“…The requirement for equations (1) to (15) is that ξ, η and τ are independent of u, equations ( 16), ( 17) and (18) give ξ x = τ t = η y , equations (19), (20) and (21) give ξ t /c 2 = τ x , η t /c 2 = τ y and η x = −ξ y , equations (34), (35) and (36) give φ = βu + α where α = α(x, y, t) and β = β(x, y, t) are functions. From the equation (37), (38) and (39) we get β x = 0, β y = 0 and β t = 0, from (40) we find β = Q = c 4 2 /m 2 c 2 . The most general infinitesimal symmetry of the two-dimensional KG equation in ideal fluid has coefficient function of the form ξ = c 5 y + (c 6 t + c 2 ) /c 2 , η = −c 5 x + (c 7 t + c 2 ) /c 2 , τ = c 6 x + c 7 y + c 1 c 2 and φ = c 4 2 /m 2 c 2 u + α where c 1 , .…”