基于牛顿拉夫逊法潮流计算的matlab实验报告(2)

2019-01-03 17:13

LN10 LN11 LN12 LN13 LN14 LN15 LN16 LN17 LN18 LN19 LN20 LN21 LN22 LN23 LN24 LN25 LN26 LN27 LN28 LN29 LN30 LN31 LN32 LN33 LN34 BUS-8 BUS-7 BUS-11 BUS-8 BUS-9 BUS-39 BUS-11 BUS-13 BUS-14 BUS-15 BUS-16 BUS-17 BUS-19 BUS-21 BUS-24 BUS-18 BUS-27 BUS-22 BUS-23 BUS-24 BUS-26 BUS-27 BUS-28 BUS-29 BUS-29 BUS-5 BUS-6 BUS-6 BUS-7 BUS-8 BUS-9 BUS-10 BUS-10 BUS-13 BUS-14 BUS-15 BUS-16 BUS-16 BUS-16 BUS-16 BUS-17 BUS-17 BUS-21 BUS-22 BUS-23 BUS-25 BUS-26 BUS-26 BUS-26 BUS-28 0.00080 0.00060 0.00070 0.00040 0.00230 0.00100 0.00040 0.00040 0.00090 0.00180 0.00090 0.00070 0.00160 0.00080 0.00030 0.00070 0.00130 0.00080 0.00060 0.00220 0.00320 0.00140 0.00430 0.00570 0.00140 0.01120 0.00920 0.00820 0.00460 0.03630 0.02500 0.00430 0.00430 0.01010 0.02170 0.00940 0.00890 0.01950 0.01350 0.00590 0.00820 0.01730 0.01400 0.00960 0.03500 0.03230 0.01470 0.04740 0.06250 0.01510 0.07380 0.05650 0.06945 0.03900 0.19020 0.60000 0.03645 0.03645 0.08615 0.18300 0.08550 0.06710 0.15200 0.12740 0.03400 0.06595 0.16080 0.12825 0.09230 0.18050 0.25650 0.11980 0.39010 0.51450 0.12450

LN35: BUS-4接有并联电容器,B4=1.0000 LN36: BUS-5接有并联电容器,B4=2.0000

5)变压器参数见表D-4

表D-4 变压器参数 序号 TR37 TR38 TR39 TR40 TR41 TR42 TR43 TR44 TR45 TR46 TR47 TR48 节点I BUS-11 BUS-13 BUS-30 BUS-31 BUS-32 BUS-34 BUS-33 BUS-35 BUS-36 BUS-37 BUS-38 BUS-20 节点J BUS-12 BUS-12 BUS-2 BUS-6 BUS-10 BUS-20 BUS-19 BUS-22 BUS-23 BUS-25 BUS-29 BUS-19 R(p.u.) 0.00160 0.00160 0.00000 0.00000 0.00000 0.00090 0.00070 0.00000 0.00050 0.00060 0.00080 0.00070 X(p.u.) 0.04350 0.04350 0.01810 0.02500 0.02000 0.01800 0.01420 0.01430 0.02720 0.02320 0.01560 0.01380 变比(%) 100.6 100.6 102.5 107.0 107.0 100.9 107.0 102.5 100.0 102.5 102.5 106.0

%IEEE-美国新英格兰10机39节点测试系统 % 1 2 3 4 5 6 % bus volt angle p q type bus=[ 1 1.0000 0.00 0.00 0.00 1 2 1.0000 0.00 0.00 0.00 1 3 1.0000 0.00 -3.22 -0.024 1 4 1.0000 0.00 -5.00 -1.84 1 5 1.0000 0.00 0.00 0.00 1 6 1.0000 0.00 0.00 0.00 1 7 1.0000 0.00 -2.338 -0.84 1 8 1.0000 0.00 -5.22 -1.76 1 9 1.0000 0.00 0.00 0.00 1 10 1.0000 0.00 0.00 0.00 1 11 1.0000 0.00 0.00 0.00 1 12 1.0000 0.00 -0.085 -0.88 1 13 1.0000 0.00 0.00 0.00 1 14 1.0000 0.00 0.00 0.00 1 15 1.0000 0.00 -3.20 -1.53 1 16 1.0000 0.00 -3.29 -0.323 1 17 1.0000 0.00 0.00 0.00 1 18 1.0000 0.00 -1.58 -0.30 1 19 1.0000 0.00 0.00 0.00 1 20 1.0000 0.00 -6.80 -1.03 1 21 1.0000 0.00 -2.74 -1.15 1 22 1.0000 0.00 0.00 0.00 1 23 1.0000 0.00 -2.475 -1.15 1 24 1.0000 0.00 -3.08 -0.922 1 25 1.0000 0.00 -2.24 -0.472 1 26 1.0000 0.00 -1.39 -0.17 1 27 1.0000 0.00 -2.81 -0.755 1 28 1.0000 0.00 -2.06 -0.276 1 29 1.0000 0.00 -2.835 -0.269 1 30 1.0475 0.00 2.50 0.00 2 31 1.0000 0.00 0.00 0.00 3 32 1.0000 0.00 6.50 1.759 1 33 1.0000 0.00 6.32 1.0335 1 34 1.0123 0.00 5.08 0.00 2 35 1.0493 0.00 6.50 0.00 2 36 1.0000 0.00 5.60 0.9688 1 37 1.0278 0.00 5.40 0.00 2 38 1.0265 0.00 8.30 0.00 2 39 1.0300 0.00 -1.04 0.00 2];

