Quasi-cubic room with specular reflection and uniform absorption


Academic case: Quasi cubic room (8m x 10m x 9m) with specular reflection (no diffusion) and 10% uniform surface absorption, with a single source and 7 punctual receivers

Licence Creative Commons
All elements of this simulation are licensed under Licence Creative Commons Attribution 4.0 International License.

What is tested?

Comparison between SPPS/TCR simulations and results from the NORMAL code described in [Yang, 2000].

[yang, 2000] L.N. YANG, B.M. SHIELD, DEVELOPMENT OF A RAY TRACING COMPUTER MODEL FOR THE PREDICTION OF THE SOUND FIELD IN LONG ENCLOSURES, Journal of Sound and Vibration, Volume 229, Issue 1, 2000, Pages 133-146, ISSN 0022-460X, dx.doi.org/10.1006/jsvi.1999.2477.

CAUTION - The following results present comparisons between numerical simulations carried out with I-Simpa and 'reference' data available in the scientific literature. However, it is difficult to prejudge the concept of 'reference'. The deviation between the simulations and the reference data that can be observed do not necessarily call into question the corresponding simulations but can also be associated with other sources of deviation (modeling assumptions, numerical instabilities, experimental uncertainties, etc.). In addition, some numerical models (like SPPS), based on random methods, may produce small deviations between two distinct simulations.


Sound pressure level (SPL)

Regarding the y-scale for the sound pressure level (SPL) results, one can see a very good agreement between the SPPS code, as well as the TCR code, with the reference results (NORMAL code).

Reverberation time (RT30)

Here again, the SPPS code and the reference data are very closed together. The TCR code (Eyring formulae, i.e. with a constant value for all receivers) gives values slightly below.

Early decay time (EDT)

Regarding the y-scale of the early decay time (EDT), the SPPS code and the reference data are very closed. One can however observe quasi-uniform value for all receiver locations with the SPPS code, while there are small variations with the reference data.

Calculation parameters

Active calculation of Atmospheric absorptionNO
Active calculation of diffusion by fitting objectsNO
Active calculation of direct field onlyNO
Active calculation of transmissionNO
Calculation methodEnergetic
Limit value of the particle extinction5.0
Number of sound particles per source1 000 000
Number of sound particles per source (display)0
Random initialization number0
Receiver radius0.31
Simulation length (s)3.000
Time step (s)0.002
Active calculation of Atmospheric absorptionNO