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Breakdown voltage

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become conductive, that area has almost no voltage drop and the full voltage is applied across the remaining length of the insulator, resulting in a higher gradient and electric field, causing additional areas in the insulator to break down. The breakdown quickly spreads in a conductive path through the insulator until it extends from the positive to the negative contact. The voltage at which this occurs is called the
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is applied, all insulators become conductors. If the voltage applied across a piece of insulator is increased, at a certain electric field strength the number of charge carriers in the material suddenly increases enormously and its resistivity drops, causing a strong current to flow through it. This
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of the voltage. The voltage gradient may vary at different points across the object, due to its shape or local variations in composition. Electrical breakdown occurs when the field first exceeds the dielectric strength of the material in some region of the object. Once one area has broken down and
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The maximum voltage between collector and emitter that can be safely applied (and with no more than some specified leakage current, often) when no circuit at the base of the transistor is there to remove collector-base leakage. Typical values: 20 volts to as high as 700 volts; very early Germanium
759:(BIL) specified. This is the crest value of an impulse waveform with a standardized wave shape, intended to simulate the electrical stress of a lightning surge or a surge induced by circuit switching. The BIL is coordinated with the typical operating voltage of the apparatus. For high-voltage 202:
The breakdown voltage of a material is not a definite value because it is a form of failure and there is a statistical probability whether the material will fail at a given voltage. When a value is given it is usually the mean breakdown voltage of a large sample. Another term is
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them. The released electrons are accelerated by the field and strike other atoms, creating more free electrons and ions in a chain reaction, flooding the material with charged particles. This occurs at a characteristic electric field strength in each material, measured in
249:). Using other gases, this breakdown potential may decrease to an extent that two uninsulated surfaces with different potentials might induce the electrical breakdown of the surrounding gas. This may damage an apparatus, as a breakdown is analogous to a short circuit. 763:, the impulse level is related to the clearance to ground of energized components. As an example, a transmission line rated 138 kV would be designed for a BIL of 650 kV. A higher BIL may be specified than the minimum, where the exposure to lightning is severe. 616:
Many small-signal transistors need to have any breakdown currents limited to much lower values to avoid excessive heating. To avoid damage to the device, and to limit the effects excessive leakage current may have on the surrounding circuit, the following
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difference that can be applied across the material before the insulator conducts. In solid insulating materials, this usually creates a weakened path within the material by creating permanent molecular or physical changes by the sudden
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is created across a piece of the material by applying a voltage difference between electrical contacts on different sides of the material. The force of the field causes the charge carriers within the material to move, creating an
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all the electrons are tightly bound to atoms, so under normal conditions there are very few mobile charge carriers in the material. Applying a voltage causes only a very small current to flow, giving the material a very high
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The maximum voltage rating between collector and emitter with some specified resistance (or less) between base and emitter. A more realistic rating for real-world circuits than the open-base or open-emitter scenarios
216:. The impulse breakdown voltage is simulating lightning strikes, and usually uses a 1.2 microsecond rise for the wave to reach 90% amplitude, then drops back down to 50% amplitude after 50 microseconds. 233:
In standard conditions at atmospheric pressure, air serves as an excellent insulator, requiring the application of a significant voltage of 3.0 kV/mm before breaking down (e.g.,
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The maximum reverse voltage on the base with respect to the emitter. Typically around 5 volts - more for germanium transistors, less for UHF transistors usually.
521: 501: 477: 457: 209:, where the probability of failure at a given voltage is so low it is considered, when designing insulation, that the material will not fail at this voltage. 265: 871:
