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CATT Acoustic could be described as a room acoustic prediction program, based on the image source model. We started with creating a simple shoebox-shaped room in CATT-Acoustics, with the dimensions: h = 8, d = 25 and w = 25 [m] (providing a total volume of 5 000 m^3):

Our shoebox-shaped room

In the first part of our task, we should vary the absorption properties in our room in order to achieve different reverberation times. As a sound source, we used three anechoic sound files (speech, drum and guitar - as in the Matlab task). Then, one of our CATT models was selected and the distance to the sound source was varied in three steps.

We continued with one of the (mono) impulse responses and its reverberant part of the impulse response was delayed and the impulse response was auralized in order to investigate the subjectively perceived diffusivity of the sound.

Investigation of the room's reverberation time..

By changing absorption coefficient of the plates in our room, five different reverberation times, RT, between 0.3 to 2 s in the 1 kHz octave band were obtained. The frequency dependence of the absorption coefficients were also set differently between the special cases. Diffuseness of the reflections were set to the default 10 %. The impulse respons for each of these rooms' settings was convolved with speech, drum and guitar music. The source was placed in one corner and the receiver in about the middle of the room (please note, not exactly in the middle).

The sound files sounds very different when played through the different rooms. The first case with RT = 0.3 s sounds like a anechoic room. Also the apparent size of the room changes, for example listen to the difference between 0.7 s drum and 1.0 s drum where the echo is first heard in the drum sound and then with RT = 1.0 s we hear a clear fluttering instead.

Perceived reverberation time as a function of H

For the second CATT-task, the 5th model with RT = 2.0 is was chosen in order to observe the perceived reverberation time at three different receiver positions.

Theresult should be compared with the 5.23-graph in the 'ATA book' wherethe perceived reverberation time is to be compared with the parameter H.

His a function of the ratio between the direct and the reverberant partof the acoustic energy. The direct part is proportional to the distancer to the power of -2 (distance between the source and the receiver) andthe reverberant part can be calculated as 4 divided by the area of theroom. Adobe photoshop user guide pdf. According to the graph, the closer you are to the sound sourcethe shorter the apparent reverberation time.

'ATA book': Figure 5.23

The area of our room is 2050 m^2. The source was, as before, placed in one corner with the coordinates (-12 , 0.5 , 0.5). The receivers were placed at the three different positions, providing their respective H.

The impulse response for each of these positions was then convolved with speech and a test person was used to estimate the perceived reverberation times.

The result corresponds well to the graph 5.23, even though our range of H is outside the range in 5.23 for position 1 and 3 (H = 22.1 and -12.8). The perceived reverberation time is clearly a function of distance. If you are in the direct sound field you will experience a shorter reverberation time than if you were further away.

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Subjectively perceived diffusivity:

The last CATT task was to explore how a delayed signal in one channel can influence the feeling of from where the sound is localized.

In order to do the investigation, we exported one of the binaural impulse responses from our CATT room into Matlab. Then one of the channels were duplicated and these two created mono responses were used as a stereo response. Different delay times in one of the channels were introduced to see how the direction of the source was affected and how the echo was perceived.

Listening to these three files, one can feel the directivity of the sound which signal has the delay time in one of the channels. If there is a delay in the right channel, one can feel the sound comes from the direction of left. Respectively, if there is a delay in the left channel - the directivity of the sound for the listener will be towards the right side. For the signal without any delay in both of the channels, we feel that the sound comes directly from in front of the face.