CN107133418A - Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms - Google Patents

Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms Download PDF

Info

Publication number
CN107133418A
CN107133418A CN201710383303.XA CN201710383303A CN107133418A CN 107133418 A CN107133418 A CN 107133418A CN 201710383303 A CN201710383303 A CN 201710383303A CN 107133418 A CN107133418 A CN 107133418A
Authority
CN
China
Prior art keywords
transport
fluids
fluids material
tvd
stratospheric
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201710383303.XA
Other languages
Chinese (zh)
Other versions
CN107133418B (en
Inventor
刘哲
林磊
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Individual
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to CN201710383303.XA priority Critical patent/CN107133418B/en
Publication of CN107133418A publication Critical patent/CN107133418A/en
Application granted granted Critical
Publication of CN107133418B publication Critical patent/CN107133418B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2119/00Details relating to the type or aim of the analysis or the optimisation
    • G06F2119/06Power analysis or power optimisation
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02ATECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
    • Y02A90/00Technologies having an indirect contribution to adaptation to climate change
    • Y02A90/10Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Computer Hardware Design (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)
  • Complex Calculations (AREA)

Abstract

The invention discloses the advection transport equation that a kind of Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms includes building Fluids material, and then numerical discretization is carried out to the advection transport equation, obtain the discrete equation of Fluids material conveying;The discrete equation that Fluids material is conveyed disassembles into the step number equal with its dimension;Obtain the flow field data of Fluids material and input and iterative numerical calculating is carried out in the discrete equation conveyed to Fluids material, predict the Fluids material concentration in each default iteration time section;During iterative numerical is calculated, different types of total variance abatement restricted function is used alternatingly according to the step number equal with its dimension in each dimension respectively in different default iteration time sections to calculate Fluids material concentration in next period, the change of Fluids material stratospheric transport process medium fluid material concentration is finally simulated and predict.

