Multi-scale wave-flow-sediment coupling beach evolution prediction model method

Through the multi-scale wave-flow-silt coupled shore and beach evolution prediction model method, the problems of long calculation time and difficult parameter confirmation of existing tidal beach landform morphology evolution models are solved, and efficient and high-precision tidal beach landform morphology evolution simulation is achieved. .

CN119476096AActive Publication Date: 2025-02-18HOHAI UNIV

Patent Information

Application Number
CN202411507649.2
Authority / Receiving Office
CN · China
Patent Type
Applications(China)
Current Assignee / Owner
Filing Date
2024-10-25
Publication Date
2025-02-18
Estimated Expiration
2044-10-25

AI Technical Summary

Technical Problem

The existing tidal flat landform morphological evolution model has a long time to calculate and is difficult to confirm parameters. Especially for viscous sediment, the existing model has efficiency and accuracy problems in the simulation and prediction of long-term geomorphological evolution.

Method used

A multi-scale wave-flow-silt coupled shore and beach evolution prediction model method is proposed, including tidal power module, wave power module and silt power module. The finite difference method is iteratively solved to obtain the dynamic evolution process of tidal landform morphology.

Benefits of technology

The calculation efficiency of the morphological evolution of the coastal tidal beaches is significantly improved, the calculation time is only 1/5 of that of the traditional model, and the simulation accuracy is improved. The topographic curve is relatively close to the Delft3D model, and the error decreases with time.

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Abstract

The invention discloses a multi-scale wave-flow-sediment coupling beach evolution prediction model method, and relates to the technical field of tidal flat landform morphology evolution simulation, comprising the steps of integrating a tidal current power module, a wave motion module and a sediment power module, solving, and predicting landform morphology evolution of a tidal flat area; establishing a coordinate system according to actually measured tidal flat topographic data, obtaining tidal current, wave and sediment data based on a hydrometric station, taking the data as boundary conditions, and importing the boundary conditions into the model; constructing a beach evolution prediction model based on integration of tidal current power, wave motion and sediment power modules, and setting parameters required by each module; a finite difference method is adopted to solve a fluid continuity equation, a wave energy conservation equation, a one-dimensional vertical average suspended sediment convection and diffusion equation and a bottom bed updating equation, and tidal flat section terrains at different stages are obtained, so that the tidal flat section form evolution process under the action of waves and flow is accurately simulated, and compared with a traditional tidal current sediment model, the simulation precision is higher, and the simulation efficiency is higher. And the calculation efficiency can be obviously improved.
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Description

Technical Field

[0001] The invention relates to the technical field of tidal flat landform evolution simulation technology, and in particular to a multi-scale wave-current-sediment coupling shore evolution prediction model method. Background Art

[0002] Tidal flats are buffer zones between humans and the ocean. Tidal flat profiles are controlled by factors such as tides, waves, sediment, and organisms. The complex feedback mechanism between multiple dynamic factors increases the complexity of tidal flat profile morphology prediction. Under the influence of the positive feedback of hydrodynamics and morphology, tidal flats are in a long-term dynamic balance of erosion or siltation. Numerical models play an important role in analyzing and predicting the evolution of tidal flat morphology.

[0003] However, such models require complex boundary conditions and input parameters, which are generally in two-dimensional or three-dimensional form. The simulation and prediction of long-term landform evolution usually requires a long computing time. In addition, the near-bottom sediment flux terms in the existing sediment module control equations are calculated using the shear stress method. The suspension and sedimentation states of sediment are usually controlled by the critical scour shear stress and the critical erosion shear stress, while the critical erosion shear stress and erosion rate generally need to be determined in the laboratory. It is difficult to confirm the parameters, especially for cohesive sediment. Many studies have found that the values ​​are arbitrarily taken and are not very reasonable. Summary of the invention

[0004] In order to solve the above technical problems, the present invention provides a multi-scale wave-current-sediment coupled beach evolution prediction model method, comprising the following steps:

[0005] S1. According to the given offshore tidal flat sea area topographic data, a coordinate system is established, and then the tidal, wave and sediment conditions of the area are obtained based on the observation station;

[0006] S2. Construct a wave-current-sediment coupled beach evolution prediction model. The wave-current-sediment coupled beach evolution prediction model includes a tidal current dynamics module, a wave dynamics module, and a sediment dynamics module. The tidal current dynamics module is constructed based on the fluid continuity equation with zero gradient on the free surface. The wave propagation module is generated based on the wave energy conservation equation. Starting from the sediment entrainment force formula, the near-bottom sediment flux F required for the one-dimensional average suspended sediment convection diffusion equation is provided. s , combined with the bed renewal equation dominated by the near-bottom sediment flux, a sediment dynamics module is constructed;

[0007] S3, collating the data obtained in step S1 and using them as boundary conditions to import into the wave-current-sediment coupled beach evolution prediction model;

[0008] S4. The finite difference method is used to iteratively solve the wave-current-sediment coupled beach evolution prediction model to obtain the dynamic evolution process of tidal flat landform morphology.

