torre(barajas julio)

7/21/2019 Torre(Barajas Julio)

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INSTITUTO TECNOLÓGICO SUPERIOR DE IRAPUATO

ITESIINSTITUTO TECNOLÓGICO SUPERIOR DE IRAPUATO

ANALISIS DE DISTINTOS TIPOS DELINEA DE TRASMISION.

ALUMNOS:

JOSÉ FERNANDO BARAJAS CASTRO. JULIO ADRIAN ORTIZ MARTINEZ.

CARRERA: ING. ELECTROMECÁNICA.

MATERIA: SISTEMAS DE POTENCIA.

MAESTRO: M.I. JOSE MIGUEL GARCIA GUZMAN

FIGURA1 .Dimensiones i!o "e o##e $%o #$ns!o#$"$ 11& '( %n )i#)%io

DATOS OBTENIDOS DEL ANALISISDE UNA TORRE DE TRASMISION

PARA UN CONDUCTOR POR FASE.

ANALISIS DE LA INDUCTANCIA EN UNA LINEA DE TRASMISION

TIPO DEL(mh/km)= L (h/m)=

XL(ohms)=

XLpu115=

XLpu230=

XLpu40=

CONDUCTOR 1.0e-005 *

WAXWIN 1.3914 0.1391 157.3583 1.1899 0.2975 0.09

PARTRIDGE 1.3808 0.1381 156.1647 1.1808 0.2952 0.09OSTRICH 1.3693 0.1369 154.8639 1.171 0.2927 0.09

ER!IN 1.3681 0.1368 154.7313 1.17 0.2925 0.09

!INNET 1.3576 0.1358 153.5397 1.161 0.2902 0.0

ORIO!E 1.3521 0.1352 152.9208 1.1563 0.2891 0.09

CHI"CADEE 1.3516 0.1352 152.8598 1.1558 0.289 0.09

I#IA 1.3411 0.1341 151.6737 1.1469 0.2867 0.09

PE!ICAN 1.3335 0.1333 150.8125 1.1404 0.2851 0.09

$!IC"ER 1.3257 0.1326 149.9321 1.1337 0.2834 0.09

HAW" 1.3229 0.1323 149.6184 1.1313 0.2828 0.09HEN 1.3171 0.1317 148.9633 1.1264 0.2816 0.09

OSPRE% 1.318 0.1318 149.0644 1.1271 0.2818 0.09

PARA"EET 1.3103 0.131 148.1897 1.1205 0.2801 0.09

DO&E 1.3074 0.1307 147.8606 1.118 0.2795 0.09

ROO" 1.2969 0.1297 146.6812 1.1091 0.2773 0.09

GROS#EA" 1.2942 0.1294 146.3732 1.1068 0.2767 0.09

DRA"E 1.2717 0.1272 143.8233 1.0875 0.2719 0.08

TERN 1.2799 0.128 144.7587 1.0946 0.2736 0.09

RAI! 1.2617 0.1262 142.6944 1.079 0.2697 0.08CARDINA! 1.2565 0.1256 142.1057 1.0745 0.2686 0.08

ORTO!AN 1.2536 0.1254 141.7802 1.0721 0.268 0.08

#!UE'A% 1.2462 0.1246 140.944 1.0657 0.2664 0.085

$INCH 1.2408 0.1241 140.3296 1.0611 0.2653 0.08

#ITTERN 1.2329 0.1233 139.4382 1.0544 0.2636 0.08

PHEASANT 1.2275 0.1227 138.8242 1.0497 0.2624 0.08#O#A!IN" 1.2211 0.1221 138.1012 1.0442 0.2611 0.08

P!O&ER 1.2159 0.1216 137.5098 1.0398 0.2599 0.08

!APWING 1.2109 0.1211 136.9453 1.0355 0.2589 0.08

$A!CON 1.2052 0.1205 136.3022 1.0306 0.2577 0.08

#!UE#IRD 1.1789 0.1179 133.3352 1.0082 0.2521 0.08

ANALISIS DE LA CAPACITANCIA EN UNA LINEA DE

TRASMISION.

TIPO DEC(µf/km)= C(F/m) =

XC(ohm)=

XCpu115=

XCpu230=

XCpu400=

CONDUCTOR

1.0e-011*

1.0e(003*

WAXWIN 0.0083 0.8291 1.0666 8.0647 2.0162 0.6666

PARTRIDGE 0.0084 0.8357 1.0582 8.0013 2.0003 0.6614

OSTRICH 0.0084 0.843 1.049 7.9321 1.983 0.6556

ER!IN 0.0084 0.8437 1.0481 7.9251 1.9813 0.6551

!INNET 0.0085 0.8505 1.0397 7.8617 1.9654 0.6498

ORIO!E 0.0085 0.8541 1.0354 7.8288 1.9572 0.6471

CHI"CADEE 0.0085 0.8544 1.0349 7.8256 1.9564 0.6468

I#IA 0.0086 0.8614 1.0266 7.7625 1.9406 0.6416

PE!ICAN 0.0087 0.8665 1.0205 7.7168 1.9292 0.6378

$!IC"ER 0.0087 0.8718 1.0144 7.67 1.9175 0.634

HAW" 0.0087 0.8737 1.0121 7.6533 1.9133 0.6326

HEN 0.0088 0.8777 1.0075 7.6184 1.9046 0.6297OSPRE% 0.0088 0.8771 1.0083 7.6238 1.906 0.6302

PARA"EET 0.0088 0.8824 1.0021 7.5773 1.8943 0.6263

DO&E 0.0088 0.8845 0.9998 7.5598 1.89 0.6249

ROO" 0.0089 0.8919 0.9915 7.4971 1.8743 0.6197

GROS#EA" 0.0089 0.8938 0.9893 7.4808 1.8702 0.6183

DRA"E 0.0091 0.9103 0.9714 7.3452 1.8363 0.6071 TERN 0.009 0.9042 0.978 7.3949 1.8487 0.6112

RAI! 0.0092 0.9178 0.9635 7.2852 1.8213 0.6022

CARDINA! 0.0092 0.9218 0.9593 7.2539 1.8135 0.5996

ORTO!AN 0.0092 0.924 0.957 7.2366 1.8091 0.5981

#!UE'A% 0.0093 0.9297 0.9512 7.1921 1.798 0.5945

$INCH 0.0093 0.9339 0.9468 7.1595 1.7899 0.5918

#ITTERN 0.0094 0.9402 0.9406 7.1121 1.778 0.5879

PHEASANT 0.0094 0.9445 0.9363 7.0794 1.7699 0.5852

#O#A!IN" 0.0095 0.9497 0.9312 7.041 1.7603 0.582

P!O&ER 0.0095 0.9539 0.927 7.0096 1.7524 0.5794

!APWING 0.0096 0.958 0.923 6.9796 1.7449 0.5769

$A!CON 0.0096 0.9539 0.9185 6.9454 1.7363 0.5741

#!UE#IRD 0.0098 0.958 0.8977 6.7876 1.6969 0.561

PARA DOS CONDUCTOR POR FASE.

ANALISIS DE LA INDUCTANCIA EN UNA LINEA DE TRASMISION.

TIPO DEL(mh/km)= L(h/m) =

XL(ohms)=

XLpu115=

XLpu230=

XLpu400=

CONDUCTOR 1.0e-005 *

WAXWIN 1.1797 0.118 133.4229 1.0089 0.2522 0.0834

PARTRIDGE 1.1744 0.1174 132.826 1.0044 0.2511 0.083

OSTRICH 1.1687 0.1169 132.1757 0.9994 0.2499 0.0826

ER!IN 1.1681 0.1168 132.1093 0.9989 0.2497 0.0826!INNET 1.1628 0.1163 131.5135 0.9944 0.2486 0.0822

ORIO!E 1.1601 0.116 131.2041 0.9921 0.248 0.082

CHI"CADEE 1.1598 0.116 131.1736 0.9919 0.248 0.082

I#IA 1.1546 0.1155 130.5806 0.9874 0.2468 0.0816

PE!ICAN 1.1508 0.1151 130.15 0.9841 0.246 0.0813

$!IC"ER 1.1469 0.1147 129.7098 0.9808 0.2452 0.0811

HAW" 1.1455 0.1145 129.5529 0.9796 0.2449 0.081

HEN 1.1426 0.1143 129.2253 0.9771 0.2443 0.0808

OSPRE% 1.143 0.1143 129.2759 0.9775 0.2444 0.0808PARA"EET 1.1392 0.1139 128.8386 0.9742 0.2436 0.0805

DO&E 1.1377 0.1138 128.674 0.973 0.2432 0.0804

ROO" 1.1325 0.1133 128.0843 0.9685 0.2421 0.0801

GROS#EA" 1.1312 0.1131 127.9303 0.9673 0.2418 0.08

DRA"E 1.1199 0.112 126.6553 0.9577 0.2394 0.0792

TERN 1.124 0.1124 127.1231 0.9612 0.2403 0.0795

RAI! 1.1149 0.1115 126.0909 0.9534 0.2384 0.0788

CARDINA! 1.1123 0.1112 125.7965 0.9512 0.2378 0.0786

ORTO!AN 1.1108 0.1111 125.6338 0.95 0.2375 0.0785#!UE'A% 1.1071 0.1107 125.2157 0.9468 0.2367 0.0783

$INCH 1.1044 0.1104 124.9085 0.9445 0.2361 0.0781

#ITTERN 1.1005 0.11 124.4628 0.9411 0.2353 0.0778

PHEASANT 1.0978 0.1098 124.1558 0.9388 0.2347 0.0776

#O#A!IN" 1.0946 0.1095 123.7943 0.9361 0.234 0.0774

P!O&ER 1.092 0.1092 123.4986 0.9338 0.2335 0.0772

!APWING 1.0895 0.1089 123.2164 0.9317 0.2329 0.077

$A!CON 1.0866 0.1087 122.8948 0.9293 0.2323 0.0768

#!UE#IRD 1.0735 0.1074 121.4113 0.918 0.2295 0.0759 ANALISIS DE LA CAPACITANCIA EN UNA LINEA DE

TRASMISION.