Description

Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms
Technical field
Calculated the invention belongs to fluid dynamic numerical simulation and calculating field, more particularly to a kind of alternately TVD difference that is based on The Fluids material stratospheric transport analogy method of method.
Background technology
Numerical model is research and the important work for forecasting the motion such as river, ocean and its interior transport of substances in nature Tool, with the development of computer technology and social economy, numerical model is in scientific research, operational forecast and Hu Ku, ocean etc. The effect become more and more important is played in the industry such as environmental management and planning.
Advection is that the main process that material carries out space conveying is carried in Fluids, and advection process is represented by equation (1).It is generally using the method for difference that the progress of (1) formula is discrete in numerical model, obtain such as the advection difference side of formula (2) form Journey, then carries out iterative numerical to formula (2), obtains material concentration c spatial distribution and change over time.
Wherein, c transports material concentration for certain, and u, v, w are respectively the flow velocity in x, y, z direction.
Wherein,For the material concentration at half storey grid, Δ t is discrete Time step, Δ x, Δ y, Δ z are respectively the grid spacing in x, y, z direction, and label subscript n represents time step number, subscript i, J, k represent the grid label in x, y, z direction respectively.
In difference equation (2), the material concentration at half storey grid how is calculatedIt is the main difference of different difference schemes Where not.For example, upstreame scheme uses upstream grid concentration, middle poor form uses being averaged for upstream and downstream grid Concentration.Although these algorithms calculate easy, the problem of there is low precision or strong numerical solidification, cause analog result distortion compared with It is strong and the stability of model can be influenceed.
Total variance abatement (Total Variation Diminishing, abbreviation TVD) difference scheme is the high-precision nothing of a class The advection difference algorithm of frequency dispersion, it is widely used in ocean and Atmospheric Numerical Model and correlative study.TVD algorithms are mainly The high-precision item of back-diffusion is added on the basis of original low precision upstreame scheme, the precision of advection form is improved, draws simultaneously Enter restricted function to control the intensity of high-precision item added, with this, keep in whole integral process forward, numeric format it is total It is deteriorated and keeps not increasing, so as to effectively suppresses the numerical solidification that high accurate scheme generally has.
The algorithm of TVD advection forms is following (by taking x directions as an example):
As shown in formula (3), calculatingWhen, plus high-precision correction term on the basis of upstreame scheme, and before correction term Add restricted function ψ (ri+1/2), thus obtain:
Wherein,
Add after restricted function and ensure the total variance of result of calculationHolding does not increase, i.e.,:
TV(cn+1)≤TV(cn) (4)
Restricted function need to be caused to meet following conditions:
Wherein, r represents concentration gradient ratio, i.e.,Or
Although TVD restricted functions have a variety of, a kind of restricted function of single use can not be controlled in TVD forms well The intensity of the high-precision item of addition, thereby resulted in above TVD numeric formats still have certain numerical d ispersion (e.g., Minmod, Van Leer, MUSCL, HSIMT) and the pseudo- effect of back-diffusion (e.g., Superbee).In addition, TVD forms can ensure one-dimensional before In the case of total variance do not increase, it is and then barely satisfactory in the case of multidimensional, however it remains numerical solidification.Therefore, existing TVD is utilized When advection difference scheme to the transport of substances in Fluids simulate for a long time, unsatisfactory simulation knot is still suffered from Really.
The content of the invention
In order to solve the deficiencies in the prior art, the invention provides a kind of Fluids based on alternately TVD difference algorithms Material stratospheric transport analogy method, it provides a kind of effectively decrease numerical d ispersion and the pseudo- effect of back-diffusion and solves multidimensional frequency dispersion and puts down Difference method-the TVDal (TVD with Alternating Limiters) of stream format, it is right in Fluids to be applied to The simulation and forecast of transport of substances.
A kind of Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms of the present invention, including:
The advection transport equation of Fluids material is built, and then numerical discretization is carried out to the advection transport equation, is obtained The discrete equation conveyed to Fluids material;The dimension of the discrete equation of the Fluids material conveying is at least two dimension;
The discrete equation that Fluids material is conveyed disassembles into the step number equal with its dimension;
Obtain the flow field data of Fluids material and input in the discrete equation conveyed to Fluids material and enter line number Value iterative calculation, predicts the Fluids material concentration in each default iteration time section;