[0009] The technical solution further defined in the present invention is:

[0010] Furthermore, in step S2, the tidal power module is based on the fluid continuity equation, assuming that at any time, the gradient of the free surface is 0, that is, there is no oscillation of the liquid surface, and ignoring the momentum equation, the control equation is as follows:

[0011]

[0012] Where u represents the average velocity in the depth of the tidal flat section, t represents time, and x represents the distance across the shore; water depth h = η-z b , η represents the water surface height, z b Indicates the bed elevation;

[0013] The water surface height η function satisfies the following formula:

[0014]

[0015] Where A is the tidal amplitude, T c represents the power flow period, T c =12h.

[0016] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, in step S2, a wave power module is formed based on the wave energy conservation equation, and the wave energy conservation equation is as follows:

[0017]

[0018] Where E represents wave energy, ρ represents the density of seawater, g represents the acceleration due to gravity, H rms Represents the root mean square wave height; S tot represents the total wave energy term, c g is the group velocity, S fric represents the wave bottom friction term, S break represents the wave breaking source term;

[0019] Group velocity c g It represents the propagation speed of wave energy. Based on linear wave theory, it is expressed as follows:

[0020]

[0021] Where c = σ / k represents the phase velocity of the wave, σ represents the wave frequency, k represents the wave number, and the direction of the wave phase velocity is fixed to the shoreward direction;

[0022] Wave bottom friction term S fric As shown below:

[0023]

[0024] Among them, α f represents the wave energy dissipation coefficient, H represents the wave height, T w represents the wave period;

[0025] When the water depth gradient is large and the wave height exceeds a certain proportion of the water depth, the waves break, as shown in the following formula:

[0026]

[0027] Among them, α represents the constant 1; Qb represents the probability of wave breaking determined by the discriminant index b, H represents wave height, the maximum wave height is H max =0.78h.

[0028] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, in step S2, starting from the sediment entrainment force formula, the near-bottom sediment flux F required by the one-dimensional average suspended sediment convection-diffusion equation is provided. s , and combined with the bottom bed renewal equation controlled by the near-bottom sediment flux to form a sediment dynamic module. The sediment model control equation adopts the one-dimensional vertical average suspended sediment convection diffusion equation, which is as follows:

[0029]

[0030] F s =αω(C * -C)

[0031] Where h represents water depth, C represents vertical average sediment content, t represents time, u represents depth average velocity in the tidal flat section, x represents cross-shore distance, ε represents horizontal suspended sediment diffusion coefficient, and F represents the average vertical average sediment content. s represents the suspended sediment flux near the bottom, α represents the constant 1, ω represents the sediment settling velocity, C * Indicates the force of holding sand;

[0032] The near-bottom sediment flux will cause scouring or siltation of the bottom bed, and the bed surface renewal equation is expressed by the following formula:

[0033]

[0034] Where p represents the porosity of the bed sediment, ρ s represents the sediment density, z b Indicates the bed surface elevation.

[0035] As mentioned above, a multi-scale wave-current-sediment coupled beach evolution prediction model method, the sediment carrying force C * The same dimension as the vertical average sediment content C:

[0036]

[0037] Among them, C D represents the drag coefficient, ρ and ρ s They represent the density of water and sediment respectively, U represents the dynamic factor, and g represents the acceleration due to gravity;

[0038] Drag coefficient C D It is related to the Reynolds number and the bed surface roughness, and is expressed by the Manning formula:

[0039]

[0040] The calculation formula of power factor U is:

[0041]

[0042] Where n represents the roughness, u c represents the tidal flow velocity, u w represents the wave velocity, f c and f w represent the tidal current and wave resistance coefficient f respectively c =gn 2 / h 1 / 3 ,, ξ represents the displacement amplitude of the bottom particles, ξ=u w T w / 2π,T w represents the wave period, k s represents the Nicolaz function value;

[0043] The formula of sand holding force is summarized as follows:

[0044] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, in step S3, the boundary conditions required by the wave-current-sediment coupled beach evolution prediction model are the land boundary and the seaward boundary, the land boundary adopts a closed boundary condition, and the seaward open boundary adopts different boundary conditions according to different equations;

[0045] The tidal equation adopts the Dirichlet boundary condition of flow, and the boundary physical quantity is a constant; the wave equation boundary adopts the Dirichlet boundary condition of root mean square wave height; the sediment equation adopts the Dirichlet boundary condition at high tide and the Neumann boundary condition at low tide, and the gradient of the boundary physical quantity is a constant.