TIPO DEC(µf/km)= C(f/m) =

XC(ohms) =

XCpu115 =

XCpu230 =

XCpu400 =

CONDUCTOR

1.0e-010*

WAXWIN 0.0096 0.0963 918.1601 6.9426 1.7357 0.5739

PARTRIDGE 0.0097 0.0968 913.9641 6.9109 1.7277 0.5712

OSTRICH 0.0097 0.0972 909.3917 6.8763 1.7191 0.5684

ER!IN 0.0097 0.0973 908.9254 6.8728 1.7182 0.5681

!INNET 0.0098 0.0977 904.7365 6.8411 1.7103 0.5655

ORIO!E 0.0098 0.098 902.5609 6.8247 1.7062 0.5641

CHI"CADEE 0.0098 0.098 902.3466 6.823 1.7058 0.564

I#IA 0.0098 0.0985 898.1771 6.7915 1.6979 0.5614

PE!ICAN 0.0099 0.0988 895.1498 6.7686 1.6922 0.5595

$!IC"ER 0.0099 0.0991 892.0549 6.7452 1.6863 0.5575

HAW" 0.0099 0.0993 890.952 6.7369 1.6842 0.5568

HEN 0.0099 0.0995 888.6492 6.7195 1.6799 0.5554

OSPRE% 0.0099 0.0995 889.0047 6.7222 1.6805 0.5556

PARA"EET 0.01 0.0998 885.9299 6.6989 1.6747 0.5537

DO&E 0.01 0.0999 884.7731 6.6902 1.6725 0.553

ROO" 0.01 0.1004 880.627 6.6588 1.6647 0.5504

GROS#EA" 0.0101 0.1005 879.5443 6.6506 1.6627 0.5497DRA"E 0.0102 0.1016 870.5806 6.5828 1.6457 0.5441

TERN 0.0101 0.1012 873.8689 6.6077 1.6519 0.5462

RAI! 0.0102 0.102 866.6123 6.5528 1.6382 0.5416

CARDINA! 0.0102 0.1023 864.5428 6.5372 1.6343 0.5403

ORTO!AN 0.0102 0.1024 863.3987 6.5285 1.6321 0.5396

#!UE'A% 0.0103 0.1028 860.459 6.5063 1.6266 0.5378

$INCH 0.0103 0.103 858.2993 6.49 1.6225 0.5364

#ITTERN 0.0103 0.1034 855.1658 6.4663 1.6166 0.5345

PHEASANT 0.0104 0.1037 853.0073 6.45 1.6125 0.5331

#O#A!IN" 0.0104 0.104 850.4659 6.4307 1.6077 0.5315

P!O&ER 0.0104 0.1042 848.387 6.415 1.6038 0.5302

!APWING 0.0104 0.1045 846.4027 6.4 1.6 0.529

$A!CON 0.0105 0.1048 844.1419 6.3829 1.5957 0.5276

#!UE#IRD 0.0106 0.1061 833.7119 6.3041 1.576 0.5211

PARA TRES CONDUCTOR POR FASE.

ANALISIS DE LA INDUCTANCIA EN UNA LINEA DE

TRASMISION.

TIPO DEL(M/!M)= L(/M) =

XL(OM") =

XLP#115 =

XLP#230 =

XLP#400 =

CONDUCTOR

1.0E-005*

WAXWIN 1.1092 0.1109 125.4444 0.9485 0.2371 0.0784

PARTRIDGE 1.1057 0.1106 125.0465 0.9455 0.2364 0.0782

OSTRICH 1.1018 0.1102 124.6129 0.9423 0.2356 0.0779

ER!IN 1.1014 0.1101 124.5687 0.9419 0.2355 0.0779

!INNET 1.0979 0.1098 124.1715 0.9389 0.2347 0.0776

ORIO!E 1.0961 0.1096 123.9652 0.9374 0.2343 0.0775

CHI"CADEE 1.0959 0.1096 123.9449 0.9372 0.2343 0.0775

I#IA 1.0924 0.1092 123.5495 0.9342 0.2336 0.0772

PE!ICAN 1.0899 0.109 123.2624 0.932 0.233 0.077

$!IC"ER 1.0873 0.1087 122.969 0.9298 0.2325 0.0769

HAW" 1.0864 0.1086 122.8644 0.929 0.2323 0.0768

HEN 1.0844 0.1084 122.646 0.9274 0.2318 0.0767

OSPRE% 1.0847 0.1085 122.6797 0.9276 0.2319 0.0767

PARA"EET 1.0821 0.1082 122.3882 0.9254 0.2314 0.0765

DO&E 1.0812 0.1081 122.2785 0.9246 0.2312 0.0764ROO" 1.0777 0.1078 121.8853 0.9216 0.2304 0.0762

GROS#EA" 1.0768 0.1077 121.7827 0.9209 0.2302 0.0761

DRA"E 1.0693 0.1069 120.9327 0.9144 0.2286 0.075613

TERN 1.072 0.1072 121.2445 0.9168 0.2292 0.0758

RAI! 1.066 0.1066 120.5564 0.9116 0.2279 0.0753

CARDINA! 1.0642 0.1064 120.3602 0.9101 0.2275 0.0752ORTO!AN 1.0633 0.1063 120.2517 0.9093 0.2273 0.0752

#!UE'A% 1.0608 0.1061 119.9729 0.9072 0.2268 0.075

$INCH 1.059 0.1059 119.7681 0.9056 0.2264 0.0749

#ITTERN 1.0564 0.1056 119.471 0.9034 0.2258 0.0747

PHEASANT 1.0545 0.1055 119.2663 0.9018 0.2255 0.0745

#O#A!IN" 1.0524 0.1052 119.0253 0.9 0.225 0.0744

P!O&ER 1.0507 0.1051 118.8282 0.8985 0.2246 0.0743

!APWING 1.049 0.1049 118.64 0.8971 0.2243 0.0742

$A!CON 1.0471 0.1047 118.4257 0.8955 0.2239 0.074#!UE#IRD 1.0384 0.1038 117.4367 0.888 0.222 0.0734

TRASMISION.

TIPO DE C(µf/km) C(f/m) XC(ohm)XCpu115

XCpu230

XCpu400

CONDUCTOR

1.0e-010*

WAXWIN 0.0102 0.1018 868.693 6.5686 1.6421 0.5429PARTRIDGE 0.0102 0.1021 865.8957 6.5474 1.6369 0.5412OSTRICH 0.0102 0.1025 862.8474 6.5244 1.6311 0.5393ER!IN 0.0103 0.1025 862.5365 6.522 1.6305 0.5391!INNET 0.0103 0.1029 859.7439 6.5009 1.6252 0.5373ORIO!E 0.0103 0.103 858.2935 6.4899 1.6225 0.5364CHI"CADEE 0.0103 0.103 858.1506 6.4889 1.6222 0.5363I#IA 0.0103 0.1034 855.371 6.4678 1.617 0.5346PE!ICAN 0.0104 0.1036 853.3528 6.4526 1.6131 0.5333$!IC"ER 0.0104 0.1039 851.2895 6.437 1.6092 0.5321HAW" 0.0104 0.104 850.5543 6.4314 1.6079 0.5316

HEN 0.0104 0.1042 849.0191 6.4198 1.605 0.5306OSPRE% 0.0104 0.1041 849.256 6.4216 1.6054 0.5308PARA"EET 0.0104 0.1044 847.2062 6.4061 1.6015 0.5295DO&E 0.0104 0.1045 846.435 6.4003 1.6001 0.529

ROO" 0.0105 0.1048 843.671 6.3794 1.5948 0.5273GROS#EA" 0.0105 0.1049 842.9491 6.3739 1.5935 0.5268DRA"E 0.0106 0.1057 836.9733 6.3287 1.5822 0.5231

TERN 0.0105 0.1054 839.1655 6.3453 1.5863 0.5245RAI! 0.0106 0.106 834.3278 6.3087 1.5772 0.5215CARDINA! 0.0106 0.1062 832.9481 6.2983 1.5746 0.5206ORTO!AN 0.0106 0.1063 832.1854 6.2925 1.5731 0.5201#!UE'A% 0.0107 0.1065 830.2256 6.2777 1.5694 0.5189$INCH 0.0107 0.1067 828.7858 6.2668 1.5667 0.518#ITTERN 0.0107 0.107 826.6968 6.251 1.5628 0.5167PHEASANT 0.0107 0.1072 825.2578 6.2401 1.56 0.5158#O#A!IN" 0.0107 0.1074 823.5635 6.2273 1.5568 0.5147P!O&ER 0.0108 0.1076 822.1776 6.2168 1.5542 0.5139!APWING 0.0108 0.1077 820.8547 6.2068 1.5517 0.513

$A!CON 0.0108 0.1079 819.3475 6.1954 1.5489 0.5121#!UE#IRD 0.0109 0.1089 812.3942 6.1429 1.5357 0.5077

PARA CUATRO CONDUCTOR POR

ANALISIS DE LA INDUCTANCIA EN UNA LINEA DE

TRASMISION.