During iterative numerical is calculated, in different default iteration time sections respectively in each dimension according to The equal step number of its dimension is used alternatingly different types of total variance abatement restricted function to calculate the earth in next period Flowing material concentration, finally simulates and predicts the change of Fluids material stratospheric transport process medium fluid material concentration.
Further, the building method based on the abatement form that is deteriorated, the advection transport equation to earth flowing material is carried out Numerical discretization.
Further, total variance abatement restricted function includes the restricted function and numerical value back-diffusion property of numerical d ispersion property Restricted function.
Further, Fluids material concentration is the function on time and space.
Further, the process for asking for the advection transport equation of Fluids material is:
Fluids material concentration is respectively to the derived function for the directioin parameter for characterizing space, then the side with corresponding sign space After being multiplied to the flow velocity of parameter, the Fluids material concentration that finally adds up obtains Fluids material to the derived function of time Advection transport equation.
Wherein, the restricted function of the numerical d ispersion property is Minmod functions.
The restricted function of the numerical d ispersion property is Van Leer functions.
The restricted function of the numerical d ispersion property is MUSCL functions.
The restricted function of the numerical d ispersion property is HSIMT functions.
The restricted function of the numerical value back-diffusion property includes Superbee functions.
Wherein, actually calculate in, frequently with several classical TVD restricted functions mainly have:
Superbee:
ψ(r)Superbee=max [0, min (2r, 1), min (r, 2)] (6)
Van Leer(or Harmonic):
ψ(r)VanLeer=(r+ | r |)/(r+1) (7)
MUSCL:
Minmod:
ψ(r)Minmod=max [0, min (r, 1)] (9)
HSIMT:
ψ(r)HSIMT=max [0, min (2r, 2, β)] (10)
Wherein,
Compared with prior art, the beneficial effects of the invention are as follows:
(1) this method does not change original formula increase extra computation amount, but is used alternatingly not in different time step Connatural algorithm, largely reduces the numerical d ispersion and the pseudo- effect of back-diffusion of traditional TVD advections difference algorithm so that The error of analog result is smaller.
(2) alternately restricted function is split with discrete equation in this method and be combined, it is flat without frequency dispersion based on obtained multidimensional Flow algorithm, effectively eliminates the TVD advection forms numerical solidification problem that transport of substances is simulated in the case of Multi-dimension calculation.
Brief description of the drawings
The Figure of description for constituting the part of the application is used for providing further understanding of the present application, and the application's shows Meaning property embodiment and its illustrate be used for explain the application, do not constitute the improper restriction to the application.
Fig. 1 is the schematic flow sheet of the present invention;
Fig. 2 (a) is initial time material concentration distribution map;
Fig. 2 (b) is the Superbee analog results based on traditional TVD algorithms;
Fig. 2 (c) is the HSIMT analog results based on traditional TVD algorithms;
Fig. 2 (d) is the Superbee analog results that traditional TVD algorithms combination discrete equation splits algorithm;
Fig. 2 (e) is the HSIMT analog results that traditional TVD algorithms combination discrete equation splits algorithm;
Fig. 2 (f) is the analog result of the inventive method.
Embodiment
It is noted that described further below is all exemplary, it is intended to provide further instruction to the application.Unless another Indicate, all technologies used herein and scientific terminology are with usual with the application person of an ordinary skill in the technical field The identical meanings of understanding.
It should be noted that term used herein above is merely to describe embodiment, and be not intended to restricted root According to the illustrative embodiments of the application.As used herein, unless the context clearly indicates otherwise, otherwise singulative It is also intended to include plural form, additionally, it should be understood that, when in this manual using term "comprising" and/or " bag Include " when, it indicates existing characteristics, step, operation, device, component and/or combinations thereof.
The dimension of discrete equation of Fluids material conveying is at least two dimension, below with Fluids material convey from Exemplified by dissipating the dimension of equation and being two dimension:
As shown in figure 1, the Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms of the present invention, Including:
Step 1:Build Fluids material advection transport equation, and then to the advection transport equation carry out numerical value from Dissipate, obtain the discrete equation of Fluids material conveying.
The advection transport equation for building Fluids material is formula (1):
Numerical discretization is carried out to the advection transport equation, the discrete equation for obtaining the conveying of Fluids material is formula (2):
Wherein,For the material concentration at half storey grid, Δ t is discrete time step, Δ x, Δ y are respectively the grid spacing in x, y direction, and label subscript n represents time step number, and subscript i, j represents x, y direction respectively Grid label.
Step 2:The discrete equation that Fluids material is conveyed disassembles into the step number equal with its dimension.
