 mm concrete floor.These experiments confirm that steady-state coupling loss factors that are used in SEA for sound radiation can also be used in TSEA to predict maximum sound pressure levels when the time interval is chosen as described in Part 1o ft his paper in section 2.4 [1]. Figures 11 and 12 also provide evidence that close agreement can be obtained between TSEA predictions and measurements when TSEA uses either ameasured, hybrid or synthetic transient power input. ...
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... final stage is to investigate the effect of different damping conditions in Experiment A. Figure 13 shows close agreement between measured and TSEA predicted ACTA ACUSTICA UNITED WITH ACUSTICA Vol. 100 (2014) maximum sound pressure levels due to transient excitation of the plate for different room and plate damping conditions. The TSEA predicted levels tend to lie within the 95% confidence intervals of the measurements. ...
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... underlying reasons for the differences between the undamped and damped plates in Figure 13 are likely to be due to acombination of (a) the smearing effect of the Fast time-weighting and (b) the energy balance during the time period in which the maximum sound pressure levelisdetermined. The latter aspect can be considered using TSEA. ...
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... latter aspect can be considered using TSEA. Fort he damping conditions shown in Figure 13, the time period during which the maximum sound pressure level is determined (measured or predicted)v aries between 0.2 and 1s.T og ives ome insight into the net power flowb etween the plate and the room during this time period it is instructive to use the time-varying modal energies from the TSEA model. This is because the net power flowtransferred between twocoupled subsystems is proportional to the difference in their modal energies. ...
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... is because the net power flowtransferred between twocoupled subsystems is proportional to the difference in their modal energies. Fort he damping conditions in Figure 13, the time-varying modal energy leveld i ff erence at 1kHz is shown in Figure 14 as the ratio of the plate modal energy to the room modal energy. The results are shown during the 1stime period after transient excitation. ...
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... is because the net power flowtransferred between twocoupled subsystems is proportional to the difference in their modal energies. Fort he damping conditions in Figure 13, the time-varying modal energy leveld i ff erence at 1kHz is shown in Figure 14 as the ratio of the plate modal energy to the room modal energy. The results are shown during the 1stime period after transient excitation. ...
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... stage of the validation concerns TSEA prediction of the maximum velocity leveldue to structure-borne sound transmission from as ource plate to either an adjacent or non-adjacent receiving plate using the heavyweight building from Experiment B. The maximum velocity levels are predicted with TSEA using ameasured transient power input because it wass hown in section 3t hat the accuracy is similar to that for hybrid and synthetic transient powers. The measured and TSEA predicted maximum velocity levels are shown on Figure 15a and 15b for adjacent plates and Figure 15c for non-adjacent plates. In all cases there is good agreement between measurements and TSEA, with at endencyf or TSEA to underestimate by up to 5dBi n the mid-and high-frequencyranges. ...
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... stage of the validation concerns TSEA prediction of the maximum velocity leveldue to structure-borne sound transmission from as ource plate to either an adjacent or non-adjacent receiving plate using the heavyweight building from Experiment B. The maximum velocity levels are predicted with TSEA using ameasured transient power input because it wass hown in section 3t hat the accuracy is similar to that for hybrid and synthetic transient powers. The measured and TSEA predicted maximum velocity levels are shown on Figure 15a and 15b for adjacent plates and Figure 15c for non-adjacent plates. In all cases there is good agreement between measurements and TSEA, with at endencyf or TSEA to underestimate by up to 5dBi n the mid-and high-frequencyranges. ...

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