登录
首页 » C# » UDF2

UDF2

于 2019-11-25 发布
0 210
下载积分: 1 下载次数: 5

代码说明:

说明:  udf模拟油膜蒸发过程及其温度分布和各组分的浓度(Udf simulates oil film evaporation process and its temperature distribution and concentration of each component)

文件列表:

UDF2\common_shared.h, 169761 , 2016-07-02
UDF2\const_shared.h, 6135 , 2016-07-02
UDF2\converge_udf.dll, 363520 , 2018-08-17
UDF2\converge_udf.exp, 278440 , 2018-08-17
UDF2\converge_udf.lib, 389376 , 2018-08-17
UDF2\csi_libraries.h, 111612 , 2016-07-02
UDF2\fgm_shared.h, 4796 , 2016-07-02
UDF2\makefile, 3726 , 2016-07-02
UDF2\makefile.win, 3628 , 2016-07-02
UDF2\make_udf.bat, 4659 , 2016-07-02
UDF2\mechanism_shared.h, 5779 , 2016-07-02
UDF2\mpi_replacement_functions.h, 5413 , 2016-07-02
UDF2\parsing.h, 19694 , 2016-07-02
UDF2\prototype_shared.h, 35914 , 2016-07-02
UDF2\rif_common_shared.h, 2104 , 2016-07-02
UDF2\safe_prototypes.h, 475 , 2016-07-02
UDF2\sage_common_shared.h, 2722 , 2016-07-02
UDF2\structures_shared.h, 107604 , 2016-07-02
UDF2\sundials_subset.h, 3989 , 2016-07-02
UDF2\table.h, 5852 , 2016-07-02
UDF2\tools_shared.h, 15875 , 2016-07-02
UDF2\udf_libraries.h, 38556 , 2016-07-02
UDF2\user_available.c, 2937 , 2016-07-02
UDF2\user_bc.c, 1938 , 2016-07-02
UDF2\user_bc.obj, 233070 , 2018-08-17
UDF2\user_bound.c, 1419 , 2016-07-02
UDF2\user_bound.obj, 232563 , 2018-08-17
UDF2\user_break_custom.c, 3562 , 2016-07-02
UDF2\user_break_custom.obj, 233744 , 2018-08-17
UDF2\user_calc_grad_g_eqn.c, 2243 , 2016-07-02
UDF2\user_calc_grad_g_eqn.obj, 236171 , 2018-08-17
UDF2\user_calc_g_eqn_src.c, 33139 , 2016-07-02
UDF2\user_calc_g_eqn_src.obj, 292566 , 2018-08-17
UDF2\user_combust_ctc.c, 22713 , 2016-07-02
UDF2\user_combust_ctc.obj, 256529 , 2018-08-17
UDF2\user_combust_g_eqn.c, 6546 , 2016-07-02
UDF2\user_combust_g_eqn.obj, 240503 , 2018-08-17
UDF2\user_combust_main.c, 20007 , 2016-07-02
UDF2\user_combust_main.obj, 252878 , 2018-08-17
UDF2\user_combust_model.c, 1446 , 2016-07-02
UDF2\user_combust_model.obj, 232604 , 2018-08-17
UDF2\user_combust_multizone.c, 1362 , 2016-07-02
UDF2\user_combust_multizone.obj, 236877 , 2018-08-17
UDF2\user_combust_nox.c, 13571 , 2016-07-02
UDF2\user_combust_nox.obj, 251653 , 2018-08-17
UDF2\user_combust_rif.c, 52339 , 2016-07-02
UDF2\user_combust_rif.obj, 334333 , 2018-08-17
UDF2\user_combust_sage.c, 35016 , 2016-07-02
