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HBLS系列高频电感
尺寸毫米(公寸):0603、1005、1608、2012
电感范围:1.0~680nH
额定电流(mA):±0.3nH,±5%
产品介绍
HBLS系列高频电感,积层式晶片电感系列是由瓷料和低阻抗的银导体组成,提供优越之的品质系数及共振频率。
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产品料号
Model
感值
Inductance
公差
Tolerances
品质系数
Q
测试频率
Test Frequency
共振频率
Self-resonant Frequency
直流电阻
DC Resistance (Ω)Max.
额定电流
Rated Current (mA)Max.

Symbol 符号 nH % min MHz GHz DCR Ir
产品料号
Model
感值
Inductance
公差
Tolerances
品质系数
Q
测试频率
Test Frequency
共振频率
Self-resonant Frequency
直流电阻
DC Resistance (Ω)Max.
额定电流
Rated Current (mA)Max.

Symbol 符号 nH % min MHz GHz DCR Ir
HBLS0603-1N0S 1 ±0.3nH 4 100 10 0.14 250 0.33Max
HBLS0603-1N2S 1.2 ±0.3nH 4 100 10 0.14 250 0.33Max
HBLS0603-1N5S 1.5 ±0.3nH 4 100 10 0.18 230 0.33Max
HBLS0603-1N8S 1.8 ±0.3nH 4 100 10 0.19 200 0.33Max
HBLS0603-2N2S 2.2 ±0.3nH 4 100 8.8 0.22 200 0.33Max
HBLS0603-2N7S 2.7 ±0.3nH 5 100 7.7 0.25 200 0.33Max
HBLS0603-3N3S 3.3 ±0.3nH 5 100 6.7 0.3 180 0.33Max
HBLS0603-3N9S 3.9 ±0.3nH 5 100 6 0.3 170 0.33Max
HBLS0603-4N7S 4.7 ±0.3nH 5 100 5.3 0.4 150 0.33Max
HBLS0603-5N1S 5.1 ±0.3nH 5 100 4.7 0.4 150 0.33Max
HBLS0603-5N6S 5.6 ±0.3nH 5 100 4.2 0.4 150 0.33Max
HBLS0603-6N8J 6.8 ±5% 5 100 3.5 0.5 150 0.33Max
HBLS0603-8N2J 8.2 ±5% 5 100 3.2 0.55 150 0.33Max
HBLS0603-10NJ 10 ±5% 5 100 2.8 0.65 150 0.33Max
HBLS0603-12NJ 12 ±5% 5 100 2.4 0.7 100 0.33Max
HBLS0603-15NJ 15 ±5% 5 100 2.2 0.8 100 0.33Max
HBLS0603-18NJ 18 ±5% 5 100 2.1 0.9 100 0.33Max
HBLS0603-22NJ 22 ±5% 5 100 1.8 1.5 100 0.33Max
HBLS0603-27NJ 27 ±5% 4 100 1.8 1.8 50 0.33Max
HBLS0603-33NJ 33 ±5% 4 100 1.7 2.1 50 0.33Max
HBLS0603-39NJ 39 ±5% 4 100 1.5 2.4 50 0.33Max
HBLS1005-1N0S 1 ±0.3nH 8 100 10 0.08 300 0.5±0.05
HBLS1005-1N2S 1.2 ±0.3nH 8 100 10 0.09 300 0.5±0.05
HBLS1005-1N5S 1.5 ±0.3nH 8 100 6 0.1 300 0.5±0.05
HBLS1005-1N8S 1.8 ±0.3nH 8 100 6 0.12 300 0.5±0.05
HBLS1005-2N0S 2 ±0.3nH 8 100 6 0.12 300 0.5±0.05
HBLS1005-2N2S 2.2 ±0.3nH 8 100 6 0.13 300 0.5±0.05
HBLS1005-2N4S 2.4 ±0.3nH 8 100 6 0.13 300 0.5±0.05
HBLS1005-2N7S 2.7 ±0.3nH 8 100 6 0.13 300 0.5±0.05
HBLS1005-3N0S 3 ±0.3nH 8 100 6 0.16 300 0.5±0.05
