Diffuse field acoustic testing

Diffuse field acoustic testing is the testing of the mechanical resistance of a spacecraft to the acoustic pressures during launch.

In the aerospace industry, acoustic chambers are the main facilities for such tests. A chamber is a reverberant room that creates a diffuse sound field and is composed of an empty volume (from 1 m³ to 2900 m³) and a multifrequency sound generation system.

Diffuse field principle

Theoretically, diffuse field is defined as a Sound pressure field where there is no privileged direction of the energy. In other words, when sound pressure is the same everywhere in the room. This is obtained with large rooms with no absorbent materials on walls, ceiling or floor. Diffusion is enhanced in asymmetric rooms. To obtain such conditions, the room must be reverberant. The source's direct field must be negligible compared to the reverberant field, avoiding privileged propagation.^[1]

Reverberation time

Reverberation is due to multiple reflections on walls with some delays that come back to the receptor. Summing up these contributions, a reverberant pressure field is created. The more reverberation, the more the field is diffused.

Two oft-used measures of reverberation time quantify this parameter, : $RT_{30}$ and $RT_{60}$ . These values are the interval for the sound pressure level to the lower of 30 or 60 dBSPL. It can be obtained by measuring the sound pressure decrease after a sound impulse or by using approximate formulas such as Sabine's or Eyring's. In the case of a diffuse field (low absorption on the walls, and big volumes) Sabine's formula is used.

$RT_{60}=0.16{\frac {V}{A}}$

Where $A=\sum S\times \alpha$ is the equivalent absorption area involving the surface $S$ of the walls and their absorption coefficient $\alpha$ .

Geometrical approach

Schematic representation of specular (in blue) and diffused (in green) reflections of an incident wave ray (in red)

Many theoretical ways to model sound propagation are used. One of these is the geometrical approach. This represents sound waves as a ray of energy propagating. When it meets an obstacle, this ray has two possible behaviors: It can be reflected following the normal of the plan, specular reflection. Alternatively it can be separated into many rays following a mathematical law (for example Lambert's law), diffused reflection.

Quantities involving diffuse pressure field

Frequency is a main factor of a good diffused field. Some phenomena linked to frequency of the sound pressure field lead to poor homogeneity of a pressure field. The frequency response of a room is the amplification or reduction of some frequencies. It represents the repartition of pressure with respect to frequency. In low frequencies this can lead to mode apparition. These modes are due to standing waves that lead to maximum and minimum pressure according to the geometry of the room. To determine the frequency for which the pressure field can be considered diffused, Schroeder's frequency is commonly used. It is obtained considering the frequency from which the modal overlap exceeds $M=3$ . Below this frequency, the field is not diffuse and standing waves create pressure modes

$F_{s}=2000{\sqrt {\frac {RT_{60}}{V}}}$

Where $RT_{60}$ is the reverberation time of the room and $V$ its volume.

Schematic transverse cut view of pressure modes in a duct (closed-closed)

For example, in the case of a rectangular room, low frequency modes are determined relative to the room dimensions as

$f_{lmn}={\frac {c_{0}}{2}}{\sqrt {\left({\frac {l}{L_{x}}}\right)^{2}+\left({\frac {m}{L_{y}}}\right)^{2}+\left({\frac {n}{L_{z}}}\right)^{2}}}$

Where $l$ , $m$ and $n$ are respectively the mode of the length $L_{x}$ , $L_{y}$ and $L_{z}$ of the room and $c_{0}$ the celerity of sound in the working fluid.

Aerospace application

Acoustic tests are mainly use for environmental tests on aircraft structures.^[2] Satellites are expensive products with high-engineering built-in components.^[3] To improve the resistance of a spacecraft during launch and during its orbital life, analysis is focused on tests in three categories : Thermal, Radio-frequencies and Vibrations. This last test area is focused on the mechanical stresses that the specimen will meet during its life, especially during launch.

Mechanical forces applied during spacecraft launch
Launch steps	Resulting mechanical aggressions
First Stage ignition and boosters ignition	Acoustic vibration and quasi-static loads
Boosters extinction	Sinusoidal vibrations
First stage Extinction	Sinusoidal vibrations
Second Stage ignition	Quasi-static loads
Fairing release	Pyrotechnic shock
Second stage extinction	Sinusoidal vibrations
Third stage ignition	Quasi-static loads
Third stage extinction	Sinusoidal vibrations
Spacecraft release	Clamp band release shock

Acoustics creates mechanical stresses during the first five seconds. Sound pressure levels can go up to 150 dBSPL. Acoustic tests are used to verify the mechanical resistance of the satellite and its elements to acoustic pressures generated.

Accelerometer measurement

Once the sound generation system is working, acceleration measurement is performed by accelerometers placed on the specimen.

Acoustic chamber

Sound generation

To test a satellite, a sound generation system generates a broadband spectrum ([25 Hz-10000]Hz) simulating the maximum envelope of all launchers that the satellite may fly in. To qualify, three tests are realized with changing global gain compared to launcher spectrum:

Low-Level : - 8 dB SPL
Intermediate : - 4 dB SPL
PFM (Proto Flight Model) : 0 dB SPL

Before testing the satellite, an empty room test is performed to check the chamber's signature.

This pressure field is generated by multifrequency sirens powered by nitrogen or compressed air modulators. This system can generate sound pressure levels up to 160 dBSPL. Each acoustic chamber has its own configurations, but each siren is centered on a frequency where sound pressure levels are the highest. In some cases these sirens can be completed with electroacoustic systems to generate and control midrange and high frequencies. Sirens generate low frequencies, but with high sound pressure levels distortion appears that leads to higher harmonics. Loudspeakers are used in some chambers to control these frequencies.

To produce exact levels, piloting microphones check sound pressure levels and apply a realtime gain correction to adjust the level.

Advantages

Homogeneity : Spatial homogeneity guaranteed for ± 1.5 dBSPL
Low frequency generation : Very efficient low frequency generation (below 50 Hz)
Security : Control with piloting microphones that adjust the level or abort if needed
Representativeness : Faithful to real stresses during launch
Well known process : Used by many aerospace industries

Disadvantages

Gas generation : May require large amounts of nitrogen
High frequency control : If no high frequency sirens or electroacoustic devices are included, only harmonics generated by distortion produce mid and high frequencies.

Examples

Thales Alenia Space (Cannes) : 1000 m³
IABG (Ottobrunn) : 1378 m³
NASA : 2860 m³

References

^ Potel, Catherine; Bruneau, Michel (2006). Acoustique générale: équations différentielles et intégrales, solutions en milieux fluides et solides, applications. Ellipses. ISBN 978-2-7298-2805-9.
^ Tustin, Wayne; Mercado, Robert (1 August 1984). Random vibration in perspective. Tustin Institute of Technology. ISBN 978-0-918247-00-1.
^ Maral, Gerard; Bousquet, Michel (2009). Satellite Communications Systems: Systems, Techniques and Technology (5 ed.). Wiley. ISBN 978-0-470-71458-4.

External links

[potel-1] Potel, Catherine; Bruneau, Michel (2006). Acoustique générale: équations différentielles et intégrales, solutions en milieux fluides et solides, applications. Ellipses. ISBN 978-2-7298-2805-9.

[tustin-2] Tustin, Wayne; Mercado, Robert (1 August 1984). Random vibration in perspective. Tustin Institute of Technology. ISBN 978-0-918247-00-1.

[MaralBousquet2009-3] Maral, Gerard; Bousquet, Michel (2009). Satellite Communications Systems: Systems, Techniques and Technology (5 ed.). Wiley. ISBN 978-0-470-71458-4.

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