H. Moscicka-Grzesiak, H. Gruszka and M. Stroinski, ‘‘Influence of Electrode Curvature on Predischarge Phenomena and Electric Strength at 50 Hz of a Vacuum
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Rectifier diodes (semiconductor or tube/valve) may have several voltage ratings, such as the peak inverse voltage (PIV) across the diode, and the maximum
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of that object. Breakdown voltage varies with the material composition, shape of an object, and the length of material between the electrical contacts.
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in the diode. Exceeding the breakdown voltage of a diode, per se, is not destructive; although, exceeding its current capacity will be. In fact,
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Field-effect transistors have similar maximum ratings, the most important one for junction FETs is the gate-drain voltage rating.
61:, the breakdown voltage is the minimum reverse voltage that makes the diode conduct appreciably in reverse. Some devices (such as 720:
Collector to emitter rating when a specific base-emitter voltage is supplied, such as in some high voltage switching scenarios.
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Two different breakdown voltage measurements of a material are the AC and impulse breakdown voltages. The AC voltage is the
149:. Breakdown occurs when the electric field becomes strong enough to pull electrons from the molecules of the material, 880:
R. V. Latham, High Voltage Vacuum Insulation: Basic concepts and technological practice, Academic Press, London, 1995.
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are exposed to transient lightning surge voltages induced on the power circuit. Electrical apparatus will have a
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Two technical standards governing performing these tests are ASTM D1816 and ASTM D3300 published by ASTM.
195:. Within rarefied gases found in certain types of lamps, breakdown voltage is also sometimes called the 165:
When a voltage is applied across a piece of insulator, the electric field at each point is equal to the
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normal diodes that exploit the breakdown voltage of a diode to provide regulation of voltage levels.
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J. M. Meek and J. D. Craggs, Electrical Breakdown of Gases, John Wiley & Sons, Chichester, 1978.
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G. Cuttone, C. Marchetta, L. Torrisi, G. Della Mea, A. Quaranta, V. Rigato and S. Zandolin,
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Kalyatskii, I.I., Kassirov, G.M., and Smirnov, G.V., Prib. Tekh. Eksp., 1974, no. 4, p. 84.
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A detailed derivation, and some background information, is given in the article about
396:{\displaystyle V_{\mathrm {b} }={\frac {B\,p\,d}{\ln \left(A\,p\,d\right)-\ln \left}}} 894: 752: 213: 610: 563: 253: 192: 109: 96: 860:
Surface Treatment of HV Electrodes for Superconducting Cyclotron Beam Extraction,
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point-contact transistors such as the OC10 had values around 5 volts or less.
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Collector to emitter rating when base is shorted to emitter; equivalent to
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that can be applied without causing an exponential increase in the leakage
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is the minimum voltage that causes a portion of an insulator to experience
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Emelyanov, A.A., Izv. Vyssh. Uchebn. Zaved., Fiz., 1989, no. 4, p. 103.
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represents the distance in centimetres between the electrodes, and
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from the positive contact to the negative contact. For example, in
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input voltage to the rectifier circuit (which will be much less).
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Standard Handbook for Electrical Engineers, Eleventh Edition
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The breakdown voltage in a partial vacuum is represented as
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and other electrical apparatus connected to overhead
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In a gas, the breakdown voltage can be determined by
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which are free to move about inside the material. An