HBLS1005-3N3S 3.3 ±0.3nH 8 100 6 0.16 300 0.5±0.05
HBLS1005-3N9S 3.9 ±0.3nH 8 100 4 0.21 300 0.5±0.05
HBLS1005-4N7S 4.7 ±0.3nH 8 100 4 0.21 300 0.5±0.05
HBLS1005-5N6S 5.6 ±0.3nH 8 100 4 0.23 300 0.5±0.05
HBLS1005-6N8J 6.8 ±5% 8 100 3.9 0.25 300 0.5±0.05
HBLS1005-8N2J 8.2 ±5% 8 100 3.6 0.28 300 0.5±0.05
HBLS1005-10NJ 10 ±5% 8 100 3.2 0.31 300 0.5±0.05
HBLS1005-12NJ 12 ±5% 8 100 2.7 0.4 300 0.5±0.05
HBLS1005-15NJ 15 ±5% 8 100 2.3 0.46 300 0.5±0.05
HBLS1005-18NJ 18 ±5% 8 100 2.1 0.55 300 0.5±0.05
HBLS1005-22NJ 22 ±5% 8 100 1.9 0.6 300 0.5±0.05
HBLS1005-27NJ 27 ±5% 8 100 1.6 0.7 300 0.5±0.05
HBLS1005-33NJ 33 ±5% 8 100 1.3 0.8 200 0.5±0.05
HBLS1005-39NJ 39 ±5% 8 100 1.2 0.9 200 0.5±0.05
HBLS1005-47NJ 47 ±5% 8 100 1 1 200 0.5±0.05
HBLS1005-56NJ 56 ±5% 8 100 0.75 1 200 0.5±0.05
HBLS1005-68NJ 68 ±5% 8 100 0.75 1.2 180 0.5±0.05
HBLS1005-82NJ 82 ±5% 8 100 0.6 1.3 150 0.5±0.05
HBLS1005-R10J 100 ±5% 8 100 0.6 1.5 150 0.5±0.05
HBLS1005-R12J 120 ±5% 8 100 0.6 1.6 150 0.5±0.05
HBLS1608-1N0S 1 ±0.3nH 8 100 10 0.05 300 0.8±0.15
HBLS1608-1N2S 1.2 ±0.3nH 8 100 10 0.05 300 0.8±0.15
HBLS1608-1N5S 1.5 ±0.3nH 8 100 6 0.1 300 0.8±0.15
HBLS1608-1N8S 1.8 ±0.3nH 8 100 6 0.1 300 0.8±0.15
HBLS1608-2N2S 2.2 ±0.3nH 8 100 6 0.1 300 0.8±0.15
HBLS1608-2N7S 2.7 ±0.3nH 10 100 6 0.1 300 0.8±0.15
HBLS1608-3N3S 3.3 ±0.3nH 10 100 6 0.12 300 0.8±0.15
HBLS1608-3N9S 3.9 ±0.3nH 10 100 6 0.14 300 0.8±0.15
HBLS1608-4N7S 4.7 ±0.3nH 10 100 4 0.16 300 0.8±0.15
HBLS1608-5N6S 5.6 ±0.3nH 10 100 4 0.18 300 0.8±0.15
HBLS1608-6N8J 6.8 ±5% 10 100 4 0.22 300 0.8±0.15
HBLS1608-8N2J 8.2 ±5% 10 100 3.5 0.24 300 0.8±0.15
HBLS1608-10NJ 10 ±5% 12 100 3.4 0.26 300 0.8±0.15
HBLS1608-12NJ 12 ±5% 12 100 2.6 0.28 300 0.8±0.15
HBLS1608-15NJ 15 ±5% 12 100 2.3 0.32 300 0.8±0.15
HBLS1608-18NJ 18 ±5% 12 100 2 0.35 300 0.8±0.15
HBLS1608-22NJ 22 ±5% 12 100 1.6 0.4 300 0.8±0.15
HBLS1608-27NJ 27 ±5% 12 100 1.4 0.45 300 0.8±0.15
HBLS1608-33NJ 33 ±5% 12 100 1.2 0.55 300 0.8±0.15
HBLS1608-39NJ 39 ±5% 12 100 1.1 0.6 300 0.8±0.15
HBLS1608-47NJ 47 ±5% 12 100 0.9 0.7 300 0.8±0.15
HBLS1608-56NJ 56 ±5% 12 100 0.9 0.75 300 0.8±0.15
