CN110543688B - Hydrological model confluence method of multi-blocking two-dimensional diffusion wave equation under reservoir group regulation - Google Patents

Hydrological model confluence method of multi-blocking two-dimensional diffusion wave equation under reservoir group regulation Download PDF

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CN110543688B
CN110543688B CN201910716827.5A CN201910716827A CN110543688B CN 110543688 B CN110543688 B CN 110543688B CN 201910716827 A CN201910716827 A CN 201910716827A CN 110543688 B CN110543688 B CN 110543688B
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董宁澎
余钟波
杨传国
徐伟
董增川
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Abstract

The invention discloses a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation, which comprises the following steps: (1) Collecting related data in a research area, and determining a dispatching rule, a regulation and storage node and an upstream water collecting area range of a reservoir; (2) Calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity according to the scheduling rule and the regulation and storage node of the large reservoir, and constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir; (3) According to the dispatching rule and the regulation and storage node of the large reservoir, a two-dimensional diffusion wave equation set of a downstream grid of the reservoir is constructed; (4) According to the regulation nodes and the dispatching rules of the small reservoir, a two-dimensional diffusion wave equation set of the grid where the small reservoir is located is constructed; (5) And performing basin confluence calculation on the equation set to obtain a final confluence result. The invention can improve the model structure of the distributed hydrological model, thereby realizing the simulation of the confluence process under the regulation and storage of the reservoir group and improving the simulation precision of the hydrological model.

Description

Hydrological model confluence method of multi-blocking two-dimensional diffusion wave equation under reservoir group regulation
Technical Field
The invention relates to the technical field of hydrological model confluence, in particular to a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation.
Background
The reservoir is a tool for scientifically, actively and reasonably developing, utilizing and storing water resources and changing regional water circulation rules by human beings. Wherein, the number of large and medium-sized reservoirs (hereinafter collectively referred to as large reservoirs) is relatively small, but the regulation and storage capacity is strong, and the hydrological effect is obvious; the small reservoirs are widely and densely distributed, but the regulation capacity and the hydrological effect are relatively weak, and the reservoir group is the combination of the two.
According to the 'nature-society' binary water resource theory, the watershed reservoir groups can obviously influence the cyclic conversion speed between surface water and underground water, and change the rules of hydrologic cyclic evolution and updating. As an important tool for researching hydrologic cycle, the hydrologic model can simulate the space-time distribution of watershed water resources through modules such as runoff generation, confluence, underground water and the like. Limited by the limitation of computational power, early hydrological models are mostly based on lumped or semi-distributed structures, and simplified convergence calculation methods such as unit lines, linear reservoirs, ma Sijing are adopted. With the development of computer technology, fully distributed models are gradually developed, and such models usually use a river course grid as a computing unit, and perform convergence calculation directly through a discrete one-dimensional saint-venin equation set or a simplified form thereof.
In recent years, the concept of traditional river channel convergence is abandoned by a partial distributed hydrological model, and convergence calculation is carried out on a full-basin grid by adopting a two-dimensional diffusion wave equation. However, due to the regulation of the reservoir group, the hydraulic connection between the upstream and downstream of the natural river is broken, the river flow no longer has continuity, and the two-dimensional diffusion wave equation cannot be applied here. Under the background, because a current hydrological model confluence calculation method of two-dimensional diffusion waves under reservoir group regulation is lacked, the influence of the reservoir group regulation on a confluence process is ignored by the model, the hydrological effect of a hydraulic engineering group cannot be described, and the interaction between a reservoir group consisting of large, medium and small reservoirs and water circulation is difficult to reflect on a physical mechanism.
Disclosure of Invention
The purpose of the invention is as follows: in order to overcome the defects of the prior art, the invention provides a hydrological model confluence method for blocking a two-dimensional diffusion wave equation more under reservoir group regulation.