% 1 2 3 4 5 6 7 % line: from bus to bus R, X, G, B/2 K line=[ 2 1 0.00350 0.04110 0 0.34935 0; 39 1 0.00100 0.02500 0 0.37500 0; 3 2 0.00130 0.01510 0 0.12860 0; 25 2 0.00700 0.00860 0 0.07300 0; 4 3 0.00130 0.02130 0 0.11070 0; 18 3 0.00110 0.01330 0 0.10690 0; 5 4 0.00080 0.01280 0 0.06710 0; 14 4 0.00080 0.01290 0 6 5 0.00020 0.00260 0 8 5 0.00080 0.01120 0 7 6 0.00060 0.00920 0 11 6 0.00070 0.00820 0 8 7 0.00040 0.00460 9 8 0.00230 0.03630 0 39 9 0.00100 0.02500 0 11 10 0.00040 0.00430 0 13 10 0.00040 0.00430 0 14 13 0.00090 0.01010 0 15 14 0.00180 0.02170 0 16 15 0.00090 0.00940 0 17 16 0.00070 0.00890 0 19 16 0.00160 0.01950 0 21 16 0.00080 0.01350 0 24 16 0.00030 0.00590 0 18 17 0.00070 0.00820 0 27 17 0.00130 0.01730 0 22 21 0.00080 0.01400 0 23 22 0.00060 0.00960 0 24 23 0.00220 0.03500 0 26 25 0.00320 0.03230 0 27 26 0.00140 0.01470 0 28 26 0.00430 0.04740 0 29 26 0.00570 0.06250 0 29 28 0.00140 0.01510 0 4 0 0 0 5 0 0 0 11 12 0.00160 0.04350 0 13 12 0.00160 0.04350 0 30 2 0.00000 0.01810 0 31 6 0.00000 0.02500 0 32 10 0.00000 0.02000 0 34 20 0.00090 0.01800 0 0.06910 0; 0.02170 0; 0.07380 0; 0.05650 0; 0.06945 0; 0 0.03900 0; 0.19020 0; 0.60000 0; 0.03645 0; 0.03645 0; 0.08615 0; 0.18300 0; 0.08550 0; 0.06710 0; 0.15200 0; 0.12740 0; 0.03400 0; 0.06595 0; 0.16080 0; 0.12825 0; 0.09230 0; 0.18050 0; 0.25650 0; 0.11980 0; 0.39010 0; 0.51450 0; 0.12450 0;

0 1.0000 0 2.0000 0 100.60000/100; 0 100.60000/100; 0 102.50000/100 ; 0 107.00000/100 ; 0 107.00000/100 ; 0 100.90000/100 ;

0; 0; 33 19 0.00070 0.01420 0 0 107.00000/100 ; 35 22 0.00000 0.01430 0 0 102.50000/100 ; 36 23 0.00050 0.02720 0 0 100.00000/100 ; 37 25 0.00060 0.02320 0 0 102.50000/100 ; 38 29 0.00080 0.01560 0 0 102.50000/100 ; 20 19 0.00070 0.01380 0 0 106.00000/100] ; 计算结果牛顿-拉夫逊法潮流计算结果 节点计算结果:

n节点 节点电压 节点相角(角度) 节点注入功率 1 1.049185 2 1.053167 3 1.041493 4 1.036574 5 1.044652 6 1.043883 7 1.032645 8 1.031177 9 1.042715 10 1.046426 11 1.044322 12 1.030736 13 1.042351 14 1.036310 15 1.018517 16 1.025492 17 1.032750 18 1.034779 19 1.044862 20 0.988148 21 1.024926 22 1.042650 23 1.032952 24 1.021125 25 1.060163 26 1.052697 27 1.037683 28 1.050444 29 1.050163 30 1.004392 31 0.991632 32 1.050539 33 1.047500 34 1.012300 35 1.049300 -8.874991 -6.367180 -9.207297 -10.042585 -8.959237 -8.293104 -10.342431 -10.811816 -10.595648 -6.010476 -6.792462 -6.795388 -6.675491 -8.232337 -8.519794 -7.051856 -8.077118 -8.936485 -2.382169 -3.811032 -4.596980 -0.070512 -0.245457 -6.906503 -4.952002 -6.205207 -8.217337 -2.695196 0.063077 1.594781 2.892572 7.797786 -3.957598 1.385774 4.925324 0.000000 + j 0.000000 0.000000 + j 0.000000 -3.220000 + j -0.024000 -5.000000 + j -1.840000 0.000000 + j 0.000000 0.000000 + j 0.000000 -2.338000 + j -0.840000 -5.220000 + j -1.760000 0.000000 + j 0.000000 0.000000 + j 0.000000 0.000000 + j 0.000000 -0.085000 + j -0.880000 0.000000 + j 0.000000 0.000000 + j 0.000000 -3.200000 + j -1.530000 -3.290000 + j -0.323000 0.000000 + j 0.000000 -1.580000 + j -0.300000 0.000000 + j 0.000000 -6.800000 + j -1.030000 -2.740000 + j -1.150000 0.000000 + j 0.000000 -2.475000 + j -1.150000 -3.080000 + j -0.922000 -2.240000 + j -0.472000 -1.390000 + j -0.170000 -2.810000 + j -0.755000 -2.060000 + j -0.276000 -2.835000 + j -0.269000 6.500000 + j 1.759000 6.320000 + j 1.033500 5.600000 + j 0.968800 2.500000 + j 1.211174 5.080000 + j 1.826359 6.500000 + j 2.637566

