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Catt acoustic v8
Catt acoustic v8













(1975), Nouvelle formule pour la dure´de reverberation. (1932), A modified formula for reverberation, J. (2010), Reverberation Radius in Real Rooms, Telfor Journal, 2, 2, 86–91. (1976), Effect of non-uniform distribution of absorption on reverberation, Journal of Sound Vibration, 46, 2, 209–224.

catt acoustic v8

(2008), On the minimum audible difference in direct-to-reverberant energy ratio, J. LARSEN E., IYER N., LANSING C.R., FENG A.S. (1991), Room Acoustics, Elsevier Applied Science, London. (1979), Critical distance measurement of rooms from the sound energy spectral response, J. Acta Acustica united with Acustica, 94, 6, 883–890. (2008), Comparison of Predicted, Measured and Auralized Sound Fields with Respect to Speech Intelligibility in Classrooms Using CATT-Acoustic and ODEON. (2006), Estimation Methods for Sound Levels and Reverberation Time in a Room with Irregular Shape or Absorption Distribution, Acta Acustica United with Acustica, 92, 797–806. (1959), Reverberation formula which seems to be more accurate with non-uniform distribution of absorption, J. (1930), Reverberation time in dead rooms, J. (2003), The average absorption coefficient for enclosed spaces with non uniformly distributed absorption, Applied Acoustics, 64, 845–862.ĮYRING C.F. CATT, Mariagatan 16A, 41471 Gothenburg, Sweden.ĭUCOURNEAU J., PLANEAU V. (2000), Predicting reverberation times in a simulated classroom, J. (2009), A comparative analysis of energy models in churches, J. Simul., 7, 1, 1–16.īERARDI U., CIRILLO E., MARTELLOTTA F. Am., 135, 1, 223–230.īERARDI U., (2014), Simulation of acoustical parameters in rectangular churches, J. (2014), Mean-free-paths in concert and chamber music halls and the correct method for calibrating dodecahedral sound sources, J. (1988), Energy relations in concert auditoriums, J. (1941), Practical Acoustics and Planning Against Noise, Ed. Proceedings of Meetings on Acoustics, 19, 015141.īAGENAL H. (2013), The reverberation radius in an enclosure with asymmetrical absorption distribution. (2012), Sound Pressure Level in Rooms: Study of steady state intensity, total sound level, reverberation distance, a new discussion of steady state intensity and other experimental formulae, Building Acoustics, 19, 3, 205–220.ĪRAU-P. According to this interpretation, the time corresponding to the sound to travel a reverberation radius should be assumed as the lower limit of integration of the diffuse sound energy.ĪRAU-P. Finally, this paper introduces a new interpretation of the reverberation radius in non-diffuse sound fields. Then, a comparison between the classic formulas and the new one is performed in some rectangular rooms with non-uniformly distributed sound absorption.

catt acoustic v8

Starting from theories for determining the reverberation time in non-diffuse sound fields, this paper firstly proposes a new formula to calculate the reverberation radius in rooms with non-uniformly distributed sound absorption. Nevertheless, the generally used formulas for the reverberation radius have been used in any circumstance. However, these theories are only valid in perfectly diffused sound fields thus, only when the energy density is constant throughout a room. The currently used formulas to calculate the reverberation radius have been derived by the classic theories of Sabine or Eyring. The reverberation radius is the distance from a sound source at which the direct sound level equals the reflected sound level.

catt acoustic v8

This paper discusses the concept of the reverberation radius, also known as critical distance, in rooms with non-uniformly distributed sound absorption.















Catt acoustic v8