569: 547: 515: 495: 471: 451: 427: 395: 909: 621:transistor maximum ratings are often specified: 503:represents the pressure of the surrounding gas, 862:IEEE. Trans. DEI, Vol. 4, pp. 218<223, 1997. 34:High voltage breakdown of an insulator string 27:Voltage at which insulator becomes conductive 182:Breakdown voltage is a characteristic of an 318: 314: 294: 290: 573: 29: 734: 660:The maximum collector-to-base voltage, 548:{\displaystyle \gamma _{\mathrm {se} }} 137:, and these are classed as insulators. 72: 14: 910: 116:one or more of the negatively charged 483:that depend on the surrounding gas, 435:is the breakdown potential in volts 222: 24: 664:. Typical values 25 to 1200 volts. 539: 536: 419: 372: 369: 275: 83:Materials are often classified as 25: 934: 590:that defines the largest reverse 428:{\displaystyle V_{\mathrm {b} }} 570:Diodes and other semiconductors 883: 874: 865: 852: 843: 834: 825: 807: 13: 1: 800: 757:basic lightning impulse level 727:Some devices may also have a 140:However, if a strong enough 7: 766: 557:Secondary Electron Emission 214:line frequency of the mains 158:per centimeter, called its 10: 939: 815:"Benefits of BDV testing?" 226: 76: 889:D. G. Fink, H. W. Beaty, 662:with emitter open-circuit 245:, or the electrodes of a 186:that defines the maximum 177: 67:forward breakdown voltage 50:and become electrically 582:Breakdown voltage is a 731:of voltage specified. 729:maximum rate of change 579: 549: 517: 497: 473: 453: 429: 397: 35: 923:Electrical parameters 893:, McGraw-Hill, 1978, 602:are essentially just 577: 550: 518: 498: 474: 454: 430: 398: 120:in each atom, called 33: 918:Electrical breakdown 735:Electrical apparatus 527: 507: 487: 463: 443: 410: 266: 147:electrical breakdown 122:conduction electrons 79:Electrical breakdown 73:Electrical breakdown 48:electrical breakdown 784:Dielectric strength 774:Avalanche breakdown 631:(sometimes written 241:across plates of a 160:dielectric strength 794:Lichtenberg figure 789:Electrical treeing 761:transmission lines 753:transmission lines 580: 545: 513: 493: 469: 449: 425: 393: 36: 578:Diode I-V diagram 516:{\displaystyle d} 496:{\displaystyle p} 472:{\displaystyle B} 452:{\displaystyle A} 391: 378: 206:withstand voltage 172:breakdown voltage 97:charged particles 40:breakdown voltage 16:(Redirected from 930: 902: 887: 881: 878: 872: 869: 863: 856: 850: 847: 841: 838: 832: 829: 823: 822: 811: 745:circuit breakers 554: 552: 551: 546: 544: 543: 542: 522: 520: 519: 514: 502: 500: 499: 494: 478: 476: 475: 470: 458: 456: 455: 450: 434: 432: 431: 426: 424: 423: 422: 402: 400: 399: 394: 392: 390: 389: 385: 384: 380: 379: 377: 376: 375: 359: 326: 322: 298: 285: 280: 279: 278: 223:Gases and vacuum 197:striking voltage 110:electric current 21: 18:Striking voltage 938: 937: 933: 932: 931: 929: 928: 927: 908: 907: 906: 905: 901:, page 17-20 ff 888: 884: 879: 875: 870: 866: 857: 853: 848: 844: 839: 835: 830: 826: 821:. 17 June 2021. 813: 812: 808: 803: 798: 779:Avalanche diode 769: 737: 717: 704: 695: 684: 672: 657: 644: 637: 630: 572: 555:represents the 535: 534: 530: 528: 525: 524: 508: 505: 504: 488: 485: 484: 464: 461: 460: 444: 441: 440: 418: 417: 413: 411: 408: 407: 368: 367: 363: 358: 351: 347: 340: 336: 310: 306: 299: 286: 284: 274: 273: 269: 267: 264: 263: 231: 225: 180: 101:charge carriers 91:based on their 81: 75: 28: 23: 22: 15: 12: 11: 5: 936: 926: 925: 920: 904: 903: 882: 873: 864: 851: 842: 833: 824: 805: 804: 802: 799: 797: 796: 791: 786: 781: 776: 770: 768: 765: 736: 733: 722: 721: 718: 715: 710: 702: 696: 693: 688: 685: 682: 677: 673: 670: 665: 658: 655: 650: 646: 642: 635: 628: 571: 568: 541: 538: 533: 512: 492: 468: 448: 421: 416: 404: 403: 388: 383: 374: 371: 366: 362: 357: 354: 350: 346: 343: 339: 335: 332: 329: 325: 321: 317: 313: 309: 305: 302: 297: 293: 289: 283: 277: 272: 227:Main article: 224: 221: 179: 176: 142:electric field 105:electric field 77:Main article: 74: 71: 65:) also have a 26: 9: 6: 4: 3: 2: 935: 924: 921: 919: 916: 915: 913: 900: 896: 892: 886: 877: 868: 861: 855: 846: 837: 828: 820: 816: 810: 806: 795: 792: 790: 787: 785: 782: 780: 777: 775: 772: 771: 764: 762: 758: 754: 750: 746: 742: 732: 730: 725: 719: 714: 711: 708: 701: 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135:resistivity 126:resistivity 93:resistivity 912:Categories 899:007020974X 801:References 749:switchgear 247:spark plug 145:is called 89:insulators 85:conductors 52:conductive 584:parameter 532:γ 481:constants 365:γ 345:⁡ 334:⁡ 328:− 304:⁡ 243:capacitor 235:lightning 184:insulator 118:electrons 44:insulator 767:See also 239:sparking 167:gradient 151:ionizing 130:ceramics 643:(BR)CEO 619:bipolar 596:current 592:voltage 193:current 188:voltage 99:called 897:  739:Power 676:above. 406:where 178:Solids 114:metals 63:TRIACs 59:diodes 42:of an 705:when 588:diode 586:of a 237:, or 156:volts 895:ISBN 709:= 0. 479:are 459:and 57:For 38:The 716:CEX 703:CER 694:CES 683:EBO 671:CER 656:CBO 638:or 636:CEO 629:CEO 611:RMS 87:or 914:: 817:. 747:, 743:, 633:BV 566:. 439:, 437:DC 342:ln 331:ln 301:ln 256:. 199:. 162:. 69:. 54:. 713:V 707:R 700:V 691:V 680:V 668:V 653:V 645:) 640:V 626:V 540:e 537:s 511:d 491:p 467:B 447:A 420:b 415:V 387:] 382:) 373:e 370:s 361:1 356:+ 353:1 349:( 338:[ 324:) 320:d 316:p 312:A 308:( 296:d 292:p 288:B 282:= 276:b 271:V 20:)

Index

Striking voltage

insulator
electrical breakdown
conductive
diodes
TRIACs
Electrical breakdown
conductors
insulators
resistivity
charged particles
charge carriers
electric field
electric current
metals
electrons
conduction electrons
resistivity
ceramics
resistivity
electric field
electrical breakdown
ionizing
volts
dielectric strength
gradient
insulator
voltage
current

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