[0046] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, step S4 specifically includes the following sub-steps:

[0047] S4.1. Based on the provided boundary conditions, solve the tidal dynamics module and wave propagation module using the finite difference method to calculate the flow velocity and wave velocity distribution on the tidal flat terrain;

[0048] S4.2. Substitute the velocity and wave velocity distribution obtained from the wave dynamics module and the tidal current dynamics module into the sediment entrainment force formula to calculate the sediment entrainment force, discretely solve the average suspended sediment convection diffusion equation and the sediment entrainment force formula, and obtain the suspended sediment concentration distribution on the tidal flat terrain;

[0049] S4.3. Based on the solved suspended sediment concentration distribution, substitute it into the bed update equation and use the forward Euler method to iterate and solve it to obtain the tidal flat profile topography at different simulation stages.

[0050] As described above, in a multi-scale wave-current-sediment coupled shore evolution prediction model method, in step S4.1, the tidal dynamic equation includes the time derivative term Where h represents water depth, t represents time, and the time derivative term By directly differentiating the water surface function with respect to time, the equation is transformed into an ordinary differential equation:

[0051]

[0052] Where x represents the cross-shore distance, q represents the flow rate per single width, and the unit is m 2 / s, q = hu, q is discretized by first-order forward difference, u represents the depth-averaged velocity in the tidal flat section direction; i represents the spatial scale, Δx represents the spatial step length, q i+1 represents the single-width flow q value at spatial position i+1, q i Represents the single-width flow q value at spatial position i; when determining the boundary flow q bd =∫Δh(x, t)dx / Δt, the equation is directly solved by iteration, where Δh represents the change in water level and Δt represents the time step.

[0053] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, in step S4.2, the wave energy conservation equation in the wave power module includes the convection term The first-order forward difference is used to solve the space, and the backward Euler method is used to implicitly solve the equation in the time term:

[0054]

[0055] Among them, c g represents the wave group velocity, E represents the wave energy, x represents the cross-shore distance, Δx represents the spatial step size, and j represents the time scale; It represents the wave energy at spatial position i and time scale j+1; It represents the wave energy at the spatial position i+1 and the time scale j+1; represents the wave energy at spatial position i and time scale j; It represents the group velocity at the spatial position i+1 and the time scale j+1; It represents the group velocity at spatial position i and time scale j+1; Represents the total wave energy at spatial position i and time scale j.

[0056] As described above, in a multi-scale wave-current-sediment coupled beach evolution prediction model method, in step S4.3, the suspended sediment convection diffusion equation in the sediment dynamics module includes the convection term Where h represents the water depth, u represents the average velocity in the depth of the tidal flat section, C represents the vertical average sediment content, and x represents the cross-shore distance; the discretization of the convection term adopts the upwind format, that is, the first-order backward difference is used when the tide u>0, and the first-order forward difference is used when the tide u<0; the time discretization also adopts the implicit backward Euler method; the source term part less than 0 -αωC is linearized implicitly, where α represents the constant 1 and ω represents the sediment settling velocity; the specific discretization format is as follows:

[0057] Time Item:

[0058]

[0059] Diffusion term:

[0060]

[0061] Convection term:

[0062]

[0063] in, represents the water depth at spatial position i and time scale j; represents the water depth at spatial position i-1 and time scale j; represents the water depth at spatial position i+1 and time scale j; It represents the suspended sediment concentration at the spatial position i and the time scale j+1; It represents the suspended sediment concentration at spatial position i and time scale j; It represents the suspended sediment concentration at the spatial position i-1 and the time scale j+1; It represents the suspended sediment concentration at the spatial position i+1 and the time scale j+1; represents the flow velocity at spatial position i+1 and time scale j; represents the flow velocity at spatial position i and time scale j; It represents the flow velocity at the spatial position i-1 and the time scale j;

[0064] Substitute the suspended sediment concentration distribution into the bed update equation and use the forward Euler method to iterate and solve. The discrete format is:

[0065]

[0066] in, It represents the sand-carrying force at spatial position i and time scale j; It represents the sand-carrying force at the spatial position i and the time scale j+1;

[0067] The simulated tidal flat profile topography is obtained, and the tidal flat evolution law under the action of waves and currents is analyzed.

[0068] The beneficial effects of the present invention are:

[0069] (1) In the present invention, in terms of computational efficiency, the present invention appropriately simplifies the fluid continuity equation and the wave energy conservation equation under long-period simulation. Compared with the traditional tidal sediment model Delft3D, under the same grid parameters and simulation conditions, the computational time is only 1 / 5 of that of the traditional tidal sediment model, which significantly improves the computational efficiency of the evolution of coastal tidal flat landforms;

[0070] (2) In the present invention, in terms of calculation accuracy, compared with the Delft3D model, the terrain curves of the present invention are almost overlapped year by year, and as the dynamic conditions gradually adapt to the terrain over time, the error has a significant decreasing trend, and the calculation accuracy is almost consistent with Delft3D, with higher simulation accuracy. BRIEF DESCRIPTION OF THE DRAWINGS

[0071] Figure 1 It is a schematic diagram of the overall process of the present invention;

[0072] Figure 2 A schematic diagram of the measured terrain and the model initial terrain in an embodiment of the present invention;

[0073] Figure 3 It is a schematic diagram of the landform evolution process of the tidal flat within 5 years when the wave conditions are not considered in the embodiment of the present invention;

