“…Set Ω = [−15, 15] × [−15, 15], we consider the following IBVPs (Deng and Liang 2020; Deng and Wu 2021)u tt − Δu = −δ 2 sin(u − v), (x, t) ∈ Ω × [0, T ], v tt − b 2 Δv = sin(u − v), (x, t) ∈ Ω × [0, T ], u(x, t), v(x, t) = (0, 0), (x, t) ∈ ∂Ω × [0, T ], u(x, 0), v(x, 0) = 4φ(x), φ(x) , u t (x, 0), v t (x, 0) = (0, 0), x ∈ Ω, in which φ(x) = arctan[exp(3 − x 2 + y 2 )]. Set u t = ω, v t = ϑ,the energy of this problem(Deng and Liang 2020;Deng and Wu 2021), which is defined byE(t) = 1 2 Ω αω 2 + β|∇u| 2 + γ ϑ 2 + |∇v| 2 + 2 G(u, v) dxdy, (5.1) is conservative. Here, G(u, v) = 1 − cos (u − v), α = β = δ −2 , γ = 1 and = b 2 .…”