
How Engine Exhaust Silencers Work
Reducing the noise of an internal combustion engine without sacrificing its performance: that is the whole point of passive mufflers. This note details the two physical mechanisms—reactive and dissipative—that make this possible.
Passive and Active Silencers
Engine exhaust silencers are devices integrated into the exhaust system of internal combustion engines. Their function is to reduce engine noise while causing as little pressure drop as possible.
These are known as passive silencers. Unlike active silencers, which use electrical and electronic components to reduce noise through active wave interference, passive silencers are purely mechanical devices—with no power supply, no electronics, and no active moving parts.
Two complementary principles: reactive attenuation and dissipative attenuation. These two physical phenomena, discussed in detail below, generally work together within a single muffler.
Attenuation due to reactive effects
Wave reflection is caused by reflective surfaces, changes in cross-sectional area, or changes in medium within the silencer. This phenomenon results in an acoustic impedance mismatch: some of the incident energy is reflected back toward the source rather than transmitted toward the outlet.
When two sound waves meet with a certain phase difference, interference —constructive or destructive—occurs, resulting in an increase or decrease in sound amplitude depending on the phase difference. Resonators (Helmholtz resonators, quarter-wave resonators, Herschel-Quincke resonators) exploit this principle precisely to generate destructive interference at targeted frequencies.
Frequency-specific characteristic: The reactive effect is most effective at low frequencies, where sound waves can be considered plane waves. It is highly effective over narrow frequency ranges centered on the resonance frequencies of the resonators within the silencer. This is why it is essential to “tune” the silencer to the fundamental frequencies to be treated in order to achieve effective attenuation.
The following equations, which apply in the plane-wave domain, can be used to calculate the characteristic frequencies of the main geometries used:
| Configuration | Formule |
|---|---|
| Fréquence d'un tube ouvert | f = n · c / 2L |
| Fréquence d'Helmholtz | f = c/2π · (S1/V1L + S2/V2L)0.5 |
| Fréquence d'un fond fermé | f = (2n+1) · c / 4L |
| Fréquence d'un résonateur d'Helmholtz | f = c/2π · (A/VL)0.5 |
| Fréquences de Herschel-Quincke | f1 = c/2(l2−l1) · f2 = c/(l1+l2) |
Attenuation due to dissipative effects
Engine mufflers also use fibrous materials to absorb some of the acoustic energy.
As the waves pass through the fibers, they cause the fibrous skeleton to vibrate, resulting in mechanical dissipation of the sound energy—which is converted into heat.
The friction between air molecules in the porous medium also leads to visco-inertial dissipation of the acoustic energy.
Efficiency range: Absorption is effective at mid and high frequencies—complementing the reactive effect, which is more effective at low frequencies.
The choice of absorbent material and its installation directly affect the sound attenuation performance. Depending on the duct geometry, the configuration varies: lining, core, or ring for cylindrical ducts; parallel baffles for rectangular ducts. To prevent fiber shedding, perforated metal sheets and/or fiberglass fabric are added for protection.
Boët StopSon silencers are designed using finite element and fluid simulation software. These tools make it possible to simultaneously account for reactive and dissipative effects while minimizing pressure drops—a joint optimization that is rarely achieved without advanced modeling.
Modeling of Porous Materials
To correctly model an absorbent fiber, it is necessary to know several intrinsic parameters of the porous material:
- Porosity
- Tortuosity
- Resistivity
- Viscous characteristic length
- Thermal characteristic length
Under certain conditions, the mechanical properties of the fibrous skeleton may also be necessary for modeling.
These parameters are fed into various physical models—Delany-Bazley-Miki, Johnson-Champoux-Allard-Lafarge, Limp, Biot-Allard—which enable BOËT silencers to be precisely tuned to the actual sound spectra of the engines in question.
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Building codes
Quality Certifications
French Code
CODAP
CODETI
U.S. Code
ASME Section VIII
ASME B31.1
ASME B31.3
European standards
EN 13445
; EN 13480
Nuclear sector
RCC-M (AFCEN)