The technical scheme is as follows: the invention relates to a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation, which comprises the following steps:
(1) Collecting the storage capacity, longitude and latitude coordinates, vector river network files and scheduling rule data of a large reservoir in a research area, establishing grid point coordinates, and determining scheduling rules, regulation and storage nodes and upstream catchment area ranges of the large reservoir; collecting the storage capacity and longitude and latitude coordinates of the small reservoir in the research area, establishing grid point coordinates, and determining a scheduling rule and a regulation and storage node of the small reservoir;
(2) Calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity according to the scheduling rule and the regulation and storage node of the large reservoir, and constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir according to the change of the corresponding water surface elevation;
(3) Determining the inflow rate of the reservoir according to the regulation and storage nodes of the large reservoir, and calculating the discharge rate of the reservoir by using the dispatching rule of the large reservoir, wherein the dispatching rule can adopt the collected actual dispatching rule or the conceptualized dispatching rule obtained by generalization. Constructing a two-dimensional diffusion wave equation set of the downstream grids of the reservoir according to the above;
(4) Determining the inflow rate of the reservoir according to the regulation nodes of the small reservoir, calculating the regulation and storage effect of the small reservoir on the runoff by using the dispatching rules of the large reservoir, and generalizing the regulation and storage effect into a source and sink item of a grid where the small reservoir is located, wherein the dispatching rules can adopt collected actual dispatching rules or generalized conceptual dispatching rules. Constructing a two-dimensional diffusion wave equation set of the grid where the small reservoir is located;
(5) And (5) performing basin confluence operation on the equation sets from the step (2) to the step (4) to obtain a final confluence result.
Further, comprising:
in the step (2), calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity, and expressing the change as follows:
Figure BDA0002155722390000021
wherein O is the outlet flow of the large reservoir, I is the inlet flow of the reservoir, A w Dt is the time step for the upstream grid surface area.
Further, comprising:
in the step (2), a two-dimensional diffusion wave equation set of the upstream grid of the reservoir is constructed, namely:
Figure BDA0002155722390000022
Figure BDA0002155722390000023
Figure BDA0002155722390000031
wherein H 'is the water surface elevation of the upstream grid under reservoir regulation, H' = H + delta H, u and v are the flow velocity in the x direction and the y direction respectively, H is the water surface elevation of the upstream grid under the natural condition,
Figure BDA0002155722390000032
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the time direction is obtained,
Figure BDA0002155722390000033
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the x direction is obtained,
Figure BDA0002155722390000034
the partial derivative of the elevation of the water surface of the upstream grid under reservoir regulation in the y direction is shown, D is the water depth of the upstream grid, g is the gravity acceleration, and K is the flow modulus.
Further, it includes:
in the step (3), a two-dimensional diffusion wave equation set of the downstream grid of the reservoir is constructed and expressed as:
Figure BDA0002155722390000035
Figure BDA0002155722390000036
Figure BDA0002155722390000037
wherein, V x 、V y The flow velocities of the large reservoir discharge flow in the x direction and the y direction respectively, u and v are the flow velocities in the x direction and the y direction respectively, A w Is the water surface area of the downstream grid, H is the water surface elevation of the downstream grid under the natural condition,
Figure BDA0002155722390000038
the partial derivative in time of the downstream grid water surface elevation in the natural situation,
Figure BDA0002155722390000039
the partial derivative in the x direction of the downstream grid water surface elevation in the natural situation,
Figure BDA00021557223900000310
the method is characterized in that the partial derivative of the elevation of the water surface of a downstream grid in the y direction under the natural condition is shown, D is the water depth of the downstream grid, g is the gravity acceleration, K is the flow modulus, and O is the outflow of a large reservoir.
Further, comprising:
in the step (4), the regulation and storage function of the small reservoir to the runoff is calculated according to the regulation and storage node and the dispatching rule of the small reservoir, and is generalized to the source and sink item of the grid where the small reservoir is located, and the source and sink item is expressed as:
Figure BDA0002155722390000041
wherein S is a source exchange item caused by reservoir regulation, O ' is the outlet flow of the small reservoir, I ' is the inlet flow of the small reservoir, A ' w The area of the water surface of the grid where the small reservoir is located.
Further, it includes:
in the step (4), a two-dimensional diffusion wave equation set of the grid where the small reservoir is located is constructed, and the method comprises the following steps:
Figure BDA0002155722390000042
Figure BDA0002155722390000043
Figure BDA0002155722390000044
wherein H' is the water surface elevation of the grid under the regulation and storage of the small reservoir,
Figure BDA0002155722390000045
the partial derivative of the grid water surface elevation in the time direction under the regulation and storage of the small reservoir,
Figure BDA0002155722390000046
the partial derivative of the grid water surface elevation in the x direction under the regulation and storage of the small reservoir,
Figure BDA0002155722390000047
the partial derivative of the grid water surface elevation in the y direction under the regulation and storage of the small reservoir is obtained; d ' is the water depth of the grid where the small reservoir is located, g is the gravity acceleration, K is the flow modulus, and u ' and v ' are the flow velocities in the x direction and the y direction respectively; v' x ,V' y The flow rates of the small reservoir discharge in the x direction and the y direction are respectively, and A is the area of the water cross section.