Step 3:Obtain the flow field data of Fluids material and input in the discrete equation conveyed to Fluids material Iterative numerical calculating is carried out, the Fluids material concentration in each default iteration time section is predicted;
During iterative numerical is calculated, in different default iteration time sections respectively in each dimension according to The equal step number of its dimension is used alternatingly different types of total variance abatement restricted function to calculate the earth in next period Flowing material concentration, finally simulates and predicts the change of Fluids material stratospheric transport process medium fluid material concentration.
Specifically, flow velocity u, v information is inputted, the parity of iterative steps is iterated and judged to discrete equation, if Odd number is calculated then to be calculated using below step a), if even number is then calculated using step b).
Step a):
Discrete equation formula (2) is disassembled as formula (3-1) and the calculating of the step of formula (3-2) two:
Wherein,Subscript com and dif represent respectively using numerical value back-diffusion property (for example, Superbee) and numerical value expansion The TVD restricted functions of property (for example, Minmod) are dissipated to calculate material concentration at half storey grid
Discrete equation is disassembled into (3-1) and (3-2) two step, advection process in x and y both directions is calculated successively:First When step calculates advection process on x directions, first using a kind of TVD restricted functions of numerical value back-diffusion property, calculating obtains middle change Measure c*;Intermediate variable c* is substituted into y directions difference equation by second step, is calculated advection process on y directions, is used a kind of numerical d ispersion The TVD restricted functions of property calculate the concentration c for obtaining new time stepn+1
Step b):
Equally it is divided to (4-1) and (4-2) two step to calculate, but the first step first calculates y directions advection process, it is anti-using a kind of numerical value The TVD restricted functions of scattering nature, calculating obtains intermediate variable c*;Intermediate variable c* is substituted into x directions difference equation by second step, X equation advection processes are calculated, using a kind of TVD restricted functions of numerical d ispersion property, the material that calculating obtains new time step is dense Degree.
Wherein,Subscript com and dif represent respectively using numerical value back-diffusion property (for example, Superbee) and numerical value expansion The TVD restricted functions of property (for example, Minmod) are dissipated to calculate material concentration at half storey grid
Finally judge to integrate the setting value whether duration reaches pattern, no then return to step 2 continues, terminated if reaching Calculate.
Present disclosure can be further illustrated by following analog result.
1st, simulated experiment:Using the inventive method and other method, the material advection process to giving a certain concentration distribution Simulated.
2nd, analog result
Exist in a horizontal two-dimension marine site, in it with 12 hours for reciprocal flowing of the cycle along 45 ° of directions, initial time Material concentration distribution is given to be distributed as shown in Fig. 2 (a), and knot is simulated after 100 cycles obtained using different advection difference algorithms Fruit is respectively as shown in Fig. 2 (b)-Fig. 2 (f).Wherein, Fig. 2 (b) and 2 (c) are based on traditional TVD algorithms Superbee and HSIMT Analog result, Fig. 2 (d) and Superbee and the HSIMT simulation that Fig. 2 (e) is that tradition TVD algorithm combinations discrete equation splits algorithm As a result;Fig. 2 (f) is the analog result of the inventive method.
From Fig. 2 (a)-Fig. 2 (f) as can be seen that the analog result based on traditional TVD algorithms has obvious numerical value frequency Dissipate, splitting numerical solidification after algorithm using discrete equation is improved, but still suffers from the pseudo- effect of numerical value back-diffusion and diffusion, is made Then maintain the distribution of true solution substantially with the inventive method, reduce the pseudo- effect of numerical value back-diffusion and diffusion of traditional TVD algorithms, Result of calculation achieves gratifying analog result without numerical solidification simultaneously.
To sum up, this method proposed by the present invention effectively weakens numerical d ispersion and the pseudo- effect of back-diffusion and solves multidimensional frequency dispersion Difference algorithm-the TVDal of advection form material advection analogy method.The method of the present invention is conversely pseudo- by the way that property is used alternatingly Traditional TVD restricted functions of effect, effectively reduce numerical d ispersion and back-diffusion, reduce the error of advection analog result, Meanwhile, Multidimensional Discrete equation is subjected to fractionation calculating, it is ensured that multidimensional advective simulation is that no numerical solidification is produced, and the above is improved logical The analog result for crossing the experiment of material advection can be seen that.
Although above-mentioned the embodiment of the present invention is described with reference to accompanying drawing, not to present invention protection model The limitation enclosed, one of ordinary skill in the art should be understood that on the basis of technical scheme those skilled in the art are not Need to pay various modifications or deform still within protection scope of the present invention that creative work can make.

Claims (10)

1. a kind of Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms, it is characterised in that including:
The advection transport equation of Fluids material is built, and then numerical discretization is carried out to the advection transport equation, obtains ground The discrete equation of ball flowing material conveying;The dimension of the discrete equation of the Fluids material conveying is at least two dimension;
The discrete equation that Fluids material is conveyed disassembles into the step number equal with its dimension;
Obtain the flow field data of Fluids material and input progress numerical value in the discrete equation conveyed to Fluids material and change In generation, calculates, and predicts the Fluids material concentration in each default iteration time section;
During iterative numerical is calculated, tieed up respectively in each dimension according to it in different default iteration time sections The equal step number of number is used alternatingly different types of total variance abatement restricted function to calculate Fluids in next period Material concentration, finally simulates and predicts the change of Fluids material stratospheric transport process medium fluid material concentration.
2. the Fluids material stratospheric transport analogy method as claimed in claim 1 based on alternately TVD difference algorithms, it is special Levy and be, based on the building method for the abatement form that is deteriorated, the advection transport equation to earth flowing material carries out numerical discretization.
3. the Fluids material stratospheric transport analogy method as claimed in claim 1 based on alternately TVD difference algorithms, it is special Levy and be, total variance abatement restricted function includes the restricted function of numerical d ispersion property and the limitation letter of numerical value back-diffusion property Number.
4. the Fluids material stratospheric transport analogy method as claimed in claim 1 based on alternately TVD difference algorithms, it is special Levy and be, Fluids material concentration is the function on time and space.
5. the Fluids material stratospheric transport analogy method as claimed in claim 4 based on alternately TVD difference algorithms, it is special Levy and be, the process for asking for the advection transport equation of Fluids material is:
Fluids material concentration is joined respectively to the derived function for the directioin parameter for characterizing space, then with the corresponding direction for characterizing space After several flow velocitys is multiplied, the Fluids material concentration that finally adds up obtains the advection of Fluids material to the derived function of time Transport equation.
6. the Fluids material stratospheric transport analogy method as claimed in claim 3 based on alternately TVD difference algorithms, it is special Levy and be, the restricted function of the numerical d ispersion property is for Minmod functions or from his scattering nature restricted function.
7. the Fluids material stratospheric transport analogy method as claimed in claim 3 based on alternately TVD difference algorithms, it is special Levy and be, the restricted function of the numerical d ispersion property is for Van Leer functions or from his scattering nature restricted function.
8. the Fluids material stratospheric transport analogy method as claimed in claim 3 based on alternately TVD difference algorithms, it is special Levy and be, the restricted function of the numerical d ispersion property is for MUSCL functions or from his scattering nature restricted function.
9. the Fluids material stratospheric transport analogy method as claimed in claim 3 based on alternately TVD difference algorithms, it is special Levy and be, the restricted function of the numerical d ispersion property is for HSIMT functions or from his scattering nature restricted function.
10. the Fluids material stratospheric transport analogy method as claimed in claim 3 based on alternately TVD difference algorithms, its It is characterised by, the restricted function of the numerical value back-diffusion property includes Superbee functions or limits letter from his back-diffusion property Number.
CN201710383303.XA 2017-05-26 2017-05-26 Earth fluid material advection transportation simulation method based on alternative TVD differential algorithm Expired - Fee Related CN107133418B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710383303.XA CN107133418B (en) 2017-05-26 2017-05-26 Earth fluid material advection transportation simulation method based on alternative TVD differential algorithm

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710383303.XA CN107133418B (en) 2017-05-26 2017-05-26 Earth fluid material advection transportation simulation method based on alternative TVD differential algorithm

Publications (2)

Publication Number Publication Date
CN107133418A true CN107133418A (en) 2017-09-05
CN107133418B CN107133418B (en) 2020-04-21

Family

ID=59733351

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710383303.XA Expired - Fee Related CN107133418B (en) 2017-05-26 2017-05-26 Earth fluid material advection transportation simulation method based on alternative TVD differential algorithm

Country Status (1)

Country Link
CN (1) CN107133418B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114840974A (en) * 2022-03-25 2022-08-02 中国气象局地球***数值预报中心 Advection mode system suitable for complex terrain and operation method thereof

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101484922A (en) * 2006-04-05 2009-07-15 财团法人Seoul大学校产学协力财团 Method of simulating detailed movements of fluids using derivative particles
CN101615219A (en) * 2009-08-04 2009-12-30 北京师范大学 A kind of high-precision difference method of simulating transport diffusion problem
CN102830121A (en) * 2012-08-17 2012-12-19 浙江工业大学 Real-time detection method of soft abrasive flow abrasive group
CN104239625A (en) * 2014-09-05 2014-12-24 中国矿业大学 Corrective fluid motion equation linear iteration-based steady state solution method
CN104636566A (en) * 2015-03-13 2015-05-20 中国矿业大学 Dynamic mesh numerical solution method based on modified fluid motion equation
CN104732093A (en) * 2015-03-30 2015-06-24 西安交通大学 FCT-FDM forward simulation method based on dispersion viscosity wave equation
US9430870B2 (en) * 2003-02-19 2016-08-30 California Institute Of Technology Level set surface editing operators
CN106294282A (en) * 2016-08-01 2017-01-04 中国石油天然气股份有限公司 Black oil reservoir simulation method and device

