Many spaces such as restaurants, open offices, and classrooms need an adaptive level of acoustic control that traditional solutions are unable to provide. Beyond simply reducing sound, these environments need effective absorption at high sound pressure levels (SPL), while maintaining natural, clear audibility at lower levels. SoundPly provides the solution.
Nearly all acoustic systems absorb sound using porous materials, such as foam, fiberglass, cotton or felt. These materials absorbs sound energy in two methods— viscous friction between air molecules as they flow throughout the open spaces inside the material, and mechanical damping from microscopic vibrations caused by air molecules impacting the porous material’s inner structure.
Due to the physical limitations of mechanical damping, porous materials absorb sound energy more effectively at low SPLs than at higher levels. Although increasing a porous material’s thickness improves its overall absorption capacity, it disproportionately improves the material’s low SPL absorption.
This bias is problematic, since the amount of porous material needed to sufficiently address higher SPLs results in the environment sounding “dead” and unnatural at lower SPL levels, due to the excessive sound absorption.
Through the innovative combination of porous and resonant absorption, SoundPly panels provide a more even, natural method of absorbing sound.
At the lowest sound levels, a micro-perforated panel absorbs the smallest percentage of acoustical energy. This is because the sound wave’s energy is below the critical threshold to propagate the evacuation and resonance of air through the panel’s micro-perforations.
This threshold is determined by several variables including the size, pattern, spacing, depth, and shape of the micro perforations, but is usually under 50 decibels.
At medium sound levels (50-80 decibels), sufficient energy exists to sustain air resonance within the micro-perforations. In this volume range, primary sound absorption occurs from acoustical energy losses through thermal and viscous friction.
At high sound levels (over 80 decibels), an additional jetting effect, called vortex shedding, becomes the dominate method of energy absorption. Air molecules are unorganized when they enter a micro-perforation, but as they flow through the perforation, the friction between the air and the perforation’s walls organize the molecules into donut-shaped rotating vortices. Due to the high level of acoustic energy contained in the vortices, they continue rotating upon exiting the perforation, and can travel a significant distance.
This jetting effect occurs on both sides of the micro-perforation, and significantly disrupts the uniformity of succeeding sound waves.