Has the advantages that: the model structure of the distributed hydrological model can be perfected by constructing the hydrological model convergence method of the multi-blocking two-dimensional diffusion wave equation under the regulation and storage of the reservoir group, so that the simulation of the convergence process under the regulation and storage of the reservoir group is realized, the simulation precision of the hydrological model is improved, the regional hydrological process under the influence of the reservoir group is quantized, the evolution rule of the regional hydrological process is revealed, theoretical guidance is provided for the development and utilization of regional water resources, and the method has important practical value.
Drawings
FIG. 1 is a schematic flow diagram of a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation;
FIG. 2 is the observed value of the monthly runoff, the simulated value of the model under the condition of no reservoir, and the simulated value of the model considering the process of regulating and storing the runoff of the reservoir group in the Ganjiang river upstream river of 1978-1986.
Detailed Description
(1) Collecting reservoir group data of a research area: collecting the storage capacity and longitude and latitude coordinates of a large reservoir and a small reservoir in a research area, and digital elevation models and vector river network data of a drainage basin from a water conservancy department respectively, and determining a regulation node of the reservoir in a hydrological model and a catchment area range of the upstream of the reservoir, wherein if the longitude and latitude coordinate data are incomplete, the longitude and latitude positions of the reservoir can be determined by using remote sensing images; collecting the scheduling rule data of the reservoir group, if the data are not complete, determining the specific position of the reservoir by using the remote sensing image, and approximating the actual scheduling rule of the reservoir by using the conceptual scheduling rule or the optimized scheduling rule.
(2) Dividing sub-basins according to a large reservoir: and converting the longitude and latitude coordinates of the large reservoir into grid point coordinates of a hydrological model according to the collected longitude and latitude coordinates of the large reservoir and the vector river network file, ensuring that the reservoir is positioned in the river network, and determining the regulation and storage nodes of the large reservoir. And processing the watershed digital elevation model, determining the boundary longitude and latitude coordinates of each reservoir water collection area (namely the upstream watershed of the reservoir regulation and storage node), converting the boundary longitude and latitude coordinates into grid point coordinates of the hydrological model, and independently dividing the boundary longitude and latitude coordinates into sub watersheds of the research area in the hydrological model and coding the sub watersheds. Keeping the upstream watershed and the downstream watershed of the reservoir relatively independent, and taking the reservoir as a coupling node of the upstream watershed and the downstream watershed;
(3) Constructing a two-dimensional diffusion wave equation of regulation and storage influence upstream of the large reservoir: calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity according to the collected large reservoir dispatching rules and the storage regulation nodes, and constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir according to the assumption that the momentum is unchanged; the method comprises the following specific steps:
calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity, and expressing as:
Figure BDA0002155722390000051
wherein O is the output flow of the large reservoir and is determined by reservoir dispatching rules, I is the input flow of the reservoir, and A w Dt is the time step for the upstream grid surface area.
Further, comprising: constructing a two-dimensional diffusion wave equation set of the reservoir upstream grid, namely:
Figure BDA0002155722390000052
Figure BDA0002155722390000053
Figure BDA0002155722390000061
wherein H 'is the water surface elevation of the upstream grid under reservoir regulation, H' = H + delta H, u and v are the flow velocity in the x direction and the y direction respectively, H is the water surface elevation of the upstream grid under the natural condition,
Figure BDA0002155722390000062
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the time direction is obtained,
Figure BDA0002155722390000063
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the x direction is obtained,
Figure BDA0002155722390000064
and D is the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the y direction, D is the water depth of the upstream grid, g is the gravity acceleration, and K is the flow modulus.
(4) Constructing a two-dimensional diffusion wave equation of the large reservoir regulation influence downstream: determining the inlet flow of the reservoir according to the regulation and storage nodes of the large reservoir, calculating the discharge flow of the reservoir by using the dispatching rule of the large reservoir, and taking the discharge flow as a source exchange item of the downstream grid of the reservoir, wherein the dispatching rule can adopt the collected actual dispatching rule or the generalized conceptual dispatching rule. And constructing a two-dimensional diffusion wave equation set of the downstream grid of the reservoir according to the equation, wherein the equation comprises a continuity equation and a momentum equation, namely:
Figure BDA0002155722390000065
Figure BDA0002155722390000066
Figure BDA0002155722390000067
wherein, V x 、V y The flow rates of the large reservoir discharge in the x direction and the y direction are respectively, the free discharge is assumed, the calculation is carried out according to the free discharge formula, u and v are the flow rates in the x direction and the y direction respectively, A w Is the water surface area of the downstream grid, H is the water surface elevation of the downstream grid under the natural condition,
Figure BDA0002155722390000068
the partial derivative in time of the downstream grid water surface elevation in the natural situation,
Figure BDA0002155722390000069
the partial derivative in the x direction of the downstream grid water surface elevation in the natural situation,
Figure BDA00021557223900000610
the partial derivative of the elevation of the water surface of the downstream grid in the y direction under the natural condition is shown, D is the water depth of the downstream grid, g is the gravity acceleration, K is the flow modulus, and O is the outflow of the large reservoir.