[0074] Figure 4 This is a schematic diagram of the landform evolution process of the tidal flat within 5 years when the wave conditions are considered in the embodiment of the present invention and the effective wave height is 0.3m;

[0075] Figure 5 It is a schematic diagram of the change of the magnitude of the sand-carrying force of the tidal flat within 5 years when the wave conditions are not considered in the embodiment of the present invention;

[0076] Figure 6It is a schematic diagram comparing the results of the model method of the embodiment of the present invention and the traditional tidal sediment model. DETAILED DESCRIPTION

[0077] This embodiment provides a multi-scale wave-current-sediment coupled beach evolution prediction model method, such as Figure 1 As shown, the following steps are included:

[0078] S1. According to the given offshore tidal flat sea area topographic data, a coordinate system is established, and then the hydrological conditions (tidal currents, waves) and sediment conditions of the area are obtained based on the observation stations.

[0079] S2. Construct a wave-current-sediment coupled beach evolution prediction model, which is implemented by tidal current module, wave dynamic module and sediment dynamic module. Construct tidal current module based on the fluid continuity equation with zero gradient on the free surface. Generate wave propagation module based on simplified wave energy conservation equation. Based on the general sediment entrainment force formula, provide the near-bottom sediment flux F required by the one-dimensional average suspended sediment convection diffusion equation. s , combined with the bottom bed renewal equation dominated by the near-bottom sediment flux, a sediment dynamics module is constructed.

[0080] The tidal current dynamics module is based on the fluid continuity equation. It is assumed that at any time, the gradient of the free surface is 0 (i.e., there is no oscillation of the liquid surface), and the momentum equation is ignored. The control equation is as follows:

[0081]

[0082] Where u represents the average velocity in the depth of the tidal flat section, t represents time, and x represents the distance across the shore; water depth h = η-z b , η represents the water surface height, z b Indicates the bed surface elevation.

[0083] The water surface height η function satisfies the following formula:

[0084]

[0085] Where A is the tidal amplitude, T c represents the power flow period, T c =12h.

[0086] The wave power module adopts a simplified phase average model and is composed of a wave power module based on a simplified wave energy conservation equation. The wave energy conservation equation is as follows:

[0087]

[0088] Where E represents wave energy, ρ represents the density of seawater, g represents the acceleration due to gravity, H rmsRepresents the root mean square wave height; S tot represents the total wave energy term, c g is the group velocity, S fric represents the wave bottom friction term, which is the main source of wave energy dissipation near the shore. break represents the wave breaking source term.

[0089] Group velocity c g It represents the propagation speed of wave energy. Based on linear wave theory, it is expressed as follows:

[0090]

[0091] Wherein, c=σ / k represents the phase velocity of the wave, σ represents the wave frequency, and k represents the wave number. The direction of the wave phase velocity in this embodiment is fixed to the shoreward direction.

[0092] Wave bottom friction term S fric As shown below:

[0093]

[0094] Among them, α f represents the wave energy dissipation coefficient, H represents the wave height, T w Represents the wave period.

[0095] When the water depth gradient is large and the wave height exceeds a certain proportion of the water depth, the waves break, as shown in the following formula:

[0096]

[0097] Among them, α represents the constant 1; Qb represents the probability of wave breaking determined by the discriminant index b, H represents wave height, the maximum wave height is H max =0.78h.

[0098] Based on the general sediment entrainment formula, the near-bottom sediment flux F required for the one-dimensional average suspended sediment convection-diffusion equation is provided. s , and combined with the bottom bed renewal equation controlled by the near-bottom sediment flux to form a sediment dynamic module. The sediment model control equation adopts the one-dimensional vertical average suspended sediment convection diffusion equation, which is as follows:

[0099]

[0100] F s =αω(C * -C)

[0101] Where h represents water depth, C represents vertical average sediment content, t represents time, u represents depth average velocity in the tidal flat section, x represents cross-shore distance, ε represents horizontal suspended sediment diffusion coefficient, and F represents the average vertical average sediment content. srepresents the suspended sediment flux near the bottom, α represents the constant 1, ω represents the sediment settling velocity, C * Indicates the sand-holding force.

[0102] Sand holding capacity C * The same dimension as the vertical average sediment content C:

[0103]

[0104] Among them, C D represents the drag coefficient, ρ and ρ s They represent the density of water and sediment respectively, U represents the dynamic factor, and g represents the acceleration due to gravity.

[0105] Drag coefficient C D It is related to the Reynolds number and the bed surface roughness, and is expressed by the Manning formula:

[0106]

[0107] The calculation formula of power factor U is:

[0108]

[0109] Where n represents the roughness, u c represents the tidal flow velocity, u w represents the wave velocity, f c and f w represent the tidal current and wave resistance coefficient f respectively c =gn 2 / h 1 / 3 ,, ξ represents the displacement amplitude of the bottom particles, ξ=u w T w / 2π,T w represents the wave period, k s represents the Nicolaz function value;

[0110] The formula of sand holding force is summarized as follows:

[0111] The near-bottom sediment flux will cause scouring or siltation of the bottom bed, and the bed surface renewal equation is expressed by the following formula:

[0112]

[0113] Where p represents the porosity of the bed sediment, ρ s represents the sediment density, z b Indicates the bed surface elevation.