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9430870B2 (en) * 2003-02-19 2016-08-30 California Institute Of Technology Level set surface editing operators
CN101484922A (en) * 2006-04-05 2009-07-15 财团法人Seoul大学校产学协力财团 Method of simulating detailed movements of fluids using derivative particles
CN101615219A (en) * 2009-08-04 2009-12-30 北京师范大学 A kind of high-precision difference method of simulating transport diffusion problem
CN102830121A (en) * 2012-08-17 2012-12-19 浙江工业大学 Real-time detection method of soft abrasive flow abrasive group
CN104239625A (en) * 2014-09-05 2014-12-24 中国矿业大学 Corrective fluid motion equation linear iteration-based steady state solution method
CN104636566A (en) * 2015-03-13 2015-05-20 中国矿业大学 Dynamic mesh numerical solution method based on modified fluid motion equation
CN104732093A (en) * 2015-03-30 2015-06-24 西安交通大学 FCT-FDM forward simulation method based on dispersion viscosity wave equation
CN106294282A (en) * 2016-08-01 2017-01-04 中国石油天然气股份有限公司 Black oil reservoir simulation method and device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114840974A (en) * 2022-03-25 2022-08-02 中国气象局地球***数值预报中心 Advection mode system suitable for complex terrain and operation method thereof
CN114840974B (en) * 2022-03-25 2022-11-25 中国气象局地球***数值预报中心 Advection mode system suitable for complex terrain and operation method thereof

Also Published As

Publication number Publication date
CN107133418B (en) 2020-04-21

Similar Documents

Publication Publication Date Title
CN104268943B (en) Fluid simulation method based on Eulerian-Lagrangian coupling method
Wang A Quadtree-based adaptive Cartesian/Quad grid flow solver for Navier-Stokes equations
Morgenthal et al. An immersed interface method for the Vortex-In-Cell algorithm
Hartmann et al. Discontinuous Galerkin methods for computational aerodynamics—3D adaptive flow simulation with the DLR PADGE code
CN113850008B (en) Self-adaptive grid disturbance domain updating acceleration method for aircraft aerodynamic characteristic prediction
CN111859529B (en) Multi-grid disturbance domain updating acceleration method for aircraft streaming numerical simulation
CN113609598B (en) RANS/LES disturbance domain updating method for aircraft aerodynamic characteristic simulation
CN107657075B (en) The Region Decomposition FInite Element of Darcy velocity at simulated groundwater dielectric interface
Bermejo et al. A conservative quasi-monotone semi-Lagrangian scheme
Giles et al. Progress in adjoint error correction for integral functionals
Suchde et al. Point cloud movement for fully Lagrangian meshfree methods
Thömmes et al. A lattice Boltzmann method for immiscible multiphase flow simulations using the level set method
Miller et al. Surface heterogeneity effects on regional-scale fluxes in the stable boundary layer: Aerodynamic roughness length transitions
Moukalled et al. Performance comparison of the NWF and DC methods for implementing high-resolution schemes in a fully coupled incompressible flow solver
CN107133418A (en) Fluids material stratospheric transport analogy method based on alternately TVD difference algorithms
Okusanya et al. Algebraic multigrid for stabilized finite element discretizations of the Navier–Stokes equations
Liu et al. An unconditionally stable spline difference scheme of O (k2+ h4) for solving the second-order 1D linear hyperbolic equation
Parent Positivity-preserving flux difference splitting schemes
Sonar Classical finite volume methods
Jiang et al. A new turbulence model for separated flows
Shanbi et al. The simulation of natural gas gathering pipeline network
CN108072899B (en) Self-adaptive implementation method of discontinuous Galerkin finite element seismic numerical simulation algorithm
Hong et al. A sharp interface immersed edge-based smoothed finite element method with extended fictitious domain scheme
Shi et al. An adaptive semi-lagrangian level-set method for convection-diffusion equations on evolving interfaces
Gillow et al. Computation of currents at microelectrodes using hp-DGFEM

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20200421