Sound transmission through slotted concrete blocks with attached gypsum board
Author(s) -
A. C. C. Warnock
Publication year - 1993
Publication title -
the journal of the acoustical society of america
Language(s) - French
Resource type - Journals
SCImago Journal Rank - 0.619
H-Index - 187
eISSN - 1520-8524
pISSN - 0001-4966
DOI - 10.1121/1.407354
Subject(s) - sound transmission class , octave (electronics) , acoustics , materials science , gypsum , resonance (particle physics) , sound (geography) , absorption (acoustics) , octave band , transmission (telecommunications) , block (permutation group theory) , air space , transmission loss , soundproofing , composite material , telecommunications , physics , computer science , geometry , engineering , mathematics , particle physics , aerospace engineering
Measurements of sound transmission loss through slotted concrete blocks with attached gypsum board showed that the cavity resonance of the blocks has an important beneficial effect. It counteracts the mass-air-mass resonance that occurs when gypsum board is added to the surface of a concrete block wall leaving an air space behind it. This significantly increases the sound transmission class rating relative to the same systems with normal-weight nonslotted blocks. The effects of the two resonances could be seen at different frequencies when there was no sound-absorbing material in the air space behind the gypsum board. When the air space was filled with sound-absorbing material, however, both resonances moved together and could not be separated, but the transmission losses and sound transmission class for the composite wall were still significantly greater than those for wall systems using nonresonant blocks. Sound absorption measurements for the slotted blocks showed the need for one-third octave band data in place of the octave band data often found in trade literature.Des mesures de l?indice d?affaiblissement acoustique \ue0 travers les blocs de b\ue9ton rainur\ue9s recouverts de plaques de pl\ue2tre ont r\ue9v\ue9l\ue9 que la r\ue9sonance de cavit\ue9 des blocs exerce un effet b\ue9n\ue9fique majeur \ue0 cet \ue9gard. Cet effet obvie au ph\ue9nom\ue8ne de r\ue9sonance masse-air-masse qui survient lorsque l?on ajoute les plaques de pl\ue2tre \ue0 la surface d?un mur de blocs en m\ue9nageant derri\ue8re une lame d?air. Ceci augmente consid\ue9rablement le coefficient de transmission sonore par rapport aux m\ueames syst\ue8mes avec blocs non rainur\ue9s de poids normal. Les incidences des deux types de r\ue9sonances pouvaient appara\ueetre \ue0 diff\ue9rentes fr\ue9quences en l?absence de tout mat\ue9riau absorbant acoustique dans la lame d?air \ue0 l?arri\ue8re des plaques de pl\ue2tre. Une fois la lame d?air combl\ue9e d?un mat\ue9riau absorbant, toutefois, les deux r\ue9sonances pr\ue9sentaient un mouvement simultan\ue9 et ne pouvaient \ueatre s\ue9par\ue9es. N\ue9anmoins, les indices d?affaiblissement acoustique et le coefficient de transmission sonore pour le mur en mat\ue9riau composite sont demeur\ue9s consid\ue9rablement plus \ue9lev\ue9s que ceux des syst\ue8mes de mur utilisant des blocs non r\ue9sonants. Les mesures de l?absorption acoustique pour les blocs rainur\ue9s ont fait ressortir la n\ue9cessit\ue9 de disposer de donn\ue9es de la bande de fr\ue9quences de tiers d?octave au lieu des donn\ue9es de la bande d?octave que l?on trouve souvent dans la documentation se rapportant au domaine.Peer reviewed: YesNRC publication: Ye
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