36 1.027800 1.819476 5.400000 + j -0.108224 37 1.026500 7.125579 8.300000 + j 0.214225 38 1.030000 -10.390696 -1.040000 + j -2.291639 39 1.000000 0.000000 5.628660 + j 1.384403

线路计算结果:

n节点I 节点J 线路功率S(I,J) 线路功率S(J,I) 线路损耗dS(I,J)

2 1 1.178698 + j -0.360055 -1.174311 + j -0.360481 0.004386 + j -0.720536 39 1 0.312135

3 2 25 2 4 3 18 3 5 4 14 4 6 5 0.009257

8 5 7 6 0.041098

11 6 8 7 9 8 39 9 0.240561

11 10 13 10 14 13 15 14 16 15 17 16 19 16 0.055672

21 16 24 16 18 17 27 17 22 21 0.222826

23 22 24 23 0.028438

6.405845 + j -2.096152 -6.361848 + j 2.408287 0.043997 + j -3.633961 + j -0.542613 3.649983 + j 0.446577 0.016021 + j -0.096036 2.370242 + j -1.109311 -2.328681 + j 0.997356 0.041562 + j -0.111955 -0.750370 + j -0.307172 0.751094 + j 0.080014 0.000724 + j -0.227159 0.337560 + j -0.663855 -0.337133 + j 0.438599 0.000427 + j -0.225256 1.635254 + j 0.499000 -1.633054 + j -0.609119 0.002200 + j -0.110119 2.621711 + j -0.216428 -2.616576 + j 0.150777 0.005135 + j -0.065651 4.826035 + j -0.675350 -4.821682 + j 0.684607 0.004353 + j -3.178130 + j -1.041836 3.186428 + j 0.998989 0.008297 + j -0.042847 -4.249274 + j -0.969559 4.259899 + j 1.010657 0.010625 + j 3.465003 + j -0.270003 -3.457273 + j 0.209136 0.007730 + j -0.060866 -1.909893 + j -0.196732 1.911274 + j 0.129559 0.001381 + j -0.067173 0.132235 + j 0.116464 -0.131977 + j -0.521432 0.000258 + j -0.404968 7.617154 + j -1.902126 -7.557438 + j 2.142687 0.059717 + j -3.483660 + j -0.203064 3.488121 + j 0.171352 0.004461 + j -0.031712 -3.008372 + j -0.730489 3.011879 + j 0.688680 0.003508 + j -0.041809 -2.934129 + j -0.411463 2.941429 + j 0.307264 0.007300 + j -0.104199 -0.311115 + j -0.998556 0.312417 + j 0.627891 0.001303 + j -0.370665 2.896296 + j 0.430232 -2.888885 + j -0.531444 0.007411 + j -0.101212 -2.048841 + j 0.950740 2.052282 + j -1.049122 0.003441 + j -0.098383 4.542969 + j 0.681545 -4.511670 + j -0.625873 0.031300 + j 3.324778 + j -0.302389 -3.316338 + j 0.177006 0.008440 + j -0.125383 0.410793 + j -0.811601 -0.410571 + j 0.744757 0.000222 + j -0.066844 -1.917560 + j 0.363855 1.920087 + j -0.475208 0.002527 + j -0.111353 -0.128621 + j 0.132648 0.128754 + j -0.475531 0.000133 + j -0.342884 6.093176 + j 1.070437 -6.064778 + j -0.847611 0.028398 + j -0.406149 + j -1.116063 0.406824 + j 0.928040 0.000675 + j -0.188024 -3.490793 + j -0.110399 3.516516 + j 0.138837 0.025723 + j


基于牛顿拉夫逊法潮流计算的matlab实验报告(2).doc 将本文的Word文档下载到电脑 下载失败或者文档不完整,请联系客服人员解决!

下一篇:18项医疗核心制度(最新)

相关阅读
本类排行
× 注册会员免费下载(下载后可以自由复制和排版)

马上注册会员

注:下载文档有可能“只有目录或者内容不全”等情况,请下载之前注意辨别,如果您已付费且无法下载或内容有问题,请联系我们协助你处理。
微信: QQ: