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长电肖特基整流管

产品名称:长电肖特基整流管

所属类别:长电肖特基整流管

产品简介:

详细介绍

       肖特基二极管是以金属与半导体接触形成的金属-半导体结原理制作的,因此也叫金属-半导体二极管。一般以贵金属(金、银、铂等)A做正极,N型半导体B做负极,以两者接触面上形成的有整流作用的势垒为原理工作的。有插件式和贴片式两种封装。

       肖特基整流管的优点是开关频率高、正向压降低等,缺点也很明显反向击穿电压低、反向漏电流偏大。但是经过科技的发展,以及对肖特基二极管的持续研究,现已有了突破性进展反向击穿电压已达到200V,新型材料的1kV肖特基整流管也已研制成功。

       肖特基整流管一般应用在低压、大电流输出电路上作为高频整流使用,在非常高的频率下可用于检波和混频,在高速逻辑电路中可用作箝位。广泛应用于开关电源、变频器、驱动器等电路中。

       长电二极管,肖特基整流管系列:

肖特基整流管PDIOVRVF封装形式
(W)(A)(V)(V)
CJ10L45G410450.47
MBR101002101000.84TO-220A
MBR10100CT2101000.95TO-220-3L
MBR10100FCT2101000.95TO-220F
MBR101502101501TO-220A
MBR10150CT2101501TO-220-3L
MBR10150FCT2101501TO-220F
MBR102002102000.95TO-220A
MBR10200CT2102001.1TO-220-3L
MBR10200FCT2102001.1TO-220F
MBR1030210300.84TO-220A
MBR1030CT210300.7TO-220-3L
MBR1030FCT210300.7TO-220F
MBR1035210350.84TO-220A
MBR1035CT210350.7TO-220-3L
MBR1035FCT210350.7TO-220F
MBR1040210400.84TO-220A
MBR1040CT210400.7TO-220-3L
MBR1040FCT210400.7TO-220F
MBR1045210450.84TO-220A
MBR1045CT210450.7TO-220-3L
MBR1045FCT210450.7TO-220F
MBR1050210500.95TO-220A
MBR1050CT210500.8TO-220-3L
MBR1050FCT210500.8TO-220F
MBR1060210600.8TO-220A
MBR1060CT210600.8TO-220-3L
MBR1060FCT210600.95TO-220F
MBR1070CT210700.95TO-220-3L
MBR1070FCT210700.95TO-220F
MBR1080210800.84TO-220A
MBR1080CT210800.95TO-220-3L
MBR1080FCT210800.95TO-220F
MBR1090210900.84TO-220A
MBR1090CT210900.95TO-220-3L
MBR1090FCT210900.95TO-220F
MBR20100CT2201001.2TO-220-3L
MBR20100FCT2201001.2TO-220F
MBR20120FCT2201200.92TO-220F
MBR201502201500.9TO-220A
MBR20150CT2201501.2TO-220-3L
MBR20150FCT2201501.2TO-220F
MBR202002202000.9TO-220A
MBR20200CT2202001.2TO-220-3L
MBR20200FCT2202001.2TO-220F
MBR2030CT220300.7TO-220-3L
MBR2030FCT220300.7TO-220F
MBR2035CT220350.7TO-220-3L
MBR2035FCT220350.7TO-220F
MBR2040CT220400.7TO-220-3L
MBR2040FCT220400.7TO-220F
MBR2045CT220450.7TO-220-3L
MBR2045FCT220450.7TO-220F
MBR2050CT220500.8TO-220-3L
MBR2050FCT220500.8TO-220F
MBR2060CT220600.8TO-220-3L
MBR2060FCT220600.8TO-220F
MBR2545FCT225450.7TO-220F
MBR30100CT2301001.05TO-220-3L
MBR30100FCT2301001.05TO-220F
MBR30100PT3.5