Acoustic Poynting Vector
One of the most awarding acoustical experimental
technique of the last decade is the vectorial intensity (Poynting
vector, energy density flow, power per unit area) measurement
method. By means of this method, visua
lisation of an acoustic
field can be achieved in terms of energy-flux lines, thus adding
to analytical possibilities not found in more conventional
procedures. Intensity is a much more informative noise emission
measurand than, e.g., the scalar acoustic pressure in air-borne
acoustic fields. The intensity concept allows the discrimination
between a reactive part of the energy flow, which is dominating
in a high quality acoustic resonator, and the active or net energy
flow, which is the interesting v
ariable in damped complex real
structures. Sound sources and sinks, as well as main propagation
paths, are clearly indicated by this physical quantity.
The existing theory regarding the acoustic Poynting vector
in the free surface of a structure which up to now has only
been established for the case of isotropic structures, was
generalized to non-isotropic structures. It was
shown that,
in this general case, the measurement of the acoustic Poynting
vector in the surface can be reduced to a measurement of the
three in-plane strain and the two in-plane velocity components.
Based on this formulation, a sensor head concept for the
determination of the acoustic Poynting vector, using multipoint
optical in-plane displacement measurement was developed. The
concept was studied experimentally with a simple case of
one-dimensional structural vibration (Fig. 1). The experimental
results obtained with a sensor head designed for one-dimensional
acoustic energy flow demonstrate the feasibility of the
technique.