TIPO DEL(mh/km) L(h/m) XL(ohm)

XLpu115

XLpu230

XLpu400

CONDUCTOR

1.0e-005

WAXWIN 1.0739 0.1074 121.4551 0.9184 0.2296 0.0759PARTRIDGE 1.0713 0.1071 121.1567 0.9161 0.229 0.0757

OSTRICH 1.0684 0.1068 120.8315 0.9137 0.2284 0.0755

ER!IN 1.0681 0.1068 120.7984 0.9134 0.2284 0.0755

!INNET 1.0655 0.1065 120.5005 0.9112 0.2278 0.0753

ORIO!E 1.0641 0.1064 120.3457 0.91 0.2275 0.0752CHI"CADEE 1.064 0.1064 120.3305 0.9099 0.2275 0.0752

I#IA 1.0613 0.1061 120.034 0.9076 0.2269 0.075

PE!ICAN 1.0594 0.1059 119.8187 0.906 0.2265 0.0749

$!IC"ER 1.0575 0.1057 119.5986 0.9043 0.2261 0.0747

HAW" 1.0568 0.1057 119.5201 0.9037 0.2259 0.0747

HEN 1.0553 0.1055 119.3564 0.9025 0.2256 0.0746

OSPRE% 1.0556 0.1056 119.3817 0.9027 0.2257 0.0746

PARA"EET 1.0536 0.1054 119.163 0.901 0.2253 0.0745

DO&E 1.0529 0.1053 119.0807 0.9004 0.2251 0.0744

ROO" 1.0503 0.105 118.7859 0.8982 0.2245 0.0742

GROS#EA" 1.0496 0.105 118.7089 0.8976 0.2244 0.0742

DRA"E 1.044 0.1044 118.0714 0.8928 0.2232 0.0738

TERN 1.046 0.1046 118.3052 0.8946 0.2236 0.0739RAI! 1.0415 0.1041 117.7892 0.8907 0.2227 0.0736

CARDINA! 1.0402 0.104 117.642 0.8895 0.2224 0.0735

ORTO!AN 1.0395 0.1039 117.5606 0.8889 0.2222 0.0735

#!UE'A% 1.0376 0.1038 117.3515 0.8873 0.2218 0.0733

$INCH 1.0363 0.1036 117.1979 0.8862 0.2215 0.0732

#ITTERN 1.0343 0.1034 116.9751 0.8845 0.2211 0.0731

PHEASANT 1.0329 0.1033 116.8216 0.8833 0.2208 0.073

#O#A!IN" 1.0313 0.1031 116.6409 0.882 0.2205 0.0729

P!O&ER 1.03 0.103 116.493 0.8809 0.2202 0.0728

!APWING 1.0288 0.1029 116.3519 0.8798 0.2199 0.0727

$A!CON 1.0274 0.1027 116.1911 0.8786 0.2196 0.0726

#!UE#IRD 1.0208 0.1021 115.4493 0.873 0.2182 0.0722

TRASMISION.

TIPO DE C(µf/km) C(f/m) =

XC(ohm)

XCpu115

XCpu230

XCpu400

CONDUCTOR

1.0e-010

WAXWIN0.0106 0.1065

830.2548 6.2779 1.5695 0.5189

PARTRIDGE

0.0107 0.1068

828.156

8 6.2621 1.5655 0.5176OSTRICH

0.0107 0.1071825.870

6 6.2448 1.5612 0.5162

ER!IN0.0107 0.1071

825.6374 6.243 1.5608 0.516

!INNET 0.0107 0.1074 823.543 6.2272 1.5568 0.5147

ORIO!E0.0108 0.1075

822.4552 6.2189 1.5547 0.514

CHI"CADEE 0.0108 0.1075 822.348 6.2181 1.5545 0.514

I#IA0.0108 0.1078

820.2633 6.2024 1.5506 0.5127

PE!ICAN 0.0108 0.108

818.749

6 6.1909 1.5477 0.5117

$!IC"ER0.0108 0.1082

817.2022 6.1792 1.5448 0.5108

HAW" 0.0108 0.1083

816.6508 6.1751 1.5438 0.5104

HEN0.0108 0.1084

815.4993 6.1663 1.5416 0.5097

OSPRE%0.0108 0.1084

815.6771 6.1677 1.5419 0.5098

PARA"EET0.0109 0.1086

814.1397 6.1561 1.539 0.5088

DO&E 0.0109 0.1087 813.5613 6.1517 1.5379 0.5085

ROO" 0.0109 0.109

811.4883 6.136 1.534 0.5072

GROS#EA" 0.0109 0.109

810.9469 6.1319 1.533 0.5068

DRA"E 0.011 0.1097 806.465 6.098 1.5245 0.504

TERN0.0109 0.1094

808.1092 6.1105 1.5276 0.5051

RAI!0.011 0.1099

804.4809 6.083 1.5208 0.5028

CARDINA! 0.011 0.1101

803.446

1 6.0752 1.5188 0.5022

ORTO!AN0.011 0.1101

802.8741 6.0709 1.5177 0.5018

#!UE'A%0.011 0.1103

801.4043 6.0598 1.5149 0.5009

$INCH0.011 0.1105

800.3244 6.0516 1.5129 0.5002

#ITTERN0.0111 0.1107

798.7576 6.0398 1.5099 0.4992

PHEASANT0.0111 0.1109

797.6784 6.0316 1.5079 0.4985

#O#A!IN" 0.0111 0.111796.407

7 6.022 1.5055 0.4978795.368

CONC!UCION

Fases con n y n+1 conductores tendrán enor y ayor ca!ac"tanc"a en e##asres!ect"$aente%

A# auentar e# rad"o de #os conductores en e##as se tendrá un "ncreento

ca!ac"t"$o &'C() s"endo ayor en !ara #a *ase de n conductores co!arado con #a

*ase de n+1 conductores%

A# ana#"ar #as *ases y e$a#uar su co!orta"ento ,ue !resentan !ara #a

"nductanc"a) se o-ser$a ,ue #a *ase con &n( conductores !resenta ayor

"nductanc"a ,ue #a *ase con &n+1( conductores%

Cuando se auenta e# rad"o de #os conductores se !resentara un "ncreento

ne.at"$o en #a "nductanc"a &/'L( !ara #as dos *ases) s"endo ayor !ara #a *ase con

n conductores res!ecto a #a de &n+1( conductores%

Carrera0

Ing. ELECTROMECÁNICA

ATERIA0

SISTEMAS ELÈCTRICOS DE POTENCIA 1

EXAMEN SEGUNDO PARCIAL

ALUNOS0

JESÚS GONZÁLEZ PONCE

DANIEL DELGADO MARTÌNEZ

Pro*esor0

JOSE MIGUEL GARCÌA GUZMAN

1% Deter"ne #a "nductanc"a y ca!ac"tanc"a !or *ase) en 23 y 234) de una#5nea de trans"s"6n ,ue ut"#"a #a estructura ,ue se #e 7a as".nado ycons"derando cada uno de #os conductores ACSR ostrados en #a ta-#a A%8!ara e# caso de a( 1 conductor !or *ase) -( 9 conductores !or *ase) c( 8conductores !or *ase y d( : conductores !or *ase% Presente #os datos de*ora ordenada en una ta-#a%

Ta-#a de "nductanc"a y ca!ac"tanc"a en torre reten"da !ara :;; 4<

CO$D#CTO

%&DIO(m

L (/m)

( F/km)

C (F/m) '10

+, 0.007734

1 1.5536 1.5536 0.0074 0.0074

2 1.342 1.342 0.0084 0.0084

3 1.2714 1.2714 0.0089 0.0089

4 1.2189 1.2189 0.0092 0.0092

/+e 0.008153

1 1.543 1.543 0.0074 0.0074

2 1.3367 1.3367 0.0085 0.0085

3 1.2679 1.2679 0.0089 0.0089

4 1.2163 1.2163 0.0092 0.0092

0.0086361 1.5315 1.5315 0.0075 0.00752 1.3309 1.3309 0.0085 0.0085

3 1.2641 1.2641 0.0089 0.0089

4 1.2134 1.2134 0.0093 0.0093

e 0.008686

1 1.5304 1.5304 0.0075 0.0075

2 1.3303 1.3303 0.0085 0.0085

3 1.2637 1.2637 0.0089 0.0089

4 1.213 1.213 0.0093 0.0093

!e 0.009156

1 1.5198 1.5198 0.0076 0.0076

2 1.3251 1.3251 0.0086 0.0086

3 1.2602 1.2602 0.0089 0.00894 1.2105 1.2105 0.0093 0.0093Oe 0.009410

71 1.5144 1.5144 0.0076 0.00762 1.3223 1.3223 0.0086 0.0086

3 1.2583 1.2583 0.009 0.009

4 1.209 1.209 0.0093 0.0093

C+ee 0.009436

1 1.5138 1.5138 0.0076 0.00762 1.3221 1.3221 0.0086 0.0086

3 1.2581 1.2581 0.009 0.009

4 1.209 1.209 0.0093 0.0093

I:+ 0.009944

1 1.5033 1.5033 0.0077 0.0077

2 1.3168 1.3168 0.0086 0.0086

3 1.2547 1.2547 0.009 0.009

4 1.2063 1.2063 0.0093 0.0093

&Cont"nuac"6n(

CO$D#CTO%

%&DIO(m)

(m/km)

L (/m)'10

C( F/km)

C (F/m) '1012 1

Pe+ 0.010337

1 1.4956 1.4956 0.0077 0.0077

2 1.3129 1.3129 0.0086 0.0086

3 1.2521 1.2521 0.009 0.009

4 1.2044 1.2044 0.0093 0.0093

$e 0.010744

1 1.4878 1.4878 0.0077 0.0077

2 1.3091 1.3091 0.0087 0.0087

3 1.2495 1.2495 0.009 0.009

4 1.2025 1.2025 0.0093 0.0093

H+ 0.010896

1 1.485 1.485 0.0077 0.0077

2 1.3077 1.3077 0.0087 0.0087

3 1.2486 1.2486 0.009 0.009

4 1.2018 1.2018 0.0094 0.0094

He 0.011214

1 1.4793 1.4793 0.0078 0.0078

2 1.3048 1.3048 0.0087 0.0087

3 1.2466 1.2466 0.009 0.009

4 1.2003 1.2003 0.0094 0.0094

O/e; 0.011163

1 1.4802 1.4802 0.0078 0.0078

2 1.3053 1.3053 0.0087 0.0087

3 1.2469 1.2469 0.009 0.009

4 1.2006 1.2006 0.0094 0.0094P++ee 0.011607 1 1.4724 1.4724 0.0078 0.0078

2 1.3014 1.3014 0.0087 0.0087

3 1.2443 1.2443 0.0091 0.0091

4 1.1986 1.1986 0.0094 0.0094

D<e 0.011772

1 1.4696 1.4696 0.0078 0.0078

2 1.2999 1.2999 0.0087 0.0087

3 1.2434 1.2434 0.0091 0.0091

4 1.1979 1.1979 0.0094 0.0094

R 0.012407

1 1.4591 1.4591 0.0079 0.0079

2 1.2947 1.2947 0.0088 0.0088

3 1.2399 1.2399 0.0091 0.0091

4 1.1953 1.1953 0.0094 0.0094

&Cont"nuac"6n(

CO$D#CTO%

%&DIO(m) $

L(m/km

L (/m)'10

C( F/km)