(5) Constructing a two-dimensional diffusion wave equation under the influence of regulation and storage of the small reservoir group: and converting the longitude and latitude coordinates of the small reservoir into grid point coordinates of a hydrological model according to the collected longitude and latitude coordinates of the small reservoir, and determining a regulation and storage node of the reservoir in the model. Determining the inflow rate of the reservoir according to the regulation nodes of the small reservoir, calculating the regulation and storage effect of the small reservoir on the runoff by utilizing the dispatching rule of the large reservoir, and approximately generalizing the regulation and storage effect into a source collection item of a grid where the small reservoir is located, wherein the dispatching rule can adopt the collected actual dispatching rule or a conceptualized dispatching rule obtained by generalization. In the process, the continuity of water flow is maintained, and a two-dimensional diffusion wave equation set of the grid where the reservoir is located is constructed according to the continuity; the method comprises the following specific steps:
calculating the regulation and storage function of the small reservoir to the runoff, and approximating the regulation and storage function to a source and sink item of a grid where the regulation and storage function is located:
Figure BDA0002155722390000071
wherein S is a source sink item caused by reservoir regulation, O ' is the outlet flow of the small reservoir, I ' is the inlet flow of the small reservoir, A ' w The area of the water surface of the grid where the small reservoir is located. When the inflow of the reservoir is larger than the outflow, a part of runoff in the period is transferred out of the watershed confluence process; when the outflow of the reservoir is larger than the inflow, a part of runoff in the period is additionally added into the watershed converging process.
And maintaining the continuity of the water flow in the process, and constructing a corresponding two-dimensional diffusion wave equation system according to the continuity equation and the momentum equation, wherein the two-dimensional diffusion wave equation system comprises the following steps:
Figure BDA0002155722390000072
Figure BDA0002155722390000073
Figure BDA0002155722390000074
wherein H' is the elevation of the grid water surface under the regulation and storage of the small reservoir,
Figure BDA0002155722390000075
the partial derivative of the grid water surface elevation in the time direction under the regulation and storage of the small reservoir,
Figure BDA0002155722390000076
the partial derivative of the grid water surface elevation in the x direction under the regulation and storage of the small reservoir,
Figure BDA0002155722390000081
the partial derivative of the grid water surface elevation in the y direction under the regulation and storage of the small reservoir is obtained; d ' is the water depth of the grid where the small reservoir is located, g is the gravity acceleration, K is the flow modulus, u ' and V ' are the flow velocity in the x and y directions, V ' respectively ' x ,V' y The flow rates of the small reservoir discharge in the x direction and the y direction are respectively, and A is the area of the water cross section.
(6) Solving a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation: in the hydrological model, in order to ensure the stability of the solution, the two-dimensional diffusion wave equation set can be respectively solved in each sub-flow domain determined in (2) by adopting an explicit difference with a time step of about 5 minutes or an implicit difference with a time step of half an hour. When the later equation is adopted, the equation set becomes a group of n linear equations of the next time step, wherein n is the grid number, then sparse matrix solving methods such as a bidirectional conjugate gradient iteration method and the like can be adopted for solving, basin convergence calculation is carried out, and a final convergence result is obtained. Therefore, a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation is established.
To judge the effectiveness of the present invention, the following experiments were made:
the invention provides a hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under regulation and storage of a reservoir group, which comprises the steps of firstly dividing an upstream basin and a downstream basin of a large reservoir into relatively independent sub-basins according to regulation and storage nodes of the large reservoir according to the characteristics of small number and strong regulation and storage capacity of the large reservoir, and calculating the changes of upstream water surface elevation and lower discharge quantity of the reservoir by utilizing a scheduling rule to construct the multi-blocking two-dimensional diffusion wave equation under regulation and storage of the large reservoir; and secondly, aiming at the characteristics that the small reservoirs are large in number, high in density and difficult to obtain in water collecting areas, the regulation and storage effects of the reservoirs on the runoff are calculated according to the regulation and storage nodes and the regulation and storage rules, a two-dimensional diffusion wave equation under the regulation and storage of the small reservoirs is constructed, and the two-dimensional diffusion wave equation are used for the confluence calculation of hydrological models under the regulation and storage of the reservoir groups. The invention effectively makes up the defect that the existing hydrological model adopting two-dimensional diffusion wave equation to carry out confluence calculation cannot simulate the confluence process under reservoir group regulation, and can perfect the model structure of the distributed hydrological model, thereby realizing the simulation of the confluence process under reservoir group regulation, improving the simulation precision of the hydrological model, and having important values in the aspects of revealing the influence rule of the reservoir group on hydrological circulation and guiding the development and utilization of regional water resources.
