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. Author manuscript; available in PMC: 2016 Jun 7.
Published in final edited form as: Phys Med Biol. 2015 May 14;60(11):4295–4312. doi: 10.1088/0031-9155/60/11/4295

Fig. 9.

Fig. 9

(a) Experimentally measured and (b) theoretically predicted spectral components of the displacements on the surface of the two-layered medium (E1 = 8 kPa, E2 = 48 kPa) at the point of excitation (r=0) with different thicknesses of the top soft layer (h1 = 5 mm, and h1 = 2 mm). (c), (e) Experimentally measured and (d), (f) theoretically predicted displacements in the time domain for the first (h1 = 5mm) and the second (h1 = 2 mm) phantoms, respectively, when two different durations of the acoustic pulse were used (0.27 ms and 2.7 ms). In calculations Pmax = 43 Pa for both phantoms.