C (F/m) '1012 1

G:e+ 0.012573

1 1.4564 1.4564 0.0079 0.0079

2 1.2934 1.2934 0.0088 0.0088

3 1.239 1.239 0.0091 0.00914 1.1946 1.1946 0.0094 0.0094

D+e 0.014071

1 1.4339 1.4339 0.008 0.008

2 1.2821 1.2821 0.0088 0.0088

3 1.2315 1.2315 0.0092 0.0092

4 1.189 1.189 0.0095 0.0095

Te 0.013500

1 1.4422 1.4422 0.008 0.008

2 1.2862 1.2862 0.0088 0.0088

3 1.2343 1.2343 0.0091 0.0091

4 1.191 1.191 0.0094 0.0094

R+ 0.014795

1 1.4239 1.4239 0.0081 0.00812 1.2771 1.2771 0.0089 0.0089

3 1.2282 1.2282 0.0092 0.0092

4 1.1865 1.1865 0.0095 0.0095

C++ 0.015189

1 1.4186 1.4186 0.0081 0.0081

2 1.2745 1.2745 0.0089 0.0089

3 1.2264 1.2264 0.0092 0.00924 1.1852 1.1852 0.0095 0.0095

O+ 0.015405

1 1.4158 1.4158 0.0081 0.0081

2 1.273 1.273 0.0089 0.0089

3 1.2255 1.2255 0.0092 0.0092

4 1.1844 1.1844 0.0095 0.0095

#=e>+; 0.015989

1 1.4083 1.4083 0.0082 0.0082

2 1.2693 1.2693 0.0089 0.0089

3 1.223 1.223 0.0092 0.0092

4 1.1826 1.1826 0.0095 0.0095

$ 0.016421

1 1.403 1.403 0.0082 0.00822 1.2667 1.2667 0.009 0.009

3 1.2212 1.2212 0.0092 0.0092

4 1.1813 1.1813 0.0095 0.0095

&Cont"nuac"6n(

CO$D#CTO%

%&DIO(m) $

L(m/km

L (/m)'10

C( F/km)

C (F/m) '1012 1

#e 0.017081

1 1.3951 1.3951 0.0083 0.0083

2 1.2627 1.2627 0.009 0.009

3 1.2186 1.2186 0.0093 0.0093

4 1.1793 1.1793 0.0095 0.0095

0.017551

1 1.3897 1.3897 0.0083 0.0083

2 1.26 1.26 0.009 0.009

3 1.2168 1.2168 0.0093 0.00934 1.1779 1.1779 0.0095 0.0095

#: 0.0181229

1 1.3833 1.3833 0.0083 0.00832 1.2568 1.2568 0.009 0.009

3 1.2146 1.2146 0.0093 0.0093

4 1.1763 1.1763 0.0096 0.0096

P<e 0.018605

1 1.378 1.378 0.0084 0.00842 1.2542 1.2542 0.009 0.009

3 1.2129 1.2129 0.0093 0.0093

4 1.175 1.175 0.0096 0.0096

!+/ 0.019075

1 1.373 1.373 0.0084 0.0084

2 1.2517 1.2517 0.0091 0.0091

3 1.2112 1.2112 0.0093 0.0093

4 1.1738 1.1738 0.0096 0.0096

$+ 0.019621

1 1.3674 1.3674 0.0084 0.0084

2 1.2489 1.2489 0.0091 0.0091

3 1.2093 1.2093 0.0093 0.00934 1.1724 1.1724 0.0096 0.0096

#=e: 0.022377

1 1.3411 1.3411 0.0086 0.0086

2 1.2357 1.2357 0.0092 0.0092

3 1.2006 1.2006 0.0094 0.0094

4 1.1658 1.1658 0.0096 0.0096

9% Deter"ne #a reactanc"a "nduct"$a y ca!ac"t"$a) tanto en !u cooen o7s) de #a #5nea de trans"s"6n anter"or coo en cada unode #os conductores de #a Ta-#a A%8 !ara e# caso de a( 1conductor !or *ase &en 11=4<) 98;4< > :;;4<() -( 9

conductores !or *ase &en 11=4<) 98;4< > :;;4<() c( 8conductores !or *ase &en 11=4<) 98;4< > :;;4<( y d( :conductores !or *ase &en 11=4<) 98;4< > :;;4<(% Su!on.a una

*recuenc"a de o!erac"6n de# s"stea de ?; 2% Presente #osdatos de *ora ordenada en una ta-#a%

Ta-#a de reactanc"a "nduct"$a en o7s y !u !ara una #5nea de 8;; 4

CO$D#CTO%

%&DIO(m)

$ XL (*)