[0114] S3. Arrange the data obtained in step S1 and use them as boundary conditions to import into the wave-current-sediment coupled beach evolution prediction model. The boundary conditions required by the model are the land boundary and the seaward boundary. The land boundary adopts a closed boundary condition, and the seaward open boundary adopts different boundary conditions according to different equations.

[0115] The tidal equation adopts the Dirichlet boundary condition of flow (the boundary physical quantity is a constant); the wave equation boundary adopts the Dirichlet boundary condition of root mean square wave height; in order to prevent excessive siltation at the boundary, the sediment equation adopts the Dirichlet boundary condition at high tide and the Neumann boundary condition at low tide (the gradient of the boundary physical quantity is a constant).

[0116] S4. The finite difference method is used to iteratively solve the wave-current-sediment coupled beach evolution prediction model to obtain the dynamic evolution process of the tidal flat landform, which specifically includes the following steps:

[0117] S4.1. During the solution process, based on the provided boundary conditions, the tidal dynamics module and the wave propagation module are solved using the finite difference method to calculate the flow velocity and wave velocity distribution on the tidal flat terrain.

[0118] The tidal current dynamic equation includes the time derivative term Where h represents water depth, t represents time, and the time derivative term By directly differentiating the water surface function with respect to time, the equation is transformed into an ordinary differential equation:

[0119]

[0120] Where x represents the cross-shore distance, q represents the flow rate per single width, and the unit is m 2 / s, q = hu, q is discretized by first-order forward difference, u represents the depth-averaged velocity in the tidal flat section direction; i represents the spatial scale, Δx represents the spatial step length, q i+1 represents the single-width flow q value at spatial position i+1, q i Represents the single-width flow q value at spatial position i; when determining the boundary flow q bd =∫Δh(x, t)dx / Δt, the equation is directly solved by iteration, where Δh represents the change in water level and Δt represents the time step.

[0121] S4.2. Substitute the flow velocity and wave velocity distribution obtained from the wave dynamics module and the tidal current dynamics module into the sediment entrainment force formula to calculate the sediment entrainment force, discretely solve the average suspended sediment convection-diffusion equation and the sediment entrainment force formula to obtain the suspended sediment concentration distribution on the tidal flat terrain.

[0122] The wave energy conservation equation in the Wave Power Module includes a convection term The first-order forward difference solution is used in space, and the backward Euler method is used to implicitly solve the equation in the time term. It is unconditionally stable at different time steps and improves the model operation efficiency, as shown in the following formula:

[0123]

[0124] Among them, c g represents the wave group velocity, E represents the wave energy, x represents the cross-shore distance, Δx represents the spatial step, and j represents the time scale. This format requires solving a system of linear equations at each time step. The coefficient matrix is ​​a tridiagonal matrix dominated by the principal diagonal, which can be solved by the Thomas algorithm. It represents the wave energy at spatial position i and time scale j+1; It represents the wave energy at the spatial position i+1 and the time scale j+1; represents the wave energy at spatial position i and time scale j; It represents the group velocity at the spatial position i+1 and the time scale j+1; It represents the group velocity at spatial position i and time scale j+1; Represents the total wave energy at spatial position i and time scale j.

[0125] S4.3. Based on the solved suspended sediment concentration distribution, substitute it into the bed update equation and use the forward Euler method to iterate and solve it to obtain the tidal flat profile topography at different simulation stages.

[0126] Substitute the flow velocity and wave velocity distribution obtained by the wave and tidal dynamics module into the sediment entrainment formula Calculate the sediment entrainment force and solve the suspended sediment concentration distribution based on the embedded average suspended sediment convection-diffusion equation and the sediment entrainment force.

[0127] Among them, the convection term is required when solving the suspended sediment convection-diffusion equation Special processing is performed. Since the tidal current has opposite directions during high and low tides, in order to avoid numerical oscillation, the discretization of the convection term adopts the upwind format, that is, the first-order backward difference is used when the flow velocity u>0 (low tide), and the first-order forward difference is used when the flow velocity u<0 (high tide); the time discretization also adopts the implicit backward Euler method; in order to ensure strict main diagonal dominance, the source term part -αωC less than 0 is linearized implicitly, where α represents the constant 1 and ω represents the sediment settling velocity; the specific discretization format is as follows:

[0128] Time Item:

[0129]

[0130] Diffusion term:

[0131]

[0132] Convection term:

[0133]

