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.
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, : formula_1 and formula_2. 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.
formula_3
Where formula_4 is the equivalent absorption area involving the surface formula_5 of the walls and their absorption coefficient formula_6.
Geometrical approach.
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 formula_7. Below this frequency, the field is not diffuse and standing waves create pressure modes
formula_8
Where formula_2 is the reverberation time of the room and formula_10 its volume.
For example, in the case of a rectangular room, low frequency modes are determined relative to the room dimensions as
formula_11
Where formula_12, formula_13 and formula_14 are respectively the mode of the length formula_15, formula_16 and formula_17 of the room and formula_18 the celerity of sound in the working fluid.
Aerospace application.
Acoustic tests are mainly use for environmental tests on aircraft structures. Satellites are expensive products with high-engineering built-in components. 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.
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:
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.