HBLS1608-68NJ 68 ±5% 12 100 0.7 0.85 300 0.8±0.15
HBLS1608-82NJ 82 ±5% 12 100 0.6 0.95 300 0.8±0.15
HBLS1608-R10J 100 ±5% 12 100 0.6 1 300 0.8±0.15
HBLS1608-R12J 120 ±5% 8 50 0.5 1.2 300 0.8±0.15
HBLS1608-R15J 150 ±5% 8 50 0.5 1.2 300 0.8±0.15
HBLS1608-R18J 180 ±5% 8 50 0.4 1.3 300 0.8±0.15
HBLS1608-R22J 220 ±5% 8 50 0.4 1.5 300 0.8±0.15
HBLS2012-1N0S 1 ±0.3nH 10 100 10 0.1 300 0.85±0.2
HBLS2012-1N2S 1.2 ±0.3nH 10 100 10 0.1 300 0.85±0.2
HBLS2012-1N5S 1.5 ±0.3nH 10 100 4 0.1 300 0.85±0.2
HBLS2012-1N8S 1.8 ±0.3nH 10 100 4 0.1 300 0.85±0.2
HBLS2012-2N2S 2.2 ±0.3nH 10 100 4 0.1 300 0.85±0.2
HBLS2012-2N7S 2.7 ±0.3nH 12 100 4 0.1 300 0.85±0.2
HBLS2012-3N3S 3.3 ±0.3nH 12 100 4 0.13 300 0.85±0.2
HBLS2012-3N9S 3.9 ±0.3nH 12 100 4 0.15 300 0.85±0.2
HBLS2012-4N7S 4.7 ±0.3nH 12 100 3.5 0.2 300 0.85±0.2
HBLS2012-5N6S 5.6 ±0.3nH 15 100 3.2 0.23 300 0.85±0.2
HBLS2012-6N8J 6.8 ±5% 15 100 2.8 0.25 300 0.85±0.2
HBLS2012-8N2J 8.2 ±5% 15 100 2.4 0.28 300 0.85±0.2
HBLS2012-10NJ 10 ±5% 15 100 2.1 0.3 300 0.85±0.2
HBLS2012-12NJ 12 ±5% 15 100 1.9 0.35 300 0.85±0.2
HBLS2012-15NJ 15 ±5% 15 100 1.6 0.4 300 0.85±0.2
HBLS2012-18NJ 18 ±5% 15 100 1.5 0.45 300 0.85±0.2
HBLS2012-22NJ 22 ±5% 18 100 1.4 0.5 300 0.85±0.2
HBLS2012-27NJ 27 ±5% 18 100 1.3 0.55 300 0.85±0.2
HBLS2012-33NJ 33 ±5% 18 100 1.2 0.6 300 0.85±0.2
HBLS2012-39NJ 39 ±5% 18 100 1 0.65 300 0.85±0.2
HBLS2012-47NJ 47 ±5% 18 100 0.9 0.7 300 0.85±0.2
HBLS2012-56NJ 56 ±5% 18 100 0.8 0.75 300 0.85±0.2
HBLS2012-68NJ 68 ±5% 18 100 0.7 0.8 300 0.85±0.2
HBLS2012-82NJ 82 ±5% 18 100 0.6 0.9 300 0.85±0.2
HBLS2012-R10J 100 ±5% 18 100 0.6 0.9 300 0.85±0.2
HBLS2012-R12J 120 ±5% 13 50 0.5 0.95 300 0.85±0.2
HBLS2012-R15J 150 ±5% 13 50 0.5 1 300 1.25±0.2
HBLS2012-R18J 180 ±5% 13 50 0.4 1.1 300 1.25±0.2
HBLS2012-R22J 220 ±5% 12 50 0.35 1.2 300 1.25±0.2
HBLS2012-R27J 270 ±5% 12 50 0.3 1.3 300 1.25±0.2
HBLS2012-R33J 330 ±5% 12 50 0.25 1.4 300 1.25±0.2
HBLS2012-R39J 390 ±5% 10 50 0.25 1.4 300 1.25±0.2
HBLS2012-R48J 470 ±5% 10 50 0.2 4 200 1.25±0.2
HBLS2012-R56J 560 ±5% 10 25 0.18 5 50 1.25±0.2
HBLS2012-R68J 680 ±5% 10 25 0.16 5 50 1.25±0.2