* Results

*Conclusion*
- little effect of rear rotor on Cp_1
- Cp1 is independent of TI
** TI effect on single-rotor, front,
| cp | ct | TI | TSR |
|    |    | 1  |     |
|    |    | 15 |     |
** Dual rotor X=4D, TI 15% -- CFD-RANS
# TI 15%, RANS results
# TSR1 TSR2/TSR1 TSR2      Cp_1      Ct_1     Cp_2    Ct_2
  5.0   0.730    3.65   0.396   0.824  -0.024  0.289
  5.0   0.600    3.00   0.397   0.829   0.010  0.284  
  5.0   0.500    2.50   0.395   0.826   0.005   0.265

TSR1 TSR2/TSR1    TSR2    Cp_1    Ct_1    Cp_2    Ct_2
5    0.733    3.665    0.394    0.82    -0.044    0.229
5    0.644    3.22    0.393    0.82    -0.02    0.218
5    0.55    2.75    0.394    0.819    -0.005    0.21
5    0.5    2.5    0.395    0.82    0.002    0.184
5    0.45    2.25    0.396    0.821    0.000    0.168
5    0.4    2    0.396    0.821    -0.004    0.153
5    0.35    1.75    0.395    0.821    -0.006    0.143
5    0.2    1    0.396    0.822    -0.004    0.09

** Dual X=4D same TSR -- BEM + Park model
 # ak, distance (norm by D)=   3.99999991E-02   4.00000000    
 # TSR1, C_T_tot, C_P_tot, omega2/omega1
   1.000000E+00   2.862664E-01   2.394140E-02   9.567473E-01
   1.250000E+00   3.237689E-01   4.581533E-02   9.503006E-01
   1.500000E+00   3.736952E-01   7.827624E-02   9.411572E-01
   1.750000E+00   4.390565E-01   1.231780E-01   9.281210E-01
   2.000000E+00   5.195406E-01   1.788598E-01   9.113323E-01
   2.250000E+00   6.136195E-01   2.441946E-01   8.893722E-01
   2.500000E+00   7.156332E-01   3.136399E-01   8.634881E-01
   2.750000E+00   8.213180E-01   3.814463E-01   8.335000E-01
   3.000000E+00   9.222423E-01   4.392351E-01   8.015752E-01
   3.250000E+00   1.001631E+00   4.755293E-01   7.784010E-01
   3.500000E+00   1.065189E+00   4.984458E-01   7.609080E-01
   3.750000E+00   1.116553E+00   5.122202E-01   7.491560E-01
   4.000000E+00   1.160889E+00   5.199742E-01   7.404510E-01
   4.250000E+00   1.196960E+00   5.233117E-01   7.338645E-01
   4.500000E+00   1.229946E+00   5.234426E-01   7.281728E-01
   4.750000E+00   1.261175E+00   5.211463E-01   7.232024E-01
   5.000000E+00   1.291180E+00   5.169932E-01   7.189118E-01
   5.250000E+00   1.313614E+00   5.118050E-01   7.153068E-01
   5.500000E+00   1.339595E+00   5.045193E-01   7.123726E-01
   5.750000E+00   1.359179E+00   4.970232E-01   7.101494E-01
   6.000000E+00   1.381723E+00   4.874390E-01   7.084185E-01
   6.250000E+00   1.399795E+00   4.772219E-01   7.073638E-01

** DONE Cp one Rear Rotor at Re 1e6 - R=0.6
*Flow Features:*
keywords:

largely stalled)
High Angle of Attack, naca0012, stall,
Goal: performance when naca0012 is stalled

C:\Users\kaiming\Documents\ZJU\naca0012_Dual_Rotor\OneRotor_Rear_1M\tsr4

| TSR | Cp      | Ct |  Re | U(m/s) | omega(rad/s) | turbulence models |
|   4 | -0.011  |    | 1e6 |    4.4 |        77.22 |   standard k-e    |
|   4 | 0.05    |    | 1e6 |    4.4 |        77.22 |   sst ko          |
| 4.5 | - 0.013 |    | 1e6 |    4.4 |        86.87 |                   |
OneRotor_Rear_1M/rear_st_tsr4_ke_7k.dat.gz
** Wake
*** TKE
refernces:
N Stergiannis CFD modelling approaches against single wind turbine wake measurements using RANS
*** velocity contour in the wake
fig.9 mycek
** wake width measurement in CFD?
iso-surface plot, set variable as: U_x

** Mean axial velocity from CFD  at a given X/D?
- wake is normal distribution, gaussian
? how to get the mean of normal distribution?

