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8.3 Governing equations   199




                     The vector field particle velocity is similar to wave equation:
                                                    1  ∂ u                                                                                     2   2 2  2
                                                      2
                                              ∇ u  =                              (8.9)                                                       ∇ u=1c ∂ u∂t
                                                2
                                                   c 2  ∂t 2
                     The sound wave equation in one dimension is as follow:
                                               2
                                                      2
                                              ∂ P  −  1  ∂ P  = 0                (8.10)                                                       ∂ P∂x −1c ∂ P∂t =0
                                                                                                                                              2
                                                                                                                                                         2
                                                                                                                                                 2
                                                                                                                                                     2 2
                                              ∂x 2  c 2  ∂t 2
                  where c and P are the speed of sound and the acoustic pressure (the local deviation
                  from the ambient pressure), respectively.
                  8.3.2  Westervelt equation
                  The Westervelt equation is a very popular and high accuracy model for ultrasound
                  modeling. The generalized Westervelt equation is as follow [59, 60]

                                      1     1  ∂ P  δ ∂ p  β ∂ p 2
                                                        3
                                                                2
                                                 2
                                  ρ∇⋅   ∇p   −  2  2  +  4  3  +  4  2  = 0    (8.11)                                                      ρ∇⋅1ρ ∇p− 1c  ∂ P∂t +δc ∂ p∂t +
                                                                                                                                                      2
                                                                                                                                                       2
                                                                                                                                                              4 3
                                                                                                                                                                  3
                                                                                                                                                          2
                                          
                                     
                                      ρ
                                             c
                                                ∂t
                                                     c
                                                            ρc
                                                                ∂t
                                                       ∂t
                                                                                                                                                     4 2 2
                                                                                                                                                          2
                                                                                                                                                   βρc ∂ p ∂t =0
                  where p, c, δ, β, and ρ are the sound pressure, the speed of sound, the sound dif-
                  fusivity, the coefficient of nonlinearity and the ambient density, respectively. In Eq.
                  (1), the first term takes diffraction into account. The third term accounts for attenu-
                  ation. The last term introduces the quadratic nonlinearity. Several simplified ver-
                  sions can be derived from Eq. (1). By using constants for all acoustic parameters, the
                  Westervelt equation for homogeneous media can be recovered [61].
                                          1  ∂ P  δ ∂ p   β  ∂ p  2
                                                              2
                                             2
                                                     3
                                     2
                                                                                                                                                            4 3
                                                                                                                                                   2
                                                                                                                                             2
                                                                                                                                                                3
                                    ∇ p  −     +  0    +   0     = 0             (8.12)                                                      ∇ p− 1c  ∂ P∂t +δ c ∂ p∂t +β
                                                                                                                                                        2
                                                                                                                                                     2
                                         c 0 2  ∂t 2  c 0 4  ∂t 3  ρ c  4  ∂t 2                                                                   0   4 2 2  0 0
                                                                                                                                                          2
                                                                                                                                                   ρ c ∂ p ∂t =0
                                                          00
                                                                                                                                                  0 0 0
                     where c , ρ , δ , and β  are the acoustic parameters for the background medium.
                           0
                              0
                                0
                                      0
                  The linear acoustic wave equation can be derived by setting β  to 0, so that
                                                                   0
                                                          3
                                                  2
                                               1  ∂ P  δ ∂ p
                                                                                                                                                        2
                                                                                                                                                                 3
                                                                                                                                                            4 3
                                         ∇ p −       +  0   = 0                  (8.13)                                                       ∇ p− 1c  ∂ P∂t +δ c ∂ p∂t =0
                                          2
                                                                                                                                                   2
                                                                                                                                              2
                                                                                                                                                     2
                                              c 0 2  ∂t 2  c 0 4  ∂t 3                                                                             0       0 0
                     Eqs (2) and (3) are useful for studies on characterizing acoustic fields of trans-
                  ducers and for approximately estimating the acoustic field in biological tissue [62].
                  Eq. (8.11) is used when heterogeneous medium such as skull [59]. On the other
                  hand, nonlinear Eqs (8.11) and (8.12) are used for lithotripsy, histotripsy, and tissue
                  harmonic imaging [63], when high pressure of ultrasound is present. Researchers
                  reported that using the linear acoustic approximation could underestimate the tem-
                  perature elevation in tissue [62].
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