In this embodiment, the drainage basin at the upstream of the Jiangxiang river is taken as a research area, and is dispersed into 1188 grids, a distributed Hydrologic Model System (HMS) of the research area in a natural state is established, and the Model performs convergence calculation through a two-dimensional diffusion wave equation. A reservoir group consisting of 8 large reservoirs and 432 small reservoirs is built in the watershed, and the runoff process of the watershed outlet section is obviously influenced by the storage regulation function of the reservoir group. Therefore, in order to quantify the influence of the reservoir group on the runoff process and improve the simulation precision, the hydrological model convergence method of the multi-blocking two-dimensional diffusion wave equation under reservoir group regulation is introduced into the HMS, and the model convergence calculation under reservoir group regulation is realized.
The embodiment comprises the following steps:
s1, collecting reservoir group data of a research area: collecting HYDO1K DEM digital elevation models of Ganjiang upstream drainage basin from USGS; the reservoir capacity of 440 reservoirs in the research area, the scheduling rule data of 8 large-scale reservoirs in the research area and the vector river network data of the river basin are collected from the Water and interest agency in Jiangxi province.
Due to the lack of longitude and latitude coordinates and scheduling rule data of the small reservoir, water surface information is extracted by utilizing Landset-8 satellite remote sensing images, longitude and latitude coordinates of 432 small reservoirs are determined, and the actual scheduling rule of the reservoir is replaced by the conceptual scheduling rule. In this embodiment, the following conceptual scheduling rule is adopted:
Figure BDA0002155722390000091
wherein Q is t For reservoir discharge, U is the human water demand, determined by water resources communique, V t For the current reservoir storage capacity, V d 、V c Respectively a dead storage capacity and a Xingli storage capacity, wherein 20 percent and 65 percent of the storage capacity are respectively taken, and r is a coefficient;
s2, dividing sub-basins according to the large reservoir: and (3) converting the longitude and latitude coordinates of the reservoir into grid point coordinates of an HMS model according to the collected longitude and latitude coordinates and vector river network files of the large reservoir in the step (1), ensuring that the reservoir is positioned in the river network, and determining the regulation and storage nodes of the large reservoir. The method comprises the steps of analyzing a HYDRO1K DEM digital elevation model by using an ARCGIS, determining boundary longitude and latitude coordinates of 8 large reservoir water collection areas (namely upstream drainage areas of reservoir regulation and storage nodes), converting the boundary longitude and latitude coordinates into grid point coordinates of HMS by using a lamb set subprogram, dividing 8 sub drainage areas in a hydrological model together and independently, and coding. Keeping the upstream watershed and the downstream watershed of 8 large-scale reservoirs relatively independent, and taking the reservoirs as coupling nodes of the upstream watershed and the downstream watershed;
s3, constructing a two-dimensional diffusion wave equation of the regulation and storage influence upstream of the large reservoir: calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity according to the large reservoir dispatching rule and the regulation node collected in the step (1), and assuming that the momentum is unchanged, and constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir according to the change of the corresponding water surface elevation; the method comprises the following specific steps:
calculating the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity, and expressing as:
Figure BDA0002155722390000092
wherein O is macrowaterThe reservoir outlet flow is determined by reservoir dispatching rules, I is the inlet flow of the reservoir, A w Obtaining the water surface area of the upstream grid from an HMS model database, wherein dt is a time step length, and taking half an hour in the HMS model.
Further, comprising: constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir, namely:
Figure BDA0002155722390000101
Figure BDA0002155722390000102
Figure BDA0002155722390000103
wherein H 'is the water surface elevation of the upstream grid under reservoir regulation, H' = H + delta H, u and v are the flow velocity in the x direction and the y direction respectively, H is the water surface elevation of the upstream grid under the natural condition,
Figure BDA0002155722390000104
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the time direction is obtained,
Figure BDA0002155722390000105
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the x direction is obtained,
Figure BDA0002155722390000106
and D is the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the y direction, D is the upstream water depth, g is the gravity acceleration, and K is the flow modulus. The variables are all from the HMS model database or calculated by the model.