XLP#+115

XLP#+230

XLP#+400

+, 0.0077

1 175.70

84 1.3286 0.3322 0.1098

2151.77

7 1.1477 0.2869 0.0949

3143.79

23 1.0873 0.2718 0.0899

4137.85

47 1.0424 0.2606 0.0862

/+e 0.0081

1174.50

96 1.3195 0.3299 0.1091

2151.17

76 1.1431 0.2858 0.0945

3143.39

64 1.0843 0.2711 0.0896

4137.56

06 1.0402 0.26 0.086

0.0086

1173.20

9 1.3097 0.3274 0.1083

2150.52

16 1.1382 0.2845 0.0941

3142.96

67 1.081 0.2703 0.0894

4137.23

26 1.0377 0.2594 0.0858

e 0.0086

1173.08

46 1.3088 0.3272 0.1082

2150.45

37 1.1376 0.2844 0.094

3142.92

14 1.0807 0.2702 0.0893

4137.18

74 1.0373 0.2593 0.0857

!e 0.0091

1171.88

57 1.2997 0.3249 0.1074

2149.86

56 1.1332 0.2833 0.0937

3142.52

56 1.0777 0.2694 0.0891

4136.90

46 1.0352 0.2588 0.0856

Oe 0.0094

1171.27

5 1.2951 0.3238 0.107

2149.54

9 1.1308 0.2827 0.0935

3142.31

07 1.0761 0.269 0.0889

4 136.735 1.0339 0.2585 0.0855

&Cont"nuac"6n(

CO$D#CTO% %&DIO(m) $ XL (*) XLP#+115 XLP#+230 XLP#+400

C+ee 0.0094361

1 171.2071 1.2946 0.3236 0.107

2 149.5263 1.1306 0.2827 0.0935

3 142.2881 1.0759 0.269 0.0889

4 136.735 1.0339 0.2585 0.0855

I:+ 0.0099441

1 170.0196 1.2856 0.3214 0.1063

2 148.9269 1.1261 0.2815 0.0931

3 141.9036 1.073 0.2682 0.0887

4 136.4296 1.0316 0.2579 0.0853

Pe+ 0.01033781 169.1488 1.279 0.3198 0.10572 148.4858 1.1228 0.2807 0.0928

3 141.6095 1.0708 0.2677 0.0885

4 136.2147 1.03 0.2575 0.0851

$e 0.0107442

1 168.2666 1.2723 0.3181 0.1052

2 148.0561 1.1195 0.2799 0.0925

3 141.3155 1.0685 0.2671 0.08834 135.9999 1.0284 0.2571 0.085

H+ 0.0108966

1 167.9499 1.2699 0.3175 0.105

2 147.8977 1.1183 0.2796 0.0924

3 141.2137 1.0678 0.2669 0.0883

4 135.9207 1.0278 0.2569 0.085

He 0.0112141

1 167.3053 1.2651 0.3163 0.1046

2 147.5697 1.1158 0.279 0.0922

3 140.9875 1.0661 0.2665 0.0881

4 135.751 1.0265 0.2566 0.0848

O/e; 0.01116331 167.4071 1.2658 0.3165 0.10462 147.6263 1.1163 0.2791 0.0923

3 141.0214 1.0663 0.2666 0.0881

4 135.785 1.0267 0.2567 0.0849

P++ee 0.0116077

1 166.5249 1.2592 0.3148 0.1041

2 147.1852 1.1129 0.2782 0.092

3 140.7273 1.0641 0.266 0.088

4 135.5588 1.025 0.2563 0.0847

&Cont"nuac"6n(

D<e 0.0117729

1 166.2082 1.2568 0.3142 0.1039

2 147.0156 1.1116 0.2779 0.0919

3 140.6256 1.0633 0.2658 0.0879

4 135.4796 1.0244 0.2561 0.0847

R 0.0124079

1 165.0207 1.2478 0.3119 0.1031

2 146.4275 1.1072 0.2768 0.0915

3 140.2297 1.0603 0.2651 0.0876

4 135.1856 1.0222 0.2555 0.0845

G:e+ 0.012573

1 164.7153 1.2455 0.3114 0.1029

2 146.2804 1.1061 0.2765 0.0914

3 140.1279 1.0596 0.2649 0.08764 135.1064 1.0216 0.2554 0.0844

D+e 0.0140716

1 162.1706 1.2262 0.3066 0.1014

2 145.0024 1.0964 0.2741 0.0906

3 139.2797 1.0532 0.2633 0.087

4 134.473 1.0168 0.2542 0.084

Te 0.0135001

1 163.1094 1.2333 0.3083 0.1019

2 145.4661 1.0999 0.275 0.0909

3 139.5964 1.0555 0.2639 0.0872

4 134.6992 1.0185 0.2546 0.0842

R+ 0.01479551 161.0397 1.2177 0.3044 0.10062 144.4369 1.0922 0.273 0.0903

3 138.9065 1.0503 0.2626 0.0868

4 134.1903 1.0147 0.2537 0.0839

C++ 0.0151892

1 160.4403 1.2132 0.3033 0.1003

2 144.1429 1.0899 0.2725 0.0901

3 138.7029 1.0488 0.2622 0.0867

4 134.0433 1.0136 0.2534 0.0838

O+ 0.0154051

1 160.1236 1.2108 0.3027 0.1001

2 143.9732 1.0886 0.2722 0.09

3 138.6011 1.048 0.262 0.0866

4 133.9528 1.0129 0.2532 0.0837

&Cont"nuac"6n(

#=e>+; 0.0159893

1 159.2754 1.2044 0.3011 0.0995

2 143.5548 1.0855 0.2714 0.0897

3 138.3184 1.0459 0.2615 0.0864

4 133.7492 1.0113 0.2528 0.0836

$ 0.0164211

1 158.6759 1.1998 0.3 0.0992

2 143.2607 1.0833 0.2708 0.0895

3 138.1148 1.0443 0.2611 0.08634 133.6022 1.0102 0.2526 0.0835

#e 0.0170815

1 157.7825 1.1931 0.2983 0.0986

2 142.8083 1.0798 0.27 0.0893

3 137.8207 1.0421 0.2605 0.0861

4 133.376 1.0085 0.2521 0.0834

Pe++ 0.0175514

1 157.1717 1.1884 0.2971 0.0982

2 142.503 1.0775 0.2694 0.0891

3 137.6172 1.0406 0.2601 0.086

4 133.2177 1.0073 0.2518 0.0833

#: 0.01812291 156.4479 1.183 0.2957 0.09782 142.1411 1.0748 0.2687 0.0888

3 137.3683 1.0387 0.2597 0.0859

4 133.0367 1.0059 0.2515 0.0831

P<e 0.0186055

1 155.8485 1.1784 0.2946 0.0974

2 141.847 1.0726 0.2681 0.0887

3 137.1761 1.0372 0.2593 0.0857

4 132.8897 1.0048 0.2512 0.0831

!+/ 0.0190754 1 155.283 1.1742 0.2935 0.0971

2 141.5643 1.0704 0.2676 0.0885

3 136.9838 1.0358 0.2589 0.0856

4 132.754 1.0038 0.251 0.083

$+ 0.0196215

1 154.6497 1.1694 0.2923 0.0967

2 141.2476 1.068 0.267 0.0883

3 136.7689 1.0342 0.2585 0.0855

4 132.5956 1.0026 0.2507 0.0829

&Cont"nuac"6n(

#=e: 0.0223774

1 151.6752 1.1469 0.2867 0.0948

2 139.7547 1.0567 0.2642 0.0873

3 135.785 1.0267 0.2567 0.08494 131.8492 0.997 0.2492 0.0824

Ta-#a de reactanc"a "nduct"$a en o7s y !u !ara una #5nea de 8;; 4

O$D#CTO% %&DIO(m) $ XC ' 10 3

(*)XCP#+115 '10

XCP#+230 '10

XCP#+400 '

+, 0.0077343

1 1.1949 9.0348 2.2587 0.7468

2 1.0526 7.9592 1.9898 0.6579

3 0.9935 7.5121 1.878 0.62094 0.9611 7.2671 1.8168 0.6007

/+e 0.0081534

1 1.1949 9.0348 2.2587 0.7468

2 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9611 7.2671 1.8168 0.6007

0.008636

1 1.1789 8.9143 2.2286 0.7368

2 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9507 7.189 1.7972 0.5942

e 0.00868681 1.1789 8.9143 2.2286 0.73682 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9507 7.189 1.7972 0.5942

!e 0.0091567

1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9935 7.5121 1.878 0.6209

4 0.9507 7.189 1.7972 0.5942

Oe 0.0094107

1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942C+ee 0.0094361 1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10 XCP#+400 '

I:+ 0.0099441

1 1.1483 8.6828 2.1707 0.7177

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

Pe+ 0.0103378

1 1.1483 8.6828 2.1707 0.7177

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

$e 0.0107442

1 1.1483 8.6828 2.1707 0.7177

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

H+ 0.0108966

1 1.1483 8.6828 2.1707 0.7177

2 1.0163 7.6848 1.9212 0.63523 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

He 0.0112141

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

O/e; 0.0111633

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

P++ee 0.0116077

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

D<e 0.0117729

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.63523 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10

XCP#+400 '

R 0.0124079

1 1.1192 8.463 2.1157 0.6995

2 1.0048 7.5975 1.8994 0.628

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

G:e+ 0.012573

1 1.1192 8.463 2.1157 0.6995

2 1.0048 7.5975 1.8994 0.628

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

D+e 0.0140716

1 1.1052 8.3572 2.0893 0.6908

2 1.0048 7.5975 1.8994 0.6283 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

Te 0.0135001

1 1.1052 8.3572 2.0893 0.6908

2 1.0048 7.5975 1.8994 0.628

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

R+ 0.0147955

1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817C++ 0.0151892 1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.62093 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

O+ 0.0154051

1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.62093 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

#=e>+; 0.0159893

1 1.0783 8.1534 2.0383 0.6739

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10 XCP#+400 '

$ 0.0164211

1 1.0783 8.1534 2.0383 0.6739

2 0.9824 7.4286 1.8572 0.614

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

#e 0.0170815

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.59424 0.9307 7.0376 1.7594 0.5817

Pe++ 0.0175514

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.9307 7.0376 1.7594 0.5817

#: 0.0181229

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

P<e 0.0186055

1 1.0526 7.9592 1.9898 0.65792 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

!+/ 0.0190754

1 1.0526 7.9592 1.9898 0.6579

2 0.9716 7.347 1.8367 0.6073

3 0.9507 7.189 1.7972 0.59424 0.921 6.9643 1.7411 0.5756

$+ 0.0196215

1 1.0526 7.9592 1.9898 0.6579

2 0.9716 7.347 1.8367 0.6073

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

#=e: 0.0223774

1 1.0281 7.7741 1.9435 0.6426

2 0.9611 7.2671 1.8168 0.6007

3 0.9406 7.1125 1.7781 0.5879

4 0.921 6.9643 1.7411 0.5756

8% Rea#"ce un co!end"o de #os resu#tados o-ten"dos !or sus otrosco!a@eros) ,u"enes tra-aaron con otro t"!o de torres% Or.an"ce d"c7osresu#tados y !resBnte#os en una ta-#a con e# *"n de o-ser$ar y co!arar c#araente #os $a#ores de "nductanc"a y ca!ac"tanc"a) as5 coo #os $a#oresde #a reactanc"a "nduct"$a y ca!ac"t"$a de #as #5neas de trans"s"6n cond"st"ntas torres) d"st"ntos conductores y d"st"ntas con*".urac"ones deconductores arados%

Ta-#a de "nductanc"a y ca!ac"tanc"a en torre reten"da !ara :;; 4<

CO$D#CTO

%&DIO(m

L(m/!M

L (/m)

( F/km)

C (F/m) '10

+, 0.007734

1 1.5536 1.5536 0.0074 0.0074

2 1.342 1.342 0.0084 0.0084

3 1.2714 1.2714 0.0089 0.0089

4 1.2189 1.2189 0.0092 0.0092

/+e 0.008153

1 1.543 1.543 0.0074 0.0074

2 1.3367 1.3367 0.0085 0.0085

3 1.2679 1.2679 0.0089 0.0089

4 1.2163 1.2163 0.0092 0.0092

0.008636

1 1.5315 1.5315 0.0075 0.00752 1.3309 1.3309 0.0085 0.0085

3 1.2641 1.2641 0.0089 0.0089

4 1.2134 1.2134 0.0093 0.0093

e 0.008686

81 1.5304 1.5304 0.0075 0.0075

2 1.3303 1.3303 0.0085 0.0085

3 1.2637 1.2637 0.0089 0.0089

4 1.213 1.213 0.0093 0.0093

!e 0.009156

1 1.5198 1.5198 0.0076 0.00762 1.3251 1.3251 0.0086 0.0086

3 1.2602 1.2602 0.0089 0.0089

4 1.2105 1.2105 0.0093 0.0093

Oe 0.009410

1 1.5144 1.5144 0.0076 0.0076

2 1.3223 1.3223 0.0086 0.0086

3 1.2583 1.2583 0.009 0.009

4 1.209 1.209 0.0093 0.0093

C+ee 0.009436

1 1.5138 1.5138 0.0076 0.0076

2 1.3221 1.3221 0.0086 0.0086

3 1.2581 1.2581 0.009 0.0094 1.209 1.209 0.0093 0.0093

I:+ 0.009944

1 1.5033 1.5033 0.0077 0.0077

2 1.3168 1.3168 0.0086 0.0086

3 1.2547 1.2547 0.009 0.009

4 1.2063 1.2063 0.0093 0.0093

&Cont"nuac"6n(

CO$D#CTO

%&DIO(m

(m/!M)

L (/m)

( F/km)

