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Port (circuit theory)

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electrical analysis. If the algebraic sum of the currents is not zero, such as in example diagram (c), then the energy delivered from an external generator is not equal to the energy entering the pair of circuit poles. The energy transfer at that place is thus more complex than a simple flow from one subsystem to another and does not meet the generalised definition of a port.
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are not guided by electrical conductors. They are, instead guided by the walls of the waveguide. Thus, the concept of a circuit conductor pole does not exist in this format. Ports in waveguides consist of an aperture or break in the waveguide through which the electromagnetic waves can pass. The
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The concept of ports can be extended into other energy domains. The generalised definition of a port is a place where energy can flow from one element or subsystem to another element or subsystem. This generalised view of the port concept helps to explain why the port condition is so defined in
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It cannot be determined if a pair of nodes meets the port condition by analysing the internal properties of the circuit itself. The port condition is dependent entirely on the external connections of the circuit. What are ports under one set of external circumstances may well not be ports under
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The one-pole representation of a port will start to fail if there are significant ground plane loop currents. The assumption in the model is that the ground plane is perfectly conducting and that there is no potential difference between two locations on the ground plane. In reality, the ground
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and that current is sourced to or sunk into the ground plane that is equal and opposite to that going into the other pole of any port. In this topology a port is treated as being just a single pole. The corresponding balancing pole is imagined to be incorporated into the ground plane.
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In general, a circuit can consist of any number of ports—a multiport. Some, but not all, of the two-port parameter representations can be extended to arbitrary multiports. Of the voltage and current based matrices, the ones that can be extended are z-parameters and
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it is a two-port. For instance, a mechanical actuator has one port in the electrical domain and one port in the mechanical domain. Transducers can be analysed as two-port networks in the same way as electrical two-ports. That is, by means of a pair of
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plane is not perfectly conducting and loop currents in it will cause potential differences. If there is a potential difference between the commoned poles of two ports then the port condition is broken and the model is invalid.
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pair of poles meets the port condition. However, it is possible to deal with such a circuit by splitting one or more poles into a number of separate poles joined to the same node. If only one external
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terminal is connected to each pole (whether a split pole or otherwise) then the circuit can again be analysed in terms of ports. The most common arrangement of this type is to designate one pole of an
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to exist at the same time. In such cases, for each physical port, a separate port must be added to the analysis model for each of the modes present at that physical port.
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and current at its ports, so the internal makeup or design of the circuit need not be considered, or even known, in determining the circuit's response to applied signals.
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The port concept is particularly useful where multiple energy domains are involved in the same system and a unified, coherent analysis is required such as with
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the current flowing into one pole from outside the circuit is equal to the current flowing out of the other pole into the external circuit. Equivalently, the
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Linear two port networks have been widely studied and a large number of ways of representing them have been developed. One of these representations is the
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frequencies because voltages and currents are not convenient to measure in formats using conductors and are not relevant at all in
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Waveguides have an additional complication in port analysis in that it is possible (and sometimes desirable) for more than one
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if it is a physical object). The port condition is that a pair of poles of a circuit is considered a port
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In the most general case, it is possible to have a generator connected to every pair of poles, that is,