S4, constructing a two-dimensional diffusion wave equation of the regulation and storage influence downstream of the large reservoir: determining the inflow rate of the reservoir according to the large reservoir regulation and storage nodes collected in the step (1), calculating the discharge rate of the reservoir according to the scheduling rules collected in the step (1), and taking the discharge rate as a source and sink item of the downstream grids of the reservoir, thereby constructing a two-dimensional diffusion wave equation set of the downstream grids of the reservoir, wherein the two-dimensional diffusion wave equation set comprises a continuity equation and a momentum equation, namely the continuity equation and the momentum equation
Figure BDA0002155722390000107
Figure BDA0002155722390000108
Figure BDA0002155722390000109
Wherein, V x 、V y The flow rates of the large reservoir discharge in the x direction and the y direction are respectively, the free discharge is assumed, the calculation is carried out according to the free discharge formula, u and v are the flow rates in the x direction and the y direction respectively, A w Is the water surface area of the downstream grid, H is the water surface elevation of the upstream grid under the natural condition,
Figure BDA0002155722390000111
the partial derivative of the upstream grid water surface elevation in the time direction in the natural situation,
Figure BDA0002155722390000112
the partial derivative in the x direction of the upstream grid water surface elevation in the natural situation,
Figure BDA0002155722390000113
the method is characterized in that the partial derivative of the elevation of the water surface of an upstream grid in the y direction under the natural condition is shown, D is the depth of downstream water, g is the gravity acceleration, K is the flow modulus, and O is the outflow of a large reservoir.
S5, constructing a two-dimensional diffusion wave equation under the influence of regulation and storage of the small reservoir group: and (3) converting the longitude and latitude coordinates of the small reservoir into HMS grid point coordinates according to the collected longitude and latitude coordinates of the small reservoir in the step (1), and determining a storage regulation node of the reservoir in the HMS model. Determining the inflow rate of the reservoir according to the obtained regulation nodes, calculating the regulation and storage functions of the small reservoir on the runoff by using the small reservoir scheduling rules collected in the step (1), and approximating and generalizing the regulation and storage functions into the source and sink items of the grid where the small reservoir is located. In the process, the continuity of water flow is maintained, and a two-dimensional diffusion wave equation set of the grid where the reservoir is located is constructed according to the continuity; the method comprises the following specific steps:
calculating the regulation and storage function of the small reservoir to the runoff, and approximating the regulation and storage function to a source and sink item of a grid where the regulation and storage function is located:
Figure BDA0002155722390000114
wherein S is a source sink item caused by reservoir regulation, O ' is the outlet flow of the small reservoir, I ' is the inlet flow of the small reservoir, A ' w The area of the water surface of the grid where the small reservoir is located. When the inflow of the reservoir is larger than the outflow, a part of runoff in the period is transferred out of the watershed confluence process; when the outflow of the reservoir is larger than the inflow, a part of runoff in the period is additionally added into the watershed converging process.
And maintaining the continuity of the water flow in the process, and constructing a corresponding two-dimensional diffusion wave equation system according to the continuity equation and the momentum equation, wherein the two-dimensional diffusion wave equation system comprises the following steps:
Figure BDA0002155722390000115
Figure BDA0002155722390000116
Figure BDA0002155722390000117
wherein H' is the water surface elevation of the grid under the regulation and storage of the small reservoir,
Figure BDA0002155722390000121
deviation of grid water surface elevation in time direction under regulation and storage of small reservoirThe number of the first and second groups is counted,
Figure BDA0002155722390000122
the partial derivative of the grid water surface elevation in the x direction under the regulation and storage of the small reservoir,
Figure BDA0002155722390000123
the partial derivative of the grid water surface elevation in the y direction under the regulation and storage of the small reservoir is obtained; d ' is the water depth of the grid where the small reservoir is located, g is the gravity acceleration, K is the flow modulus, u ' and V ' are the flow velocity in the x and y directions, V ' respectively ' x ,V' y The flow rates of the small reservoir discharge flow in the x direction and the y direction are respectively, A is the water passing section area, and the rest symbols are the same as above and are obtained from an HMS model database or calculated by a model.
S6, solving a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation: in the distributed hydrological model HMS, in order to ensure the solving stability, the two-dimensional diffusion wave equation set is respectively solved in each sub-flow domain determined in the step (2) by adopting the time implicit difference with the time step length of half an hour. The equation set becomes a set of 1188 linear equations of the next time step, wherein 1188 is the grid number, then a bidirectional conjugate gradient iteration method is adopted to solve, the drainage basin convergence calculation is performed, and the final convergence result of the outlet section of the Ganjiang upstream drainage basin is obtained.
