Acoustic focusing through two layer annuluses in air
Guan Yi-Jun1, Sun Hong-Xiang1, 2, †, , Liu Shu-Sen1, Yuan Shou-Qi1, ‡, , Xia Jian-Ping1, Ge Yong1
       

Schematic diagrams of (a) square annuluses (R1 = 24.00 mm, R2 = 36.00 mm, D1 = 12.00 mm, D2 = 18.00 mm, r1 = 2.00 mm, and r2 = 3.00 mm), (b) square and circular annuluses (θ = 9°, R1 = 14.00 mm, R2 = 18.00 mm, D1 = 12.00 mm, D2 = 18.00 mm, r1 = 2.00 mm, and r2 = 3.00 mm), (c) rhomboic annuluses (θ = 60°, d1 = 7.22 mm, d2 = 12.50 mm, D1 = 10.83 mm, D2 = 18.75 mm, r1 = 2.00 mm, and r2 = 3.00 mm), and (d) triangular annuluses (R1 = 26.27 mm, R2 = 39.40 mm, r1 = 2.00 mm, r2 = 3.00 mm, and θ = 60°). Pressure–field amplitude patterns for ((e)–(g)) square annuluses, ((h)–(j)) square and circular annuluses, ((k)–(m)) rhomboic annuluses, and ((n)–(p)) triangular annuluses with different incident positions.