C (F/m) '10

Pe+ 0.010337

1 1.4956 1.4956 0.0077 0.0077

2 1.3129 1.3129 0.0086 0.0086

3 1.2521 1.2521 0.009 0.009

4 1.2044 1.2044 0.0093 0.0093

$e 0.010744

1 1.4878 1.4878 0.0077 0.0077

2 1.3091 1.3091 0.0087 0.0087

3 1.2495 1.2495 0.009 0.009

4 1.2025 1.2025 0.0093 0.0093

H+ 0.010896

1 1.485 1.485 0.0077 0.0077

2 1.3077 1.3077 0.0087 0.0087

3 1.2486 1.2486 0.009 0.009

4 1.2018 1.2018 0.0094 0.0094He 0.011214 1 1.4793 1.4793 0.0078 0.0078

2 1.3048 1.3048 0.0087 0.0087

3 1.2466 1.2466 0.009 0.009

4 1.2003 1.2003 0.0094 0.0094

O/e; 0.011163

1 1.4802 1.4802 0.0078 0.0078

2 1.3053 1.3053 0.0087 0.0087

3 1.2469 1.2469 0.009 0.009

4 1.2006 1.2006 0.0094 0.0094

P++ee 0.011607

1 1.4724 1.4724 0.0078 0.0078

2 1.3014 1.3014 0.0087 0.0087

3 1.2443 1.2443 0.0091 0.0091

4 1.1986 1.1986 0.0094 0.0094

D<e 0.0117729

1 1.4696 1.4696 0.0078 0.0078

2 1.2999 1.2999 0.0087 0.00873 1.2434 1.2434 0.0091 0.0091

4 1.1979 1.1979 0.0094 0.0094

R 0.012407

1 1.4591 1.4591 0.0079 0.0079

2 1.2947 1.2947 0.0088 0.0088

3 1.2399 1.2399 0.0091 0.0091

4 1.1953 1.1953 0.0094 0.0094

?C=+@)

CO$D#CTO%

%&DIO(m) $

L(m/!M

L (/m)'10

C( F/km)

C (F/m) '1012 1

G:e+ 0.012573

1 1.4564 1.4564 0.0079 0.0079

2 1.2934 1.2934 0.0088 0.00883 1.239 1.239 0.0091 0.0091

4 1.1946 1.1946 0.0094 0.0094D+e 0.014071 1 1.4339 1.4339 0.008 0.008

2 1.2821 1.2821 0.0088 0.0088

3 1.2315 1.2315 0.0092 0.0092

4 1.189 1.189 0.0095 0.0095

Te 0.013500

1 1.4422 1.4422 0.008 0.008

2 1.2862 1.2862 0.0088 0.0088

3 1.2343 1.2343 0.0091 0.0091

4 1.191 1.191 0.0094 0.0094

R+ 0.014795

1 1.4239 1.4239 0.0081 0.0081

2 1.2771 1.2771 0.0089 0.0089

3 1.2282 1.2282 0.0092 0.0092

4 1.1865 1.1865 0.0095 0.0095

C++ 0.0151892

1 1.4186 1.4186 0.0081 0.0081

2 1.2745 1.2745 0.0089 0.00893 1.2264 1.2264 0.0092 0.0092

4 1.1852 1.1852 0.0095 0.0095

O+ 0.015405

1 1.4158 1.4158 0.0081 0.0081

2 1.273 1.273 0.0089 0.0089

3 1.2255 1.2255 0.0092 0.0092

4 1.1844 1.1844 0.0095 0.0095

#=e>+; 0.015989

1 1.4083 1.4083 0.0082 0.0082

2 1.2693 1.2693 0.0089 0.0089

3 1.223 1.223 0.0092 0.0092

4 1.1826 1.1826 0.0095 0.0095

$ 0.016421

1 1.403 1.403 0.0082 0.0082

2 1.2667 1.2667 0.009 0.009

3 1.2212 1.2212 0.0092 0.0092

4 1.1813 1.1813 0.0095 0.0095

&Cont"nuac"6n(

CO$D#CTO %&DIO(m $ L L (/m) C C (F/m) '10

% ) (m/!M)

'10 ( F/km) 12 1

#e 0.017081

1 1.3951 1.3951 0.0083 0.0083

2 1.2627 1.2627 0.009 0.009

3 1.2186 1.2186 0.0093 0.0093

4 1.1793 1.1793 0.0095 0.0095

Pe++ 0.017551

1 1.3897 1.3897 0.0083 0.0083

2 1.26 1.26 0.009 0.009

3 1.2168 1.2168 0.0093 0.0093

4 1.1779 1.1779 0.0095 0.0095

#: 0.018122

1 1.3833 1.3833 0.0083 0.0083

2 1.2568 1.2568 0.009 0.009

3 1.2146 1.2146 0.0093 0.0093

4 1.1763 1.1763 0.0096 0.0096

P<e 0.018605

1 1.378 1.378 0.0084 0.0084

2 1.2542 1.2542 0.009 0.009

3 1.2129 1.2129 0.0093 0.0093

4 1.175 1.175 0.0096 0.0096

!+/ 0.019075

1 1.373 1.373 0.0084 0.0084

2 1.2517 1.2517 0.0091 0.0091

3 1.2112 1.2112 0.0093 0.0093

4 1.1738 1.1738 0.0096 0.0096

$+ 0.0196215

1 1.3674 1.3674 0.0084 0.0084

2 1.2489 1.2489 0.0091 0.00913 1.2093 1.2093 0.0093 0.0093

4 1.1724 1.1724 0.0096 0.0096

#=e: 0.022377

1 1.3411 1.3411 0.0086 0.0086

2 1.2357 1.2357 0.0092 0.0092

3 1.2006 1.2006 0.0094 0.0094

4 1.1658 1.1658 0.0096 0.0096

Ta-#a de reactanc"a "nduct"$a en o7s y !u !ara una #5nea de8;; 4

CO$D#CTO%

%&DIO(m)