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has a port connecting it to an external circuit. The port meets the port condition because the current
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are connected to the pole pairs (1, 2) and (3, 4) then those two pairs are ports and the circuit is a
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Any node of a circuit that is available for connection to an external circuit is called a pole (or
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devices, but a port can no longer be defined in terms of circuit poles because in waveguides the
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are used at these frequencies and these too can be extended to an arbitrary number of ports.
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Electromagnetics, Microwave Circuit and Antenna Design for Communications Engineering
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of the currents flowing into the two poles from the external circuit must be zero.
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another. Consider the circuit of four resistors in the figure for example. If
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Simple resistive network with three possible port arrangements: (a) Pole pairs
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entering one terminal of the port is equal to the current exiting the other.
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bounded plane through which the wave passes is the definition of the port.
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Any two-pole circuit is guaranteed to meet the port condition by virtue of
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circuit topologies are commonly unbalanced circuit topologies such as
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RF and Microwave Engineering: Fundamentals of Wireless Communications
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and they are therefore one-ports unconditionally. All of the basic
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generators in all and the circuit has to be treated as a 6-port.
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that are ratios of one electrical and one mechanical variable.
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are studied since these are lossless and are commonly used in
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Point of entry and exit of electrical energy to/from a circuit
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Study of one-ports is an important part of the foundation of
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analysis. Connection between energy domains is by means of
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Russer, Chapter 10, "Microwave circuits: Linear multiports"
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Coaxial circulators. Circulators have at least three ports
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to an external circuit, as a point of entry or exit for
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Dean Karnopp, Donald L. Margolis, Ronald C. Rosenberg,
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flowing into the two nodes must be equal and opposite.
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Circuit blocks which have more than two ports include
459: 395: 352: 346: 521:are the voltages and currents respectively at port 74:The use of ports helps to reduce the complexity of 532:Common circuit blocks which are two-ports include 496: 184:It is even possible to arrange the inputs so that 948: 220:generators, then every pole must be split into 675:The idea of ports can be (and is) extended to 198:-pole circuit as the common and split it into 781: 779: 565:. Neither of these are suitable for use at 337:which can be described in matrix form by; 886:Herbert J. Carlin, Pier Paolo Civalleri, 776: 751: 749: 206:topologies and the resulting circuit has 149:are ports; (c) no pair of poles are ports 655: 551: 128: 113:The concept of ports can be extended to 18: 933:Acoustics: Sound Fields and Transducers 694: 94:, are analyzed in terms of ports. In 949: 843:Circuit Systems with MATLAB and PSpice 746: 802: 800: 764:Carlin & Civalleri, pp. 213–216 615: 13: 291:. Two-element one-ports (that is 14: 973: 797: 124: 828:Beranek & Mellow, pp. 96–100 98:, the circuit is regarded as a " 931:Leo Leroy Beranek, Tim Mellow, 835: 705:mechanical–electrical analogies 860:, John Wiley & Sons, 2012 845:, John Wiley & Sons, 2008 822: 813: 788: 767: 758: 1: 739: 547: 311:can be used. In particular, 651: 322: 247: 7: 841:Won Y. Yang, Seung C. Lee, 106:of parameters relating the 10: 978: 962:Linear electronic circuits 326: 141:are ports; (b) pole pairs 96:multiport network analysis 59:. A port consists of two 726:transfer function matrix 280:) are one-port devices. 