The simulation method effectively makes up the defect that the distributed hydrological model HMS cannot simulate the converging process under the regulation and storage of the reservoir group, and perfects the model structure of the HMS, thereby realizing the simulation of the converging process of the Ganjiang river upstream drainage basin under the regulation and storage of the reservoir group. The method can also obviously improve the simulation precision of the lunar runoff of the model in the Ganjiang upstream drainage basin. As shown in FIG. 2, by considering the influence of reservoir group regulation on the confluence process through the application of the method, the Nash efficiency coefficient (NSE) of the runoff simulation value of the Ganjiang upstream drainage basin in 1978-1986 is improved to 0.97 from 0.93, and the significance level of the paired T test is passed by 95%. In addition, the method has important values in the aspects of revealing the influence rule of the reservoir group on the hydrological cycle of the Ganjiang upstream drainage basin and guiding the development and utilization of water resources of the Ganjiang upstream drainage basin.
It is to be noted that, in this document, relational terms such as first and second, and the like are used solely to distinguish one entity or operation from another entity or operation without necessarily requiring or implying any actual such relationship or order between such entities or operations.
As will be appreciated by one skilled in the art, embodiments of the present application may be provided as a method, system, or computer program product. Accordingly, the present application may take the form of an entirely hardware embodiment, an entirely application embodiment, or an embodiment combining application and hardware aspects. Furthermore, the present application may take the form of a computer program product embodied on one or more computer-usable storage media (including, but not limited to, disk storage, CD-ROM, optical storage, and the like) having computer-usable program code embodied therein.
The present invention is described with reference to flowchart illustrations and/or block diagrams of methods, apparatus (systems), and computer program products according to embodiments of the invention. It will be understood that each flow and/or block of the flow diagrams and/or block diagrams, and combinations of flows and/or blocks in the flow diagrams and/or block diagrams, can be implemented by computer program instructions. These computer program instructions may be provided to a processor of a general purpose computer, special purpose computer, embedded processor, or other programmable data processing apparatus to produce a machine, such that the instructions, which execute via the processor of the computer or other programmable data processing apparatus, create means for implementing the functions specified in the flowchart flow or flows and/or block diagram block or blocks.
These computer program instructions may also be stored in a computer-readable memory that can direct a computer or other programmable data processing apparatus to function in a particular manner, such that the instructions stored in the computer-readable memory produce an article of manufacture including instruction means which implement the function specified in the flowchart flow or flows and/or block diagram block or blocks.
These computer program instructions may also be loaded onto a computer or other programmable data processing apparatus to cause a series of operational steps to be performed on the computer or other programmable apparatus to produce a computer implemented process such that the instructions which execute on the computer or other programmable apparatus provide steps for implementing the functions specified in the flowchart flow or flows and/or block diagram block or blocks.
While preferred embodiments of the present invention have been described, additional variations and modifications in those embodiments may occur to those skilled in the art once they learn of the basic inventive concepts. Therefore, it is intended that the appended claims be interpreted as including the preferred embodiment and all changes and modifications that fall within the scope of the invention.
It will be apparent to those skilled in the art that various changes and modifications may be made in the present invention without departing from the spirit and scope of the invention. Thus, if such modifications and variations of the present invention fall within the scope of the claims of the present invention and their equivalents, the present invention is also intended to include such modifications and variations.