UDF2\user_combust_sage.obj, 295575 , 2018-08-17
UDF2\user_combust_sage_setup.c, 15638 , 2016-07-02
UDF2\user_combust_sage_setup.obj, 261061 , 2018-08-17
UDF2\user_combust_shell.c, 41590 , 2016-07-02
UDF2\user_combust_shell.obj, 273606 , 2018-08-17
UDF2\user_combust_soot.c, 11121 , 2016-07-02
UDF2\user_combust_soot.obj, 246306 , 2018-08-17
UDF2\user_drop_distort.c, 4080 , 2016-07-02
UDF2\user_drop_distort.obj, 235597 , 2018-08-17
UDF2\user_dt.c, 3148 , 2016-07-02
UDF2\user_dt.obj, 232545 , 2018-08-17
UDF2\user_dynamic_routines.c, 66179 , 2016-07-02
UDF2\user_dynamic_routines.obj, 306726 , 2018-08-17
UDF2\user_equiv_ratio.c, 2192 , 2016-07-02
UDF2\user_equiv_ratio.obj, 235292 , 2018-08-17
UDF2\user_event.c, 3474 , 2016-07-02
UDF2\user_event.obj, 234340 , 2018-08-17
UDF2\user_film.c, 5667 , 2016-07-02
UDF2\user_film.obj, 238727 , 2018-08-17
UDF2\user_film_evap.c, 35641 , 2016-07-02
UDF2\user_film_evap.obj, 283272 , 2018-08-17
UDF2\user_film_gradp.c, 2455 , 2016-07-02
UDF2\user_film_gradp.obj, 233812 , 2018-08-17
UDF2\user_film_prop.c, 2264 , 2016-07-02
UDF2\user_film_prop.obj, 233606 , 2018-08-17
UDF2\user_film_sources.c, 3986 , 2016-07-02
UDF2\user_film_sources.obj, 234896 , 2018-08-17
UDF2\user_film_splash.c, 20786 , 2016-07-02
UDF2\user_film_splash.obj, 250412 , 2018-08-17
UDF2\user_film_strip.c, 13006 , 2016-07-02
UDF2\user_film_strip.obj, 249026 , 2018-08-17
UDF2\user_flux_limiter.c, 436 , 2016-07-02
UDF2\user_flux_limiter.obj, 232730 , 2018-08-17
UDF2\user_fsi.c, 7464 , 2016-07-02
UDF2\user_fsi.obj, 248692 , 2018-08-17
UDF2\user_ga_merit_function.c, 1765 , 2016-07-02
UDF2\user_ga_merit_function.obj, 245613 , 2018-08-17
UDF2\user_header.h, 2147 , 2016-07-02
UDF2\user_heat_transfer.c, 3073 , 2016-07-02
UDF2\user_heat_transfer.obj, 233670 , 2018-08-17
UDF2\user_initialize.c, 2168 , 2016-07-02
UDF2\user_initialize.obj, 242525 , 2018-08-17
UDF2\user_initialize_g_equation.c, 12625 , 2016-07-02
UDF2\user_initialize_g_equation.obj, 247673 , 2018-08-17
UDF2\user_inject_custom.c, 5824 , 2016-07-02
UDF2\user_inject_custom.obj, 235336 , 2018-08-17
UDF2\user_inject_profile.c, 1522 , 2016-07-02
UDF2\user_inject_profile.obj, 232645 , 2018-08-17
UDF2\user_inputs.c, 8263 , 2016-07-02
UDF2\user_inputs.obj, 244134 , 2018-08-17
UDF2\user_load_balance.c, 1570 , 2016-07-02
UDF2\user_load_balance.obj, 232715 , 2018-08-17

