I simulated Dan's experimental set-up for cross-talk measurements.
It was assumed that the LDV is fixed and measuring the lower left
hand corner element. The 2D images shows the measured amplitude
in the lower-left corner as a function of the location of the
focus of the ultrasound source. I used the theoretical beam pattern
of a focussed ultrasound. I assumed that:
Each hydrophone element scattered sound scattering constant phi
that did not vary with position in the array and that it was angle
independent.
There was no multiple scattering - that is sound scattered by
one element didn't rescatter off a second element.
I ran the scenario for two cases. The first where the scattered
sound decayed with cylindrical (1/sqrt(r)) spreading and the second
where the scattered sound decayed with spherical (1/r) spreading.
I have also included Dan's measured results: both the needle and
with the array. There appears to be atleast qualitative aggreement
with the cylindrical spreading case at phi=0.3.



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| robinc@bu.edu | April 2001 |