$ XL (*) XLP#+1

15XLP#+23

0XLP#+4

W+, 0.0077

1 175.70

84 1.3286 0.3322 0.1098

2151.77

7 1.1477 0.2869 0.0949

3143.79

23 1.0873 0.2718 0.0899

4137.85

47 1.0424 0.2606 0.0862

P+e 0.0081

1174.50

96 1.3195 0.3299 0.1091

2151.17

76 1.1431 0.2858 0.0945

3143.39

64 1.0843 0.2711 0.0896

4137.56

06 1.0402 0.26 0.086

O 0.0086

1173.20

9 1.3097 0.3274 0.1083

2150.52

16 1.1382 0.2845 0.0941

3142.96

67 1.081 0.2703 0.0894

4137.23

26 1.0377 0.2594 0.0858e 0.0086

173.08

46 1.3088 0.3272 0.1082

2150.45

37 1.1376 0.2844 0.0943 142.92

141.0807 0.2702 0.0893

4137.18

74 1.0373 0.2593 0.0857

!e 0.0091

1171.88

57 1.2997 0.3249 0.1074

2149.86

56 1.1332 0.2833 0.0937

3142.52

56 1.0777 0.2694 0.0891

4136.90

46 1.0352 0.2588 0.0856

Oe 0.0094

1171.27

5 1.2951 0.3238 0.107

2149.54

9 1.1308 0.2827 0.0935

3 142.3107 1.0761 0.269 0.0889

4136.73

5 1.0339 0.2585 0.0855

&Cont"nuac"6n(

C+ee 0.0094361

1 171.2071 1.2946 0.3236 0.107

2 149.5263 1.1306 0.2827 0.0935

3 142.2881 1.0759 0.269 0.08894 136.735 1.0339 0.2585 0.0855

I:+ 0.0099441 1 170.0196 1.2856 0.3214 0.10632 148.9269 1.1261 0.2815 0.0931

3 141.9036 1.073 0.2682 0.0887

4 136.4296 1.0316 0.2579 0.0853

Pe+ 0.01033781 169.1488 1.279 0.3198 0.10572 148.4858 1.1228 0.2807 0.0928

3 141.6095 1.0708 0.2677 0.0885

4 136.2147 1.03 0.2575 0.0851

$e 0.0107442

1 168.2666 1.2723 0.3181 0.1052

2 148.0561 1.1195 0.2799 0.0925

3 141.3155 1.0685 0.2671 0.0883

4 135.9999 1.0284 0.2571 0.085

H+ 0.0108966

1 167.9499 1.2699 0.3175 0.105

2 147.8977 1.1183 0.2796 0.0924

3 141.2137 1.0678 0.2669 0.08834 135.9207 1.0278 0.2569 0.085

He 0.0112141

1 167.3053 1.2651 0.3163 0.1046

2 147.5697 1.1158 0.279 0.0922

3 140.9875 1.0661 0.2665 0.0881

4 135.751 1.0265 0.2566 0.0848

O/e; 0.0111633

1 167.4071 1.2658 0.3165 0.1046

2 147.6263 1.1163 0.2791 0.0923

3 141.0214 1.0663 0.2666 0.0881

4 135.785 1.0267 0.2567 0.0849

P++ee 0.0116077

1 166.5249 1.2592 0.3148 0.1041

2 147.1852 1.1129 0.2782 0.092

3 140.7273 1.0641 0.266 0.088

4 135.5588 1.025 0.2563 0.0847

&Cont"nuac"6n(

D<e 0.0117729 1 166.2082 1.2568 0.3142 0.10392 147.0156 1.1116 0.2779 0.0919

3 140.6256 1.0633 0.2658 0.0879

4 135.4796 1.0244 0.2561 0.0847

R 0.01240791 165.0207 1.2478 0.3119 0.10312 146.4275 1.1072 0.2768 0.0915

3 140.2297 1.0603 0.2651 0.0876

4 135.1856 1.0222 0.2555 0.0845

G:e+ 0.012573

1 164.7153 1.2455 0.3114 0.1029

2 146.2804 1.1061 0.2765 0.0914

3 140.1279 1.0596 0.2649 0.0876

4 135.1064 1.0216 0.2554 0.0844

D+e 0.0140716

1 162.1706 1.2262 0.3066 0.1014

2 145.0024 1.0964 0.2741 0.0906

3 139.2797 1.0532 0.2633 0.0874 134.473 1.0168 0.2542 0.084

Te 0.0135001

1 163.1094 1.2333 0.3083 0.1019

2 145.4661 1.0999 0.275 0.0909

3 139.5964 1.0555 0.2639 0.0872

4 134.6992 1.0185 0.2546 0.0842

R+ 0.0147955

1 161.0397 1.2177 0.3044 0.1006

2 144.4369 1.0922 0.273 0.0903

3 138.9065 1.0503 0.2626 0.0868

4 134.1903 1.0147 0.2537 0.0839

C++ 0.0151892

1 160.4403 1.2132 0.3033 0.1003

2 144.1429 1.0899 0.2725 0.0901

3 138.7029 1.0488 0.2622 0.0867

4 134.0433 1.0136 0.2534 0.0838

O+ 0.0154051

1 160.1236 1.2108 0.3027 0.1001

2 143.9732 1.0886 0.2722 0.09

3 138.6011 1.048 0.262 0.0866

4 133.9528 1.0129 0.2532 0.0837

&Cont"nuac"6n(

#=e>+; 0.0159893

1 159.2754 1.2044 0.3011 0.0995

2 143.5548 1.0855 0.2714 0.0897

3 138.3184 1.0459 0.2615 0.0864

4 133.7492 1.0113 0.2528 0.0836

$ 0.0164211

1 158.6759 1.1998 0.3 0.0992

2 143.2607 1.0833 0.2708 0.0895

3 138.1148 1.0443 0.2611 0.0863

4 133.6022 1.0102 0.2526 0.0835

#e 0.0170815

1 157.7825 1.1931 0.2983 0.09862 142.8083 1.0798 0.27 0.0893

3 137.8207 1.0421 0.2605 0.0861

4 133.376 1.0085 0.2521 0.0834

Pe++ 0.0175514

1 157.1717 1.1884 0.2971 0.0982

2 142.503 1.0775 0.2694 0.0891

3 137.6172 1.0406 0.2601 0.086

4 133.2177 1.0073 0.2518 0.0833

#: 0.0181229

1 156.4479 1.183 0.2957 0.0978

2 142.1411 1.0748 0.2687 0.0888

3 137.3683 1.0387 0.2597 0.08594 133.0367 1.0059 0.2515 0.0831

P<e 0.0186055

1 155.8485 1.1784 0.2946 0.0974

2 141.847 1.0726 0.2681 0.0887

3 137.1761 1.0372 0.2593 0.0857

4 132.8897 1.0048 0.2512 0.0831

!+/ 0.0190754

1 155.283 1.1742 0.2935 0.0971

2 141.5643 1.0704 0.2676 0.0885

3 136.9838 1.0358 0.2589 0.08564 132.754 1.0038 0.251 0.083

$+ 0.0196215

1 154.6497 1.1694 0.2923 0.0967

2 141.2476 1.068 0.267 0.0883

3 136.7689 1.0342 0.2585 0.0855

4 132.5956 1.0026 0.2507 0.0829

&Cont"nuac"6n(

#=e: 0.0223774

1 151.6752 1.1469 0.2867 0.0948

2 139.7547 1.0567 0.2642 0.0873

3 135.785 1.0267 0.2567 0.0849

4 131.8492 0.997 0.2492 0.0824

Ta-#a de reactanc"a "nduct"$a en o7s y !u !ara una #5nea de8;; 4

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10 XCP#+400 '

+, 0.0077343 1 1.1949 9.0348 2.2587 0.7468

2 1.0526 7.9592 1.9898 0.6579

3 0.9935 7.5121 1.878 0.62094 0.9611 7.2671 1.8168 0.6007

/+e 0.0081534 1 1.1949 9.0348 2.2587 0.7468

2 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9611 7.2671 1.8168 0.6007

0.0086361 1.1789 8.9143 2.2286 0.73682 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9507 7.189 1.7972 0.5942

e 0.0086868

1 1.1789 8.9143 2.2286 0.7368

2 1.0402 7.8656 1.9664 0.6501

3 0.9935 7.5121 1.878 0.6209

4 0.9507 7.189 1.7972 0.5942

!e 0.0091567

1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9935 7.5121 1.878 0.62094 0.9507 7.189 1.7972 0.5942

Oe 0.0094107

1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

C+ee 0.0094361

1 1.1634 8.7971 2.1993 0.7271

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10 XCP#+400 '

I:+ 0.0099441

1 1.1483 8.6828 2.1707 0.7177

2 1.0281 7.7741 1.9435 0.6426

3 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942Pe+ 0.0103378 1 1.1483 8.6828 2.1707 0.7177

2 1.0281 7.7741 1.9435 0.64263 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

$e 0.0107442

1 1.1483 8.6828 2.1707 0.7177

2 1.0163 7.6848 1.9212 0.63523 0.9824 7.4286 1.8572 0.614

4 0.9507 7.189 1.7972 0.5942

H+ 0.0108966

1 1.1483 8.6828 2.1707 0.7177

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

He 0.0112141

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

O/e; 0.0111633

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9824 7.4286 1.8572 0.614

4 0.9406 7.1125 1.7781 0.5879

P++ee 0.0116077

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

D<e 0.0117729

1 1.1336 8.5715 2.1429 0.7085

2 1.0163 7.6848 1.9212 0.6352

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10 XCP#+400 '

R 0.0124079 1 1.1192 8.463 2.1157 0.6995

2 1.0048 7.5975 1.8994 0.6283 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

G:e+ 0.012573

1 1.1192 8.463 2.1157 0.6995

2 1.0048 7.5975 1.8994 0.6283 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

D+e 0.0140716

1 1.1052 8.3572 2.0893 0.6908

2 1.0048 7.5975 1.8994 0.628

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

Te 0.0135001

1 1.1052 8.3572 2.0893 0.6908

2 1.0048 7.5975 1.8994 0.628

3 0.9716 7.347 1.8367 0.6073

4 0.9406 7.1125 1.7781 0.5879

R+ 0.0147955

1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

C++ 0.0151892

1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

O+ 0.0154051

1 1.0916 8.254 2.0635 0.6822

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

#=e>+; 0.0159893

1 1.0783 8.1534 2.0383 0.6739

2 0.9935 7.5121 1.878 0.6209

3 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

&Cont"nuac"6n(

O$D#CTO% %&DIO(m) $ XC ' 10 3(*)

XCP#+115 '10

XCP#+230 '10

XCP#+400 '

$ 0.0164211

1 1.0783 8.1534 2.0383 0.6739

2 0.9824 7.4286 1.8572 0.6143 0.9611 7.2671 1.8168 0.6007

4 0.9307 7.0376 1.7594 0.5817

#e 0.0170815

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.9307 7.0376 1.7594 0.5817

Pe++ 0.0175514

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.9307 7.0376 1.7594 0.5817

#: 0.0181229

1 1.0653 8.0551 2.0138 0.6658

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

P<e 0.0186055

1 1.0526 7.9592 1.9898 0.6579

2 0.9824 7.4286 1.8572 0.614

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

!+/ 0.0190754

1 1.0526 7.9592 1.9898 0.6579

2 0.9716 7.347 1.8367 0.6073

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

$+ 0.0196215

1 1.0526 7.9592 1.9898 0.6579

2 0.9716 7.347 1.8367 0.6073

3 0.9507 7.189 1.7972 0.5942

4 0.921 6.9643 1.7411 0.5756

#=e: 0.0223774

1 1.0281 7.7741 1.9435 0.6426

2 0.9611 7.2671 1.8168 0.6007

3 0.9406 7.1125 1.7781 0.5879

4 0.921 6.9643 1.7411 0.5756

:% Escr"-a EN FORA CLARA) OETI<A > CO2ERENTE sus conc#us"onesso-re #os resu#tados o-ten"dos en #os eerc"c"os anter"ores%

De #as ta-#as .eneradas con #os datos de #a torre reten"da !ara :;;4<) se !uedeconc#u"r ,ue entre ás .rande sea e# rad"o de# conductor) enor será #a

"nductanc"a) #a "nductanc"a ta-"Bn d"s"nuye s" se auenta e# nero deconductores !or *ase) !or #o tanto s" #a "nductanc"a d"s"nuye de ".ua# anera #o7ará #a reactanc"a "nduct"$a &L() ya ,ue #a "nductanc"a es d"rectaente!ro!orc"ona# a #a reactanc"a L coo #o d"ce #a *oru#a LHL% En e# caso de #aca!ac"tanc"a) esta d"s"nuye con e# auento de# rad"o y nero de conductores)#o cua# !ro$oca ,ue #a reactanc"a ca!ac"t"$a &C( d"s"nuya) !or,ue #aca!ac"tanc"a es "n$ersaente !ro!orc"ona# a #a reactanc"a C se.n #a *oru#aC13HC% En #a reactanc"a "nduct"$a en PUs &LPU( y reactanc"a ca!ac"t"$a enPUs &CPU( !asa #o "so) ya ,ue a# d"s"nu"r L y C ta-"Bn #o 7acen LPUy CPU ta# coo #o "nd"can #as *oru#as LPU L3 y cPU c3% De #as

ta-#as ta-"Bn se !uede o-ser$ar ,ue a# auentar e# $o#tae en #a torre &11=4<)98;4< y :;;4<() #as cant"dades o !aráetros L) LPU) C y CPU d"s"nuyenesto de-"do a ,ue <L

93SL y PU3%

ITESI&INSTITUTO TECNOLÓGICO SUPERIOR DE IRAPUATO(

EAEN SEGUNDO PARCIAL0

• CJLCULO DE PARJETROS DE LKNEA DE TRANSISIÓN DE UNATORRE AUTOSOPORTADA DE :;; 4<%

ALUNOS0

• ROGELIO ACE<EDO ARANDA• ERNESTO ISAEL ARUEM LARA

CARRERA0 ING% ELECTROECJNICA%

ATERIA0 SISTEAS ELCTRICOS DE POTENCIA%

AESTRO0 %C%OSE IGUEL GARCIA GUMAN%

Con!n"#o

1- I$T%OD#CCI.$-------------------------------------------------------------------------------------3

2- P%OCEDIMIE$TO-----------------------------------------------------------------------------------4

3- %E"#LT&DO" DI"C#"IO$E"-----------------------------------------------------------------,

4- CO$CL#"IO$E"-----------------------------------------------------------------------------------10

1. In$o#%&&"'n

La e#ectr"c"dad) con e# !aso de# t"e!o y reontando 7oy en d5a se 7a con$ert"doen una !arte *undaenta# e "!ortante en #a $"da cot"d"ana) !or #o cua# a-arca yt"ene una etensa a!#"cac"6n% Por #o cua# 7oy en d5a #a soc"edad re,u"ere de esteser$"c"o !ara so#$entar sus neces"dades !r"ar"as%