[0134] in, represents the water depth at spatial position i and time scale j; represents the water depth at spatial position i-1 and time scale j; represents the water depth at spatial position i+1 and time scale j; It represents the suspended sediment concentration at the spatial position i and the time scale j+1; It represents the suspended sediment concentration at spatial position i and time scale j; It represents the suspended sediment concentration at the spatial position i-1 and the time scale j+1; It represents the suspended sediment concentration at the spatial position i+1 and the time scale j+1; represents the flow velocity at spatial position i+1 and time scale j; represents the flow velocity at spatial position i and time scale j; It represents the flow velocity at the spatial position i-1 and the time scale j;

[0135] Substitute the suspended sediment concentration distribution into the bed update equation and use the forward Euler method to iterate and solve. The discrete format is:

[0136]

[0137] in, It represents the sand-carrying force at spatial position i and time scale j; It represents the sand-carrying force at the spatial position i and the time scale j+1;

[0138] The simulated tidal flat profile topography is obtained, and the tidal flat evolution law under the action of waves and currents is analyzed.

[0139] In this embodiment, the measured section of the tidal flat near the Wanggang River estuary in Jiangsu Province is taken as an example, the profile terrain is simplified, and the initial slope of the model is taken as 0.2%. Figure 2 As shown in the figure, it is a schematic diagram of the measured topography and the initial topography of the model, with an elevation range of -6 to 4 m. The tidal ranges of M2 and S2 in the area are 3.4 m and 1.2 m respectively, and the simplified tidal range is 4 m. Two working conditions, wave and no wave, are considered, the wave period is set to 3s, and the effective wave heights are set to 0 m and 0.3 m respectively. The sediment part provides parameters such as boundary suspended sediment concentration C, diffusion coefficient ε, porosity p, sedimentation velocity ω and density.

[0140] The initial slope of the model is 0.2%, and the calculation grid spacing is 1m, so the bed elevation zb Stored in a 5000*1 grid, take the tidal difference of 4m to get the water surface function Water depth h = η-z b , which constitutes the basic condition for solving the tidal dynamics module.

[0141] wave Given the initial wave heights of 0 and 0.5 m, the results are as follows Figure 3 to Figure 4 As shown, wave bottom friction Wave energy dissipation coefficient α f At a value of 0.015, the wave breaking term The wave breaking probability Qb is determined by the discriminant index b. Constitute the wave power module.

[0142] The sediment transport module is a one-dimensional vertical average suspended sediment convection diffusion equation and a bottom bed renewal equation. According to the sediment conditions, the boundary suspended sediment concentration C is set to 0.3 kg / m 3 , the diffusion coefficient ε is taken as 10m 2 / s, porosity p = 0.5, α is 1, sediment settling velocity ω is 0.0005m / s, sediment density and water density are 1650kg / m 3 With 1000kg / m 3 , thus forming a sediment dynamic module.

[0143] In the tidal dynamic equation It can be obtained by directly derivation of the water surface function with respect to time, q is the single width flow (m 2 / s), q=hu, so the equation is transformed into:

[0144]

[0145] Discrete first-order forward difference iteration to solve variable u c .

[0146] The wave energy conservation equation includes the convection term The first-order forward difference is used to solve the space, and the backward Euler method is used to implicitly solve the equation in the time term to obtain the variable u w .

[0147]

[0148] Calculate the flow velocity u using the wave and tidal dynamics model c , wave speed u w The distribution of the sediment parameters provided is substituted into the sediment-carrying force formula. In the calculation, the sand-carrying force is calculated. The calculation result is as follows: Figure 5As shown, the suspended sediment concentration distribution is calculated based on the average suspended sediment convection-diffusion equation and the obtained sediment entrainment force. Here, the space is discretized, and the first-order backward difference format is used at low tide, and the first-order forward difference format is used at high tide. The time discretization adopts the implicit backward Euler method.

[0149] Finally, the suspended sediment concentration distribution obtained above is substituted into the bed update equation, and the forward Euler method is used to iterate and solve the tidal flat profile topography at different simulation stages, such as Figure 6 As shown, it is a schematic diagram comparing the results of the model method of the embodiment of the present invention and the traditional tidal sediment model. Compared with the Delft3D model, the annual terrain curves are almost coincident, and the error is significantly reduced over time, with higher simulation accuracy.

[0150] This embodiment cites the formula for sediment entrainment as the near-bottom sediment flux. Sediment entrainment refers to the sediment content of a water body under certain water flow and wave conditions. When the sediment content in the water body is different from the sediment entrainment capacity of the water flow, the sediment recovers to consistency (suspended or silted) at a certain rate, so that the sediment content in the water body is adapted to the hydrodynamic conditions.

[0151] The present embodiment provides a multi-scale wave-current-sediment coupled shore evolution prediction model method. According to given offshore tidal flat water area topography data, a coordinate system is established. Then, based on the observation site, the tide, wave, and sediment data of the area are obtained. The data are sorted and used as boundary conditions to import the wave-current-sediment coupled shore evolution prediction model. A tidal flat prediction model based on the integration of tidal flat dynamics, wave motion, and sediment dynamics modules is constructed, and the model parameters required for each module are set. The finite difference method is adopted to solve the fluid continuity equation, the wave energy conservation equation, the one-dimensional vertical average suspended sand convection-diffusion equation, and the bottom bed update equation in the model to obtain the tidal flat profile topography at different simulation stages, and analyze the shore evolution law of the tidal flat profile under the action of waves and currents.