下载说明:请别用迅雷下载,失败请重下,重下不扣分!

发表评论

0 个回复

  • GCMC
    巨正则系综蒙特卡罗算法的源程序;可以用来进行吸附等分子模拟;最大的好处在于可以插入或删除原子(Grand canonical ensemble Monte Carlo algorithm source can be used for adsorption, molecular simulation biggest advantage is that you can insert or delete atom)
    2008-06-09 14:45:03下载
    积分:1
  • SHORTPATHmatlab
    说明:  Dijkstra算法与Floyd算法的matlab实现,以求解最短路问题(Dijkstra algorithm and Floyd algorithm matlab realize in order to solve the shortest path problem)
    2008-10-02 16:05:59下载
    积分:1
  • 14-NR
    14节点牛拉算法计算潮流程序,用于电力系统的潮流计算程序,可以直接用于潮流计算,也可以用于学习潮流计算的流程和方法。(For power flow calculation program, can be used directly flow calculation can also be used to study flow calculation processes and methods.)
    2020-07-04 20:40:02下载
    积分:1
  • Learn R for Applied Statistics
    Do you need to gain confidence with handling numbers and formulae? Do you want a clear, step-by-step guide to the key concepts and principles of statistics? Nearly all aspects of our lives can be subject to statistical analysis. Statistics: An Introduction shows you how to interpret, analyze and present figures. Assuming minimal knowledge of maths and using examples from a wide variety of everyday contexts, this book makes often complex concepts and techniques easy to get to grips with. This new edition has been fully updated. Whether you want to understand the statistics that you are bombarded with every day or are a student or professional coming to statistics from a wide range of disciplines, Statistics: An Introduction covers it all.
    2020-06-22 22:20:01下载
    积分:1
  • chenggongjiao
    处理任意两点间多条公交、地铁线路的到达问题此,改程序将一二问综合在一起,方便精简,运行速度快(Treatment between any two many bus, subway lines to reach this issue, change the program integrated with the twelve asked to facilitate streamlined, fast)
    2013-08-18 09:29:13下载
    积分:1
  • 基于结构网格二维Euler方程的Jameson求解方法
    说明:  基于结构网格二维Euler方程的Jameson求解方法 自己写的程序,网格是现成的结构网格(Jameson solution method based on two-dimensional Euler equation of structural grid. Write their own procedures, the grid is ready - made structural grid.)
    2019-04-09 10:00:54下载
    积分:1
  • upward_kuobian
    空间数据扩边以后做fft并在频率域延拓,可用于求重磁异常(expansion of spatial data and FFT, in the frequency domain extension can be used to find the gravity and magnetic anomalies)
    2013-05-17 23:39:57下载
    积分:1
  • sce-ua
    vic模型参数率定代码,用Python编写(VIC Model Parameter rate code, written in Python)
    2021-03-14 11:39:23下载
    积分:1
  • Euler_DG_Quadrilateral_2D
    自己写了一个二维Euler方程的间断有限元程序 上次发了一个三角形单元的程序 因为不是曲边单元 所以在圆柱后面容易形成涡 现在把程序改为曲边四边形单元了 没有涡出现 单元是8节点四边形单元 节点编号顺序是 1 5 2 6 3 7 4 8 也就是四个角点依次 是1 2 3 4 然后是边的中点编号 5 6 7 8. 时间推进采用 Runge-Kutta 方法 数值通量采用全局Lax-Friedrichs通量 仍然不能捕捉激波 因为没有做重构或者加人工粘性 等这个做出来了 再发一次。 程序没有进行优化 比如说内存的消耗没有优化 比如直边单元的边界积分仍然采 用了曲边的积分方法 增加了计算量 比如面积分、线积分都是采用的是Gauss- Legendre-Lobatto积分 积分精度会比一般的Gauss-Legendre积分精度低一阶 等 等问题。 二维的 纯属交流性质 就没有考虑这些问题 ^_^ 如果物面全部是直边 那么只要改变一个参数N 就可以获得不同的计算精度 且具 有谱精度 因为单元的节点是Gauss-Legendre-Lobatto积分点。 其实就是谱元法 (物面是曲边的情况我不清楚是不是也可以通过提高基函数的阶数 也就是增加N 来提高计算精度)(Wrote a two-dimensional Euler equations with discontinuous finite element program Last made ​ ​ a triangular element of the program, not curved edge unit is so easy to form a vortex in the cylinder behind the Program to curved edge quadrilateral element vortices appear Unit is the order of 8-node quadrilateral element node number is 15,263,748 which is the four corners of the points in turn Is 1234 and then the side of the midpoint of the number 5678. Time promote the use of Runge-Kutta method Numerical flux of the overall situation of Lax-Friedrichs, flux Still can not capture the shock wave did not do the reconstruction or artificial viscosity do it Zaifayici. The program is not optimized for example, memory consumption is not optimized such as straight-edge boundary integral of the unit is still mining Integral method to increase the amount of computation such as surface integral with a curved edge, the line integral using the Gauss- The Legendr)
    2021-01-29 12:58:40下载
    积分:1
  • phase-field
    说明:  用相场法模拟晶粒的长大的一个程序,用c++编写的,(a program simulation the grain growth by Phase field written using c++)
    2021-03-02 11:39:34下载
    积分:1
  • 696518资源总数
  • 105885会员总数
  • 31今日下载