| 型号/型号规格 | 分类 | 品牌 | 封装 | 批号 | 数量 | 询价 | ||
|---|---|---|---|---|---|---|---|---|
| P2804HVG | 双N沟道MOS管 |
NIKO-SEM/尼克森 |
SOP-8 |
12+ |
1100 |
|||
| MDU5512URH | 双N沟道MOS管 |
MAGNACHIP/美格纳 |
DFN-85x6 |
12+ |
11000 |
|||
| FDC3601N | 双N沟道MOS管 |
FAIRCHILD/仙童 |
TSOP-6 |
14+ |
171 |
|||
| APM9988QBC-TRG | 双N沟道MOS管 |
SINOPOWER/大中 |
DFN-6 2x5 |
12+ |
51000 |
|||
| AOSD32344C | 双N沟道MOS管 |
AOS/万代 |
SOIC-8 |
20+ |
2999 |
|||
| AOSD32334S | 双N沟道MOS管 |
AOS/万代 |
SOIC-8 |
20+ |
2999 |
|||
| AONX38168 | 双N沟道MOS管 |
AOS/万代 |
DFN-85x6 |
18+ |
11000 |
|||
| AON7812 | 双N沟道MOS管 |
AOS/万代 |
DFN3x3_Dual |
16+ |
5999 |
|||
| AON6938 | 双N沟道MOS管 |
AOS/万代 |
DFN-85x6 |
14+ |
51000 |
|||
| AON6934 | 双N沟道MOS管 |
AOS/万代 |
DFN-85x6 |
12+ |
2999 |
|||
| AOC2802 | 双N沟道MOS管 |
AOS/万代 |
WL-CSP 4L 1.6x1.6 |
13+ |
5999 |
|||
| AO4918 | 双N沟道MOS管 |
AOS/万代 |
SOP-8 |
05+ |
1807 |
|||
| AO4840L | 双N沟道MOS管 |
AOS/万代 |
SOP-8 |
18+ |
2100 |
|||
| KIA5N80HF | MOS(场效应管) |
KIA/可易亚 |
TO-220F |
16+ |
5999 |
|||
| KHB9D5N20F-U/P | MOS(场效应管) |
KEC/开益禧 |
TO-220F |
10+ |
21000 |
|||
| KF7N60P-U/PS | MOS(场效应管) |
KEC/开益禧 |
TO-220 |
15+ |
11000 |
|||
| KF5N53DS-RTF/HS | MOS(场效应管) |
KEC/开益禧 |
TO-252 |
17+ |
1100 |
|||
| KF5N50IZ-U/HS | MOS(场效应管) |
KEC/开益禧 |
TO-251 |
15+ |
5999 |
|||
| IRFW830ATM | MOS(场效应管) |
FAIRCHILD/仙童 |
TO-263 |
00+ |
5999 |
|||
| IPW50R399CP | MOS(场效应管) |
INFINEON/英飞凌 |
TO-247 |
09+ |
5999 |
|||
| IPW50R299CP | MOS(场效应管) |
INFINEON/英飞凌 |
TO-247 |
09+ |
5999 |
|||
| IPI50R140CP | MOS(场效应管) |
INFINEON/英飞凌 |
TO-262 |
08+ |
144 |
|||
| IPF105N03LG | MOS(场效应管) |
INFINEON/英飞凌 |
TO-252 |
07+ |
1100 |
|||
| IPDH9N03LAG | MOS(场效应管) |
INFINEON/英飞凌 |
TO-252 |
09+ |
1405 |
|||
| IPD03N03LBG | MOS(场效应管) |
INFINEON/英飞凌 |
TO-252 |
08+ |
1308 |
|||
| HFU1N80 | MOS(场效应管) |
SEMIHOW |
TO-251 |
06+ |
11000 |
|||
| FQPF5N50CFTU | MOS(场效应管) |
FAIRCHILD/仙童 |
TO-220F |
10+ |
1100 |
|||
| FQD7N20TM | MOS(场效应管) |
FAIRCHILD/仙童 |
TO-252 |
13+ |
982 |
|||
| FDMS0308AS | MOS(场效应管) |
FAIRCHILD/仙童 |
DFN-85x6 |
13+ |
2100 |
|||
| FDMC86106LZ | MOS(场效应管) |
FAIRCHILD/仙童 |
MLP3.3x3.3 |
14+ |
2100 |