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Acoustic radiation force and torque on spheroidal particles in an ideal cylindrical chamber

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Academic year: 2021

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FIG. 1. (a) The cylindrical acoustic chamber with a (yel- (yel-low) spheroid located at r 0 regarding the laboratory frame O in the center of the chamber’s bottom
TABLE III. The theoretical predictions of the microspheroid at the nodal plane considering the parameters of Table II.
FIG. 2. The radiation force fields (red arrows) of the mi- mi-crospheroid aligned to the x axis
FIG. 3. The radiation torque fields (red arrows) in the levitation plane at z eq = 0.85H/2 produced by the (011) acoustic mode for (a) a soft and (b) hard lateral wall

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