- arear averaged axial mean veolocity of wake (Mycek 2014)
  +  (rotor radius,R)

reference:
#+CAPTION:area-averaged velocity (disc diameter=1D) (fig.8b mycek 2014 dual rotor)
file:figures/post/disc_averaged_axial_velocity_mycek_2014.png

Area used in my case:
 circular, r=1.2R (radius of turbine)

How to define the edge of of wake in CFD post processing  at different X/D?
how to define the edge of wake?
U_x = 0.99U_\infty
how to define the "mean" U_x in the wake?
? is r=1R used by mycek right?

*** One Rotor Front, Eldad Blade TSR 5 TI = 1%
# One Rotor, front, eldad blade
# TSR 5, TI =1%, \theta_T = 2 deg
#X/D    X   half width,    Ux    U    Ux/U
1    0.46    0.288    0.332    0.6    0.553333333
2    0.92    0.299    0.326    0.6    0.543333333
3    1.38    0.305    0.337    0.6    0.561666667
4    1.84    0.311    0.354    0.6    0.59
5    2.3    0.318    0.374    0.6    0.623333333
6    2.76    0.326    0.394    0.6    0.656666667
7    3.22    0.332    0.409    0.6    0.681666667
8    3.68    0.341    0.437    0.6    0.728333333
9    4.14    0.35    0.457    0.6    0.761666667
10    4.59    0.352    0.464    0.6    0.773333333
*** How to the area average velocity of wake at a given X/D?

1. cacluation wake width (b) at a given X/D
create a iso-surface plot with U_o,
2. get area average in CFDpost
  + create an expression in CFD post
~areaAve(Velocity in Stn Frame w)@areaAverage~
3. change X=2D...
*** *Turbulence kinetic energy*
3e-5, 1e-2
Number of contours, 51

Velocity
0.02-0.6
Number of contours, 31

** 3D streamline
what does 3D streamline means

** k correction
calibration

| TI (%) |      k | RMS Error |
|     15 | 0.0190 |    0.0190 |
|    1   |    0.0075 |     0.0371 |

*** Bayesian Calibration
- based on exprimental data: overall power

(Rathmann 2017)
variables: hub-height wind speed, wind direction
math function: probability density function
reommmended k value: 0.06 offshore and 0.09 onshore

- Rathmann, Ole Steen, et al. "Validation of the Revised WAsP Park Model." WindEurope 2017. 2017.
-  Rathmann O., Estimation of the Wake Expansion Coefficient from Eddy Diffusivity Theory. Research note, DTU Wind Energy. (2017).
-  M.C. Kennedy, A. O’Hagan. Bayesian calibration of computer models. Journal of the Royal
Statistical Society: Series B (Statistical Methodology), 63(3), 425-464. (2001).
- Murcia, J.P. et al., Uncertainty quantification in wind farm flow models. PhD thesis, DTU Wind
Energy (2017).
- Murcia, J.P. et al., Wake Model Calibration Based On SCADA Data Considering Uncertainty In The
Inflow Conditions. Private communication (2017).
***  k vs TI

k= 0.4 TI [fn:goccmen2016wind]
k=0.04 when TI=10%
k=0.4 TI_h
- TI_h : hub height TI
k=0.4TI = 0.038 at the Sexbierum wind fams [fn:pena2016application]
[fn:pena2016application] Peña, Alfredo, Pierre‐Elouan Réthoré, and M. Paul van der Laan. "On the application of the Jensen wake model using a turbulence‐dependent wake decay coefficient: the Sexbierum case." Wind Energy 19.4 (2016): 763-776.
[fn:goccmen2016wind] Göçmen, Tuhfe, et al. "Wind turbine wake models developed at the technical university of Denmark: A review." Renewable and Sustainable Energy Reviews 60 (2016): 752-769.

*** Pyakurel's method
- based on CFD data: centre line axial mean velocity
- Eq (10) in Pyakurel 2017
- *observed* axial velocity, U_s = *centre line* velocity from CFD RANS (this value is used as experimental data)
- Predicted axial velocity, U_c = Jensen model in which Ct is also from CFD RANS
Root mean square error = (U_s - U_c )_rms
 # limit
centre line veolocity is lower than the area averaged velocity, thus low centre line velocity as baseline, k is not accurate

** Jump value of moment time history of dual rotor

Data of Ch5 --Dual rotor的更多相关文章

  1. Feedback on Ch5 paper based on CFD-RANS

    It is encouraging that you took the initiative to write this journal manuscript, but it needs a lot ...

