Centrifugal glass wool is a porous sound absorbing material with good sound absorption properties. The reason why centrifugal glass wool can absorb sound is not because of the rough surface, but because of the large number of tiny pores and pores that communicate inside and outside. When sound waves are incident on the centrifugal glass wool, sound waves can enter the inside of the material along the pores, causing vibration of air molecules in the gap. Due to the viscous resistance of the air and the friction between the air molecules and the pore walls, the acoustic energy is converted into heat energy and lost.
Sound absorption performance
Centrifugal glass wool has good sound absorption performance for high frequency in sound. The main factors affecting the sound absorption performance of centrifugal glass wool are thickness, density and air flow resistance. Density is the weight of material per cubic meter. The air flow resistance is the ratio of the air pressure to the air flow rate on both sides of the material per unit thickness. Air flow resistance is the most important factor affecting the sound absorption performance of centrifugal glass wool. The flow resistance is too small, indicating that the material is sparse, the air vibration is easy to pass through, and the sound absorption performance is degraded; the flow resistance is too large, indicating that the material is dense, the air vibration is difficult to be introduced, and the sound absorption performance is also lowered. For centrifugal glass wool, the sound absorption performance has the best flow resistance.
In actual engineering, it is difficult to measure the air flow resistance, but it can be roughly estimated and controlled by thickness and bulk density.
1. As the thickness increases, the mid-low frequency sound absorption coefficient increases remarkably, but the high frequency does not change much (high-frequency absorption is always large).
2. The thickness is constant, the bulk density increases, and the sound absorption coefficient of the middle and low frequency also increases; but when the bulk density increases to a certain extent, the material becomes dense, the flow resistance is greater than the optimal flow resistance, and the sound absorption coefficient decreases. For centrifugal glass wool with a bulk density of more than 5 cm and a bulk density of 16 kg/m3, the low frequency 125 Hz is about 0.2, and the sound absorption coefficient of medium and high frequency (>500 Hz) is already close to one. When the thickness continues to increase from 5 cm, the sound absorption coefficient of the low frequency gradually increases. When the thickness is more than 1 m, the sound absorption coefficient of the low frequency 125 Hz will also be close to 1. When the thickness is constant and the bulk density is increased, the low-frequency sound absorption coefficient of the centrifugal glass wool will also increase continuously. When the bulk density is close to 110kg/m3, the sound absorption performance reaches the maximum value, 50mm thick and the frequency is close to 0.6-0.7 at 125Hz. When the bulk density exceeds 120kg/m3, the sound absorption performance decreases, because the material becomes dense, and the mid-high frequency sound absorption performance is greatly affected. When the bulk density exceeds 300kg/m3, the sound absorption performance is greatly reduced. The thickness of sound-absorbing glass wool commonly used in architectural acoustics is 2.5cm, 5cm, 10cm, and the bulk density is 16, 24, 32, 48, 80, 96, 112kg/m3. Centrifugal glass wool of 5 cm thick and 12-48 kg/m3 is usually used.
The sound absorption performance of centrifugal glass wool is also closely related to the installation conditions. When there is an air layer behind the glass wool board, the sound absorption effect of the glass wool board having the same thickness and no air layer is similar. In particular, the sound absorption performance of the middle and low frequency is much higher than that of the material on the hard bottom surface, and the sound absorption coefficient will increase as the thickness of the air layer increases, but the effect is not obvious after increasing to a certain value.
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