935:, Academic Press, 2012 888:Wideband Circuit Design 305:Foster's canonical form 254:Kirchhoff's current law 121:must be accounted for. 918:Bond Graph Methodology 755:Yang & Lee, p. 401 672: 557: 498: 309:Cauer's canonical form 150: 32: 875:, Artech House, 2003 681:electromagnetic waves 659: 555: 499: 287:, most especially in 132: 22: 730:mechanical impedance 695:Other energy domains 582:directional couplers 344: 916:Wolfgang Borutzky, 794:Russer, pp. 237–238 724:equations or a 2Ă—2 610:directional filters 573:formats. Instead, 258:electrical elements 890:, CRC Press, 1997 673: 558: 494: 488: 448: 381: 204:unbalanced circuit 151: 88:electronic filters 49:electrical network 33: 670:waveguide flanges 285:network synthesis 57:electrical energy 969: 957:Circuit theorems 920:, Springer 2009 829: 826: 820: 819:Borutzsky, p. 20 817: 811: 804: 795: 792: 786: 783: 774: 771: 765: 762: 756: 753: 722:linear algebraic 616:RF and microwave 503: 501: 500: 495: 493: 492: 485: 484: 471: 470: 453: 452: 445: 444: 433: 432: 419: 418: 407: 406: 386: 385: 378: 377: 364: 363: 329:two-port network 243: 235: 231: 227: 210:−1 ports. 148: 144: 140: 136: 76:circuit analysis 30: 26: 977: 976: 972: 971: 970: 968: 967: 966: 947: 946: 903:System Dynamics 856:Frank Gustrau, 838: 833: 832: 827: 823: 818: 814: 805: 798: 793: 789: 785:Gustrau, p. 162 784: 777: 772: 768: 763: 759: 754: 747: 742: 734:transimpedances 697: 654: 618: 586:power splitters 550: 519: 512: 487: 486: 480: 476: 473: 472: 466: 462: 455: 454: 447: 446: 440: 436: 434: 428: 424: 421: 420: 414: 410: 408: 402: 398: 391: 390: 380: 379: 373: 369: 366: 365: 359: 355: 348: 347: 345: 342: 341: 331: 325: 278:current sources 274:voltage sources 250: 241: 237: 233: 229: 225: 218: 146: 142: 138: 134: 127: 119:waveguide modes 28: 24: 17: 12: 11: 5: 975: 965: 964: 959: 945: 944: 929: 914: 905:, Wiley, 2000 899: 884: 871:Peter Russer, 869: 854: 837: 834: 831: 830: 821: 812: 796: 787: 775: 766: 757: 744: 743: 741: 738: 696: 693: 689:waveguide mode 662:Moreno coupler 653: 650: 617: 614: 549: 546: 527:column vectors 517: 510: 505: 504: 491: 483: 479: 475: 474: 469: 465: 461: 460: 458: 451: 443: 439: 435: 431: 427: 423: 422: 417: 413: 409: 405: 401: 397: 396: 394: 389: 384: 376: 372: 368: 367: 362: 358: 354: 353: 351: 327:Main article: 324: 321: 249: 246: 239: 216: 179:bridge circuit 175:box attenuator 159:if and only if 126: 125:Port condition 123: 65:port condition 47:connecting an 37:circuit theory 35:In electrical 15: 9: 6: 4: 3: 2: 974: 963: 960: 958: 955: 954: 952: 942: 938: 934: 930: 927: 923: 919: 915: 912: 908: 904: 900: 897: 893: 889: 885: 882: 878: 874: 870: 867: 863: 859: 855: 852: 848: 844: 840: 839: 825: 816: 809: 803: 801: 791: 782: 780: 770: 761: 752: 750: 745: 737: 735: 731: 727: 723: 718: 714: 710: 706: 701: 692: 690: 685: 682: 678: 671: 667: 663: 658: 649: 645: 642: 638: 634: 630: 626: 622: 613: 611: 607: 603: 599: 595: 591: 587: 583: 578: 576: 572: 568: 564: 554: 545: 543: 539: 535: 530: 528: 524: 520: 513: 489: 481: 477: 467: 463: 456: 449: 441: 437: 429: 425: 415: 411: 403: 399: 392: 387: 382: 374: 370: 360: 356: 349: 340: 339: 338: 336: 330: 320: 318: 317:filter design 314: 310: 306: 302: 298: 294: 290: 289:filter design 286: 281: 279: 275: 271: 267: 263: 259: 255: 245: 223: 219: 211: 209: 205: 201: 197: 192: 187: 182: 180: 176: 172: 166: 164: 163:algebraic sum 160: 156: 131: 122: 120: 116: 111: 109: 105: 101: 97: 93: 89: 85: 81: 77: 72: 70: 66: 62: 58: 54: 50: 46: 43:is a pair of 42: 38: 21: 932: 917: 902: 887: 872: 857: 842: 836:Bibliography 824: 815: 807: 790: 769: 760: 716: 702: 698: 686: 674: 666:matched load 646: 637:ground plane 619: 602:multiplexers 579: 575:s-parameters 563:y-parameters 559: 531: 522: 515: 508: 506: 335:z-parameters 332: 282: 251: 221: 212: 207: 199: 195: 185: 183: 167: 152: 112: 84:transformers 73: 64: 40: 34: 713:transducers 590:circulators 538:attenuators 313:LC circuits 301:LC circuits 80:transistors 951:Categories 941:0123914213 926:1848828829 911:0471333018 896:0849378974 881:1580535321 866:111834958X 851:0470822406 740:References 732:, and two 709:bond graph 633:microstrip 548:Multiports 534:amplifiers 270:capacitors 171:generators 115:waveguides 92:amplifiers 677:waveguide 652:Waveguide 641:potential 625:microwave 598:duplexers 594:diplexers 571:waveguide 567:microwave 323:Two-ports 266:resistors 262:inductors 248:One-ports 191:generator 100:black box 45:terminals 806:Karnopp 155:terminal 69:currents 23:Network 810:, p. 14 629:coaxial 606:hybrids 542:filters 236:making 108:voltage 53:circuit 939:  924:  909:  894:  879:  864:  849:  808:et al. 507:where 234:(3, 2) 232:, and 230:(1, 4) 226:(1, 3) 147:(2, 3) 143:(1, 4) 139:(3, 4) 135:(1, 2) 104:matrix 90:, and 67:– the 61:nodes 937:ISBN 922:ISBN 907:ISBN 892:ISBN 877:ISBN 862:ISBN 847:ISBN 717:port 623:and 608:and 540:and 514:and 299:and 145:and 137:and 41:port 39:, a 707:or 631:or 307:or 242:= 6 51:or 953:: 799:^ 778:^ 748:^ 660:A 621:RF 612:. 604:, 600:, 596:, 592:, 588:, 584:, 544:. 536:, 529:. 442:22 430:21 416:12 404:11 319:. 297:RL 295:, 293:RC 276:, 272:, 268:, 264:, 228:, 186:no 181:. 86:, 82:, 943:. 928:. 913:. 898:. 883:. 868:. 853:. 523:n 518:n 516:I 511:n 509:V 490:] 482:2 478:I 468:1 464:I 457:[ 450:] 438:z 426:z 412:z 400:z 393:[ 388:= 383:] 375:2 371:V 361:1 357:V 350:[ 260:( 240:2 238:C 222:n 217:2 215:C 208:n 200:n 196:n 29:I 25:N

Index


circuit theory
terminals
electrical network
circuit
electrical energy
nodes
currents
circuit analysis
transistors
transformers
electronic filters
amplifiers
multiport network analysis
black box
matrix
voltage
waveguides
waveguide modes

terminal
if and only if
algebraic sum
generators
box attenuator
bridge circuit
generator
unbalanced circuit
C2
Kirchhoff's current law

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