Claims (3)

1. A hydrological model confluence method of a multi-blocking two-dimensional diffusion wave equation under reservoir group regulation is characterized by comprising the following steps:
(1) Collecting the storage capacity, longitude and latitude coordinates, vector river network files and scheduling rule data of a large reservoir in a research area, establishing grid point coordinates, and determining a scheduling rule, a regulation node and an upstream water collecting area range of the large reservoir; collecting the storage capacity and longitude and latitude coordinates of the small reservoir in the research area, establishing grid point coordinates, and determining a scheduling rule and a regulation and storage node of the small reservoir;
(2) Calculating the change of the corresponding water surface height of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity according to the scheduling rule and the regulation and storage node of the large reservoir, and constructing a two-dimensional diffusion wave equation set of the upstream grid of the reservoir;
(3) Determining the inlet flow of the reservoir according to the regulation and storage nodes of the large reservoir, and calculating the discharge flow of the reservoir by using the scheduling rule of the large reservoir, wherein the scheduling rule adopts the collected actual scheduling rule or the conceptual scheduling rule obtained by generalization, and a two-dimensional diffusion wave equation set of the downstream grid of the reservoir is constructed;
(4) Determining the inflow rate of the reservoir according to the regulation nodes of the small reservoir, calculating the regulation and storage effect of the small reservoir on the runoff by utilizing the dispatching rule of the large reservoir, and generalizing the regulation and storage effect into a source collection item of a grid where the small reservoir is located, wherein the dispatching rule adopts the collected actual dispatching rule or the conceptualized dispatching rule obtained by generalization, and a two-dimensional diffusion wave equation set of the grid where the small reservoir is located is constructed;
(5) Performing basin confluence calculation on the equation sets in the steps (2) to (4) to obtain a final confluence result;
in the step (2), the change of the corresponding water surface elevation of the upstream grid of the reservoir caused by the change of the reservoir water storage capacity is expressed as:
Figure FDA0003808908170000011
wherein O is the outlet flow of the large reservoir, I is the inlet flow of the reservoir, A w The water surface area of the upstream grid is obtained, and dt is a time step;
in the step (2), a two-dimensional diffusion wave equation set of the upstream grid of the reservoir is constructed, namely:
Figure FDA0003808908170000012
Figure FDA0003808908170000013
Figure FDA0003808908170000021
wherein H 'is the water surface elevation of the upstream grid under reservoir regulation, H' = H + delta H, u and v are the flow velocity in the x direction and the y direction respectively, H is the water surface elevation of the upstream grid under the natural condition,
Figure FDA0003808908170000022
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the time direction is obtained,
Figure FDA0003808908170000023
the partial derivative of the water surface elevation of the upstream grid under reservoir regulation in the x direction is obtained,
Figure FDA0003808908170000024
the partial derivative of the elevation of the water surface of the upstream grid under reservoir regulation in the y direction is shown, D is the water depth of the upstream grid, g is the gravity acceleration, and K is the flow modulus;
in the step (3), a two-dimensional diffusion wave equation set of the downstream grid of the reservoir is constructed and expressed as follows:
Figure FDA0003808908170000025
Figure FDA0003808908170000026
Figure FDA0003808908170000027
wherein, V x 、V y The flow velocities of the large reservoir discharge flow in the x direction and the y direction respectively, u and v are the flow velocities in the x direction and the y direction respectively, A w Is the water surface area of the downstream grid, h is the water surface elevation of the downstream grid under the natural condition,
Figure FDA0003808908170000028
the partial derivative in time of the downstream grid water surface elevation in the natural situation,
Figure FDA0003808908170000029
for the natural situation that the elevation of the water surface of the downstream grid is xThe partial derivative in the direction of the light,
Figure FDA00038089081700000210
the method is characterized in that the partial derivative of the elevation of the water surface of a downstream grid in the y direction under the natural condition is shown, D is the water depth of the downstream grid, g is the gravity acceleration, K is the flow modulus, and O is the outflow of a large reservoir.
2. The hydrological model confluence method of multi-blocking two-dimensional diffusion wave equation under reservoir group regulation according to claim 1, wherein in the step (4), the regulation and storage effect of the small reservoir on the runoff is calculated according to the regulation and storage node and the dispatching rule of the small reservoir, and is generalized to the source and sink term of the grid where the small reservoir is located, and the source and sink term is expressed as:
Figure FDA0003808908170000031
wherein S is a source exchange item caused by reservoir regulation, O ' is the outlet flow of the small reservoir, I ' is the inlet flow of the small reservoir, A ' w Is the water surface area of the small reservoir grid.
3. The hydrological model confluence method of multi-blocking two-dimensional diffusion wave equation under regulation and storage of reservoir group according to claim 1, wherein in the step (4), the construction of the two-dimensional diffusion wave equation set of the grid where the small reservoir is located comprises:
Figure FDA0003808908170000032
Figure FDA0003808908170000033
Figure FDA0003808908170000034
wherein H' is the elevation of the grid water surface under the regulation and storage of the small reservoir,
Figure FDA0003808908170000035
the partial derivative of the grid water surface elevation in the time direction under the regulation and storage of the small reservoir,
Figure FDA0003808908170000036
the partial derivative of the grid water surface elevation in the x direction under the regulation and storage of the small reservoir,
Figure FDA0003808908170000037
the partial derivative of the grid water surface elevation in the y direction under the regulation and storage of the small reservoir is obtained; d ' is the water depth of the grid where the small reservoir is located, g is the gravity acceleration, K is the flow modulus, u ' and V ' are the flow velocity in the x and y directions, V ' respectively ' x ,V' y The flow rates of the small reservoir discharge in the x direction and the y direction are respectively, and A is the area of the water passing section.
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