575:
170:
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
31:
144:
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
169:
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
648:
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
153:
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
190:
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
107:
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
401:
132:
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
675:
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.,
553:
433:
687:
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
609:
Rectifier diodes (semiconductor or tube/valve) may have several voltage ratings, such as the peak inverse voltage (PIV) across the diode, and the maximum
174:
of that object. Breakdown voltage varies with the material composition, shape of an object, and the length of material between the electrical contacts.
598:
in the diode. Exceeding the breakdown voltage of a diode, per se, is not destructive; although, exceeding its current capacity will be. In fact,
724:
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.
212:
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.
124:, are free to move about the crystal lattice. An electric field causes a large current to flow, so metals have low
17:
755:
are exposed to transient lightning surge voltages induced on the power circuit. Electrical apparatus will have a
922:
898:
917:
526:
219:
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
409:
606:
normal diodes that exploit the breakdown voltage of a diode to provide regulation of voltage levels.
205:
831:
J. M. Meek and J. D. Craggs, Electrical
Breakdown of Gases, John Wiley & Sons, Chichester, 1978.
88:
603:
480:
43:
183:
858:
G. Cuttone, C. Marchetta, L. Torrisi, G. Della Mea, A. Quaranta, V. Rigato and S. Zandolin,
849:
Kalyatskii, I.I., Kassirov, G.M., and
Smirnov, G.V., Prib. Tekh. Eksp., 1974, no. 4, p. 84.
146:
84:
78:
51:
47:
8:
783:
773:
760:
187:
166:
159:
121:
814:
793:
788:
595:
556:
506:
486:
462:
442:
562:
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,
778:
744:
436:
238:
141:
104:
100:
242:
911:
649:
point-contact transistors such as the OC10 had values around 5 volts or less.
228:
698:
Collector to emitter rating when base is shorted to emitter; equivalent to
594:
that can be applied without causing an exponential increase in the leakage
46:
is the minimum voltage that causes a portion of an insulator to experience
128:, making them good conductors. In contrast in materials like plastics and
740:
599:
134:
125:
92:
840:
Emelyanov, A.A., Izv. Vyssh. Uchebn. Zaved., Fiz., 1989, no. 4, p. 103.
748:
246:
150:
583:
234:
523:
represents the distance in centimetres between the electrodes, and
117:
112:
from the positive contact to the negative contact. For example, in
613:
input voltage to the rectifier circuit (which will be much less).
591:
574:
129:
587:
113:
62:
58:
891:
Standard
Handbook for Electrical Engineers, Eleventh Edition
259:
The breakdown voltage in a partial vacuum is represented as
155:
618:
95:. A conductor is a substance which contains many mobile
30:
751:
and other electrical apparatus connected to overhead
529:
509:
489:
465:
445:
412:
268:
252:
In a gas, the breakdown voltage can be determined by
103:
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:
697:
692:
689:
686:
681:
678:
674:
669:
666:
663:
659:
654:
651:
647:
641:
634:
627:
624:
623:
622:
620:
614:
612:
607:
605:
604:heavily doped
601:
597:
593:
589:
585:
576:
567:
565:
564:Paschen's law
560:
559:Coefficient.
558:
531:
510:
490:
482:
466:
446:
438:
414:
386:
381:
364:
360:
355:
352:
348:
344:
341:
337:
333:
330:
327:
323:
319:
315:
311:
307:
303:
300:
295:
291:
287:
281:
270:
262:
261:
260:
257:
255:
254:Paschen's law
250:
248:
244:
240:
236:
230:
229:Gas discharge
220:
217:
215:
210:
208:
207:
200:
198:
194:
189:
185:
175:
173:
168:
163:
161:
157:
152:
148:
143:
138:
136:
131:
127:
123:
119:
115:
111:
106:
102:
98:
94:
90:
86:
80:
70:
68:
64:
60:
55:
53:
49:
45:
41:
32:
19:
890:
885:
876:
867:
859:
854:
845:
836:
827:
818:
809:
756:
741:transformers
738:
728:
726:
723:
712:
706:
699:
690:
679:
667:
661:
652:
639:
632:
625:
615:
608:
600:Zener diodes
581:
561:
405:
258:
251:
232:
218:
211:
204:
201:
196:
181:
171:
164:
139:
82:
66:
56:
39:
37:
819:www.pact.in
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:)
Text is available under the Creative Commons Attribution-ShareAlike License. Additional terms may apply.