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Understanding Sound System/Room Interactions

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As an alternate approach to trying to find a measurement that correlates with what we hear, we can try using a longer time window to “see” the LF response with better resolution. A longer time window of approximately 250 msec is shown in Figure #4.


Figure #4: The impulse response of a 1250 seat multipurpose hall. The vertical lines suggest a time window that INCLUDES most of the effects of the room. The time window shown is approximately 0.25 seconds.

To transform this longer “slice” of the impulse response into the frequency domain, we will use an 8k FFT which represents 8K/48000 seconds or 0.171 seconds. Notice again that this time window includes both the direct sound and the response of the room.

In Figure #5 the low frequency information is seen in adequate resolution, however the high frequency results look confusing. The plot shows data that has 5 Hz resolution (i.e. one data point every 5 Hertz). While this resolution provides excellent LF resolution (between 31 Hz and 62.5 Hz there are 15 data points. However at HF we have excessive resolution - between 4kHz and 8kHz there are approximately 800 data points. Simply stated, the longer time window provides good LF resolution, but excessive HF resolution.


Figure #5: The frequency response of the direct sound portion of an impulse response of a 1250 seat multi-purpose hall. The response was calculated using a 8192 point FFT (which equals a 8192/48000 or ~107 msec). As you can see the frequency response shows low frequency energy that is much more pronounced than seen with the shorter time window.


The result of studying these plots might lead you to conclude that in order to make measurements that correlate well with our listening experience, we must use very short time windows that isolate the direct sound at high frequencies, and increasingly longer time windows as we look at lower frequencies. At first glance this idea might seem to violate the often quoted phrase, “One can only affect the direct sound with processing.” However this is not the case. At mid-low and low frequencies, the interaction of a sound system and a room can be affected and optimized by signal processing. In other words, at low frequencies (long wavelengths) the direct sound and reflections from nearby surfaces combine to form a composite response. It is this composite response that a listener hears.

The ability to measure several time windows simultaneously provides a measurement that both correlates well with human hearing and provides insight into how the signal being sent to the loudspeaker can be tailored (via equalizers, or other processing) to optimize the loudspeaker/room interaction.

Our last figure shows a measurement of a loudspeaker system that includes multiple time windows and displays both the magnitude and phase response of the “system.”


Figure #6: This frequency response was calculated using a multi-windows transfer function. One result of this is the trace has equal resolution (24 data points) in each octave from 20 Hz to 20 kHz, and is therefore call a Fixed-Point-Per-Octave or FPPO transfer function. Both magnitude and phase traces are shown.

Conclusion: The use of multiple time windows allows one to isolate the direct sound of a loudspeaker in a real-world situation at high frequencies. However at lower frequencies longer time windows that include the loudspeaker/ room interaction have been found to correlate well with our listening experience. The use of multiple time windows in a single measurement is an extremely interesting way to measure and optimize the response of a sound system in a room.


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