[0152] This embodiment has a sufficient theoretical basis and can more accurately simulate the evolution process of tidal flat profile morphology under the combined action of waves and currents. Compared with the traditional tidal sediment model, it significantly improves the calculation efficiency and simulation accuracy of the evolution of coastal tidal flat morphology.

[0153] In addition to the above embodiments, the present invention may also have other implementation modes. Any technical solution formed by equivalent replacement or equivalent transformation falls within the protection scope required by the present invention.

Claims

1. A multi-scale wave-current-sediment coupled beach evolution prediction model method, characterized by: The following steps are involved: S1. According to the given offshore tidal flat sea area topographic data, a coordinate system is established, and then the tidal, wave and sediment conditions in the area are obtained based on the observation station; S2. Construct a wave-current-sediment coupled shore evolution prediction model, which includes a tidal current power module, a wave power module and a sediment power module; construct a tidal current power module based on a fluid continuity equation with a free surface gradient of 0; and generate a wave propagation module based on a wave energy conservation equation; Based on the sediment entrainment force formula, the near-bottom sediment flux F required for the one-dimensional average suspended sediment convection-diffusion equation is provided. s , combined with the bed renewal equation dominated by the near-bottom sediment flux, a sediment dynamics module is constructed; S3, collating the data obtained in step S1 and using them as boundary conditions to import into the wave-current-sediment coupled beach evolution prediction model; S4. The finite difference method is used to iteratively solve the wave-current-sediment coupled beach evolution prediction model to obtain the dynamic evolution process of tidal flat landform morphology.

2. A multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 1, characterized in that: In step S2, the tidal power module is based on the fluid continuity equation. It is assumed that at any time, the gradient of the free surface is 0, that is, there is no oscillation of the liquid surface. The momentum equation is ignored, and the control equation is as follows: Where u represents the average velocity in the depth of the tidal flat section, t represents time, and x represents the distance across the shore; water depth h = η-z b , η represents the water surface height, z b Indicates the bed elevation; The water surface height η function satisfies the following formula: Where A is the tidal amplitude, T c represents the power flow period, T c =12h.

3. A multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 2, characterized in that: In step S2, a wave power module is formed based on the wave energy conservation equation, and the wave energy conservation equation is as follows: Where E represents wave energy, ρ represents the density of seawater, g represents the acceleration due to gravity, H rms Represents the root mean square wave height; S tot represents the total wave energy term, c g is the group velocity, S fric represents the wave bottom friction term, S break represents the wave breaking source term; Group velocity c g It represents the propagation speed of wave energy. Based on linear wave theory, it is expressed as follows: Where c = σ / k represents the phase velocity of the wave, σ represents the wave frequency, k represents the wave number, and the direction of the wave phase velocity is fixed to the shoreward direction; Wave bottom friction term S fric As shown below: Among them, α f represents the wave energy dissipation coefficient, H represents the wave height, T w represents the wave period; When the water depth gradient is large and the wave height exceeds a certain proportion of the water depth, the waves break, as shown in the following formula: Among them, α represents the constant 1; Qb represents the probability of wave breaking determined by the discriminant index b, H represents wave height, the maximum wave height is H max =0.78h.

4. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 1, characterized in that: In step S2, starting from the sediment entrainment force formula, the near-bottom sediment flux F required by the one-dimensional average suspended sediment convection diffusion equation is provided. s , and combined with the bottom bed renewal equation controlled by the near-bottom sediment flux to form a sediment dynamic module. The sediment model control equation adopts the one-dimensional vertical average suspended sediment convection diffusion equation, which is as follows: F s =αω(C * -C) Where h represents water depth, C represents vertical average sediment content, t represents time, u represents depth average velocity in the tidal flat section, x represents cross-shore distance, ε represents horizontal suspended sediment diffusion coefficient, and F represents the average vertical average sediment content. s represents the suspended sediment flux near the bottom, α represents the constant 1, ω represents the sediment settling velocity, and C* represents the sediment entrainment force; The near-bottom sediment flux will cause scouring or siltation of the bottom bed, and the bed surface renewal equation is expressed by the following formula: Where p represents the porosity of the bed sediment, ρ s represents the sediment density, z b Indicates the elevation of the bed surface.