  2. viva correction statements

    * List of amendments| No. | Location     | Amendments                                                ...

  3. ARM与x86之3--蝶变ARM

    http://blog.sina.com.cn/s/blog_6472c4cc0100lqr8.html 蝶变ARM 1929年开始的经济大萧条,改变了世界格局.前苏联的风景独好,使得相当多的人选择了 ...

  4. UDF简记

    摘要: 1.开发UDF 2.开发UDAF 3.开发UDTF 4.部署与测试 5.一个简单的实例 内容:1.开发UDF 函数类需要继承org.apache.hadoop.hive.ql.UDF 实现ev ...

  5. Oracle no TOP, how to get top from order

    On ROWNUM and Limiting Results Our technologist explains how ROWNUM works and how to make it work fo ...

  6. On ROWNUM and Limiting Results

    This issue's Ask Tom column is a little different from the typical column. I receive many questions ...

  7. 快速搭建springmvc+spring data jpa工程

    一.前言 这里简单讲述一下如何快速使用springmvc和spring data jpa搭建后台开发工程,并提供了一个简单的demo作为参考. 二.创建maven工程 http://www.cnblo ...

  8. Mesh Data Structure in OpenCascade

    Mesh Data Structure in OpenCascade eryar@163.com 摘要Abstract:本文对网格数据结构作简要介绍,并结合使用OpenCascade中的数据结构,将网 ...

  9. 三维等值面提取算法(Dual Contouring)

    上一篇介绍了Marching Cubes算法,Marching Cubes算法是三维重建算法中的经典算法,算法主要思想是检测与等值面相交的体素单元并计算交点的坐标,然后对不同的相交情况利用查找表在体素 ...

随机推荐

  1. 第四篇(那些JAVA程序BUG中的常见单词)

    xxx cannot be resolved to a variable xxx无法解析为变量 resolve 解析

  2. [转]POJ WA/RE指南

    "POJ上头的题都是数学题",也不知道是那个家伙胡诌的--但是POJ的要求就是算法通过了也不让你AC.下面本人就这560题的经验,浅谈一下WA/RE了怎么办.  以下内容是扯淡-- ...

  3. [USACO 2011 Nov Gold] Cow Steeplechase【二分图】

    传送门:http://www.usaco.org/index.php?page=viewproblem2&cpid=93 很容易发现,这是一个二分图的模型.竖直线是X集,水平线是Y集,若某条竖 ...

  4. Coins HDU - 2844 POJ - 1742

    Coins HDU - 2844 POJ - 1742 多重背包可行性 当做一般多重背包,二进制优化 #include<cstdio> #include<cstring> in ...

  5. ReactJS-1-基本使用

    JSX使用 一.为什么使用JSX?React的核心机制之一就是虚拟DOM:可以在内存中创建的虚拟DOM元素.但是用js创建虚拟dom可读性差,于是创建了JSX,继续使用HTML代码创建dom,增加可读 ...

  6. Echarts生成饼状图、条形图以及线形图 JS封装

    1.在我们开发程序中,经常会用到生成一些报表,比方说饼状图,条形图,折线图等.不多说了,直接上封装好的代码,如下Echarts.js所示 以下代码是封装在Echarts.js文件中 /** * Cre ...

  7. java.lang.String 字符串操作

    1.获取文件名 //获取文件名,即就是去掉文件的后缀 /** * mypic.jpg * 获取文件名 * 1. 先找到"."的位置 * 2. 从第一个字符开始截取到".& ...

  8. json三层解析(数组解析)

    里面多了数组,所以用到了JOSNArray package com.xykj.weather; import java.io.BufferedReader; import java.io.IOExce ...

  9. 【数据分析 R语言实战】学习笔记 第四章 数据的图形描述

    4.1 R绘图概述 以下两个函数,可以分别展示二维,三维图形的示例: >demo(graphics) >demo(persp) R提供了多种绘图相关的命令,可分成三类: 高级绘图命令:在图 ...

  10. 键盘工具栏的快速集成--IQKeyboardManager

    转自:http://www.cnblogs.com/gaoxiaoniu/p/5333187.html 键盘工具栏的快速集成--IQKeyboardManager IQKeyboardManager, ...