Para trans!ortar #a ener.5a e#Bctr"ca desde #as .randes *uentes de .enerac"6n)"!#"ca un .ran reto ya ,ue se re,u"eren de .randes $ar"a-#es) !ara entre.ar una-uena ca#"dad de ener.5a) entre estas $ar"a-#es se encuentran #as estructuras de.randes a.n"tudes coo #o son su-estac"ones) estac"ones e#Bctr"cas) torres detrans"s"6n y !ostes en #a d"str"-uc"6n%

Adeás) #as #5neas de trans"s"6n son $"s"-#eente a,ue##as estructuras etá#"cascon conductores co#.antes ,ue se et"enden a $ar"as decenas o c"entos de"#6etros de #on."tud cu!#"endo #a *"na#"dad de trans!ortar .randes cant"dades

de ener.5a e#Bctr"ca desde de #os centros de .enerac"6n a #os d"*erentes centrosde consuo ,ue "nte.ran #a red de# s"stea e#Bctr"co%

(. P$o&!#")"!no

E# uso de so*tQare 7oy en d5a) son de .ran ayuda) adeás de ser e*"ca7erra"enta con #a cua# se !er"te crear y s"u#ar en t"e!o rea# s"steas) cooen e# !resente tra-ao se ut"#"a e# so*tQare de ATLA coo 7erra"enta decá#cu#o de #os !aráetros e#Bctr"cos de #as #5neas de trans"s"6n%

S"endo e# o-et"$o de #a enc"onada !ro.raac"6n) F".ura 1) se o-tendránresu#tados nuBr"cos de #os !aráetros de #a #5nea de trans"s"6n y sus$ar"ac"ones con*ore se "ncreentan e# nero de conductores !or *ase) adeásde #as !ro!"edades de# conductor de t"!o ACSR &Conductor de a#u"n"o con a#ade acero( cons"derado%

Pr"nc"!a#ente) se rea#"6 e# aná#"s"s te6r"co so-re e# cá#cu#o de #os !aráetros de#as #5neas de trans"s"6n de !otenc"a) #os cua#es *ueron o-ten"dos en c#ase) !ara

!oster"orente !#asar estos conoc""entos en #a !ro.raac"6n) #a cua# *uerea#"ada en e# so*tQare de ATLA) #a cua# *ue de .ran ayuda) !ara s"!#"*"car ya."#"ar #os !aráetros deter"nados%

En e# actua# tra-ao se !resentan cuatro ta-#as) cons"derando desde uno 7astacuatro conductores !or *ase res!ect"$aente y #as caracter5st"cas de conductoresde t"!o ACSR) !ara de esta *ora deter"nar #os !aráetros) ta#es coo)"nductanc"a) ca!ac"tanc"a) reactanc"as "nduct"$as y ca!ac"t"$as) y en s"stea !or un"dad) toando en cons"derac"6n #os $o#taes ut"#"ados a,u5 en B"co) ,ue son)11= 4<) 98; 4< y :;; 4<%

Adeás) !ara !oster"orente dar conc#us"ones so-re #os resu#tados o-ten"dos deeste aná#"s"s donde se cons"der6 una estructura) ,ue es una torre autoso!ortadade :;; 4<%

F".ura 1% Eaen se.undo !arc"a#%

*. R!+%,-#o+ #"+&%+"on!+

Se cons"der6 #a s".u"ente torre de trans"s"6n) F".ura 9% Ten"endo desde 1 a :conductores !or *ase) !ara #os cá#cu#os rea#"ados ed"ante #a !ro.raac"6n enATLA%

F".ura 9% Torre de trans"s"6n autoso!ortada de :;; 4<% A cont"nuac"6n se uestra #a!r"era ta-#a) F".ura 8) con #os datos o-ten"dos de ATLA) cons"derando un

conductor !or *ase%

F".ura 8% Cá#cu#os o-ten"dos de 1 conductor !or *ase%

Poster"orente se uestra #a ta-#a) cons"derando 9 conductores !or *ase) F".ura:%

F".ura :% Cá#cu#os o-ten"dos de 9 conductores !or *ase%

Ta-#a de datos o-ten"dos) cons"derando 8 conductores !or *ase) F".ura =%

F".ura =% Cá#cu#os o-ten"dos de 8 conductores !or *ase%

Ta-#a de datos o-ten"dos) cons"derando : conductores !or *ase) F".ura ?%

F".ura ?% Cá#cu#os o-ten"dos de : conductores !or *ase%

/. Con&,%+"on!+.

asando e# estud"o so-re #as #5neas de trans"s"6n aBreas #as cua#es s"r$en !ara#a trans*erenc"a de !otenc"a e#Bctr"ca !or ed"o de sus conductores y adeás)!ueden ad,u"r"r d"*erentes arre.#os entre sus conductores% Por #o cua#) #os ásusados en #a !ráct"ca son) #os de dos) tres y 7asta cuatro conductores !or *ase) #ocua# a !art"r y e "nde!end"enteente de estos arre.#os coo de #a estructura ,ue#os so!orta &torres de trans"s"6n() se desarro##an #os cá#cu#os necesar"os) ta#escoo) rad"os y d"stanc"as ed"as .eoBtr"cas) !ara !oster"orente ca#cu#ar #os

!aráetros de #as #5neas de trans"s"6n &Inductanc"a) ca!ac"tanc"a) res"stenc"a()#os cua#es son "!ortantes !ara o-tener su ode#o en e# S"stea E#Bctr"co dePotenc"a &SEP(%

De #os datos o-ten"dos en ta-#as anter"ores) !odeos conc#u"r #o s".u"ente0 secons"deraron 81 t"!os de conductores de t"!o ACSR &Conductor de a#u"n"o cona#a de acero() ten"endo cada uno de estos sus caracter5st"cas y !ro!"edades"nd"$"dua#es cons"derando y deter"nando !ara cada uno de estos conductores #os!aráetros ostrados en ta-#as) adeás) ca#cu#ando en s"stea de !or un"dad)so-re #os d"*erentes $o#taes usados en B"co &11= 4<) 98; 4< y :;; 4<(%

Ten"endo y cons"derando #o enc"onado anter"orente) !odeos o-ser$ar ,ue #os$a#ores de "nductanc"a y ca!ac"tanc"a $ar5an so#o !or e# $a#or de# GR &rad"oed"o .eoBtr"co() e# cua# de!ende de# rad"o de cada conductor% Donde !odeoso-ser$ar en cada ta-#a) 7ac"endo re*erenc"a res!ecto de cada conductor se!roduce una d"s"nuc"6n de #os $a#ores dados en s"stea !or un"dad) con*ore se"ncreenta e# $o#tae) es dec"r a ayor $o#tae se t"enen enores $a#ores de PU)s"endo y anten"endo esto en todas #as ta-#as a# auentar #os conductores !or *ase) es dec"r entonces a ayor $o#tae se t"ene enores $a#ores de PU%

Adeás) !odeos o-ser$ar) a# rea#"ar #a co!arac"6n de #os !aráetros coo #oes #a "nductanc"a) cuando se "ncreenta e# nero de conductores !or *ase eneste !aráetro se !roduce una d"s"nuc"6n) y en e# caso de #a ca!ac"tanc"a a#"ncreentar e# nero de conductores !or *ase) se ##e$a a ca-o una e#e$ac"6n de

este !aráetro) sa-"endo ,ue) #a ca!ac"tanc"a se deter"na a !art"r de #a*orac"6n de ca!os e#Bctr"cos) #os cua#es son or"."nados !or #a car.a ,ue se

!roduce entre conductores y ,ue a su $e está re#ac"onada con #a tens"6n de#"so conductor) adeás) con*ore se "ncreente #a #on."tud de #a #5nea de

trans"s"6n) se $ue#$e uy "!ortante e# e*ecto ca!ac"t"$o ,ue se !roduce en e##a)ya ,ue ta# e*ecto ta-"Bn se "ncreenta) contr"-uyendo des*a$ora-#eente a #aca5da de tens"6n) e*"c"enc"a) *actor de !otenc"a y esta-"#"dad de# s"stea) #o cua# se!uede $er"*"car a# re$"sar #os datos de d"*erentes ta-#as) esto de-"do a #a .eoetr5a

de #os conductores) o -"en a# cá#cu#o de# GR) ,ue es e# cua# está $ar"ando)res!ecto a #os conductores cons"derados !or *ase%

Pero suced"endo #o contrar"o en #a co!arac"6n de #os s"steas !or un"dad &Pu()es dec"r) tanto !ara s"stea !or un"dad de "nductanc"a y ca!ac"tanc"a) se !roduceuna d"s"nuc"6n con*ore se $a "ncreentando e# nero de conductores de*ase) cons"derando !ara e##o #os "sos $o#taes) esto !or #a ra6n de ,ue en Pude #a "nductanc"a) e# $a#or de #a reactanc"a -ase !eranece constantede!end"endo de# $o#tae ut"#"ado) !ero tend"endo #a $ar"ac"6n d"recta de# $a#or de#a "nductanc"a) es dec"r s" con*ore se "ncreenta e# nero de conductores !or

*ase) esta d"s"nuye coo se enc"on6) !ues !or esta ra6n en s"stea !or un"dad se !roduce esta d"s"nuc"6n con*ore se "ncreentan #os conductores !or *ase%

Adeás) sa-"endo ,ue a# "ncreentar en nero de conductores !or *ase se"ncreenta e# rad"o e*ect"$o de# conductor y !or #o tanto se reduce #a "ntens"dad de#ca!o e#Bctr"co en #os conductores cercanos y de# "so conductor) !or #o cua#reduce a su $e #as !erd"das !or e*ecto corona &ru"do aud"-#e( e "nter*erenc"ae#ectroa.nBt"ca y reduce #a reactanc"a a# "ncreentar e# GR%

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