5. A multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 4, characterized in that: The sand-carrying capacity C* has the same dimension as the vertical average sand content C: Among them, C D represents the drag coefficient, ρ and ρ s They represent the density of water and sediment respectively, U represents the dynamic factor, and g represents the acceleration due to gravity; Drag coefficient C D It is related to the Reynolds number and the bed surface roughness, and is expressed by the Manning formula: The calculation formula of power factor U is: Where n represents the roughness, u c represents the tidal flow velocity, u w represents the wave velocity, f c and f w represent the tidal current and wave resistance coefficient f respectively c =gn 2 / h 1 / 3 ,, ξ represents the displacement amplitude of the bottom particles, ξ=u w T w / 2π,T w represents the wave period, k s represents the Nicolaz function value; The formula of sand holding force is summarized as follows:

6. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 1, characterized in that: In step S3, the boundary conditions required by the wave-current-sediment coupled beach evolution prediction model are the land boundary and the seaward boundary. The land boundary adopts a closed boundary condition, and the seaward open boundary adopts different boundary conditions according to different equations. The tidal equation adopts the Dirichlet boundary condition of flow, and the boundary physical quantity is a constant; the wave equation boundary adopts the Dirichlet boundary condition of root mean square wave height; the sediment equation adopts the Dirichlet boundary condition at high tide and the Neumann boundary condition at low tide, and the gradient of the boundary physical quantity is a constant.

7. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 1, characterized in that: The step S4 specifically includes the following sub-steps: S4.

1. Based on the provided boundary conditions, solve the tidal dynamics module and wave propagation module using the finite difference method to calculate the flow velocity and wave velocity distribution on the tidal flat terrain; S4.

2. Substitute the velocity and wave velocity distribution obtained from the wave dynamics module and the tidal current dynamics module into the sediment entrainment force formula to calculate the sediment entrainment force, discretely solve the average suspended sediment convection diffusion equation and the sediment entrainment force formula, and obtain the suspended sediment concentration distribution on the tidal flat terrain; S4.

3. Based on the solved suspended sediment concentration distribution, substitute it into the bed update equation and use the forward Euler method to iterate and solve it to obtain the tidal flat profile topography at different simulation stages.

8. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 7, characterized in that: In step S4.1, the tidal current dynamic equation includes the time derivative term Where h represents water depth, t represents time, and the time derivative term By directly differentiating the water surface function with respect to time, the equation is transformed into an ordinary differential equation: Where x represents the cross-shore distance, q represents the flow rate per single width, and the unit is m 2 / s, q = hu, q is discretized by first-order forward difference, u represents the depth-averaged velocity in the tidal flat section direction; i represents the spatial scale, Δx represents the spatial step length, q i+1 represents the single-width flow q value at spatial position i+1, q i Represents the single-width flow q value at spatial position i; when determining the boundary flow q bd =∫Δh(x, t)dx / Δt, the equation is directly solved by iteration, where Δh represents the change in water level and Δt represents the time step.

9. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 7, characterized in that: In step S4.2, the wave energy conservation equation in the wave power module includes the convection term The first-order forward difference is used to solve the space, and the backward Euler method is used to implicitly solve the equation in the time term: Among them, c g represents the wave group velocity, E represents the wave energy, x represents the cross-shore distance, Δx represents the spatial step size, and j represents the time scale; It represents the wave energy at spatial position i and time scale j+1; It represents the wave energy at the spatial position i+1 and the time scale j+1; represents the wave energy at spatial position i and time scale j; It represents the group velocity at the spatial position i+1 and the time scale j+1; It represents the group velocity at spatial position i and time scale j+1; Represents the total wave energy at spatial position i and time scale j.

10. The multi-scale wave-current-sediment coupled beach evolution prediction model method according to claim 7, characterized in that: In step S4.3, the suspended sediment convection diffusion equation in the sediment dynamics module includes the convection term Where h represents the water depth, u represents the average velocity in the depth of the tidal flat section, C represents the vertical average sediment content, and x represents the cross-shore distance; the discretization of the convection term adopts the upwind format, that is, the first-order backward difference is used when the tide u>0, and the first-order forward difference is used when the tide u<0; the time discretization also adopts the implicit backward Euler method; the source term part less than 0 -αωC is linearized implicitly, where α represents the constant 1 and ω represents the sediment settling velocity; the specific discretization format is as follows: Time Item: Diffusion term: Convection term: in, represents the water depth at spatial position i and time scale j; represents the water depth at spatial position i-1 and time scale j; represents the water depth at spatial position i+1 and time scale j; It represents the suspended sediment concentration at the spatial position i and the time scale j+1; It represents the suspended sediment concentration at spatial position i and time scale j; It represents the suspended sediment concentration at the spatial position i-1 and the time scale j+1; It represents the suspended sediment concentration at the spatial position i+1 and the time scale j+1; represents the flow velocity at spatial position i+1 and time scale j; represents the flow velocity at spatial position i and time scale j; It represents the flow velocity at the spatial position i-1 and the time scale j; Substitute the suspended sediment concentration distribution into the bed update equation and use the forward Euler method to iterate and solve. The discrete format is: in, It represents the sand-carrying force at spatial position i and time scale j; It represents the sand-carrying force at the spatial position i and the time scale j+1; The simulated tidal flat profile topography is obtained, and the tidal flat evolution law under the action of waves and currents is analyzed.

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