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SLC-5020A
Measure without shaking within the measurement range.
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4263B 100kHz Ls Mode
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8.2 nH
5% AOBA
SW11008CT8N2J
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11 nH Measure by attaching a lead
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A
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15 nH
5% Fastron
0805AS-015J
|
11 nH Measure by attaching a lead
|
A
|
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18 nH
10% TDK
NL322522T-018K
|
17 nH
|
A
|
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22 nH 5% Coilcraft
1008HS-220T 2520
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nH
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27 nH
5% Coilcraft
1008HS-270T 2520
Inductance measured using a Coilcraft SMD-A fixture in an Agilent/HP 4286A impedance analyzer with Coilcraft-provided correlation pieces.
(Notation in data sheet)
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28 nH Measure by attaching a lead
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Notation in data sheet
Inductance measured using a Coilcraft SMD-A fixture in an Agilent/HP 4286A impedance analyzer with Coilcraft-provided correlation pieces.
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100 nH 10% Ceratech
FI-A2012-101K
Bead 0mA
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nH
|
A
|
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120 nH
10% TDK
NL252018T-R12K
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112 nH
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Ls 0.130# μH 100kHz
+8.3%
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120 nH +25% MAG.Layers
MLB-453215-0120A-N2
Multilayer Chip Beads 300mA
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nH
|
|
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150 nH
5% Coilcraft
1008HS-151T 2520
|
135nH
|
A
|
|
180 nH
5% TDK
NL322522T-R18J-3
|
178 nH
|
|
|
330 nH
10% Ceratech
FI-A2012-331K
Bead 0mA
|
337 nH
|
A
|
|
560 nH
5% TAIYO
LEM2520T-R56J
|
536 nH
|
Ls 0.559# μH 100kHz
+4.0%
Ls 0.55# μH 10kHz
+%
|
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560 nH
5% Delta
1008CS-561EJPS
|
516 nH
|
|
|
560 nH
20% Murata
LQH3NR56M04
|
532 nH
|
|
|
680 nH
1008HS-681
|
628 nH
|
A
|
|
680 nH
20% Murata
LQH3NR68M00
|
706 nH
|
A
|
|
680 nH
5% TDK
NL322522T-R68J-3
|
669 nH
|
A
|
|
1 μH
10% TDK
MLF3216A-1R0K000
|
987 nH
|
Ls 1.00## μH 100kHz
Ls 1.049 μH 10kHz
+14.8%
|
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1 μH
20% Panasonic
3225 ELJ-FA1R0MF
|
1.038 μH
|
A
|
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1 μH
20% SE
2520 CIG22H1R0MNE
|
1.014 μH
|
Ls 1.162 μH 10kHz
+12.4%
|
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1 μH
3216 BEAD
|
1.014 μH
|
|
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2.2 μH
20% Murata
LQH3NR2R2M04
|
2.333 μH
|
A
|
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2.7μH 5% AOBA
SWI1008FT2R7J-KY
|
Measured by pressing on the flute because it is not possible to measure due to severe corrosion
2.773 μH
|
|
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3.3 μH
5% TDK
NL252018T-3R3J
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3.228 μH
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Ls 3.370 μH 10kHz
+4.7%
|
|
4.7 μH
5% TDK
MLF453232T-4R7J
|
4.368 μH
|
A
|
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4.7 μH
20% Murata
LQH3N4R7M04
|
4.588 μH
|
A
|
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8.2 μH
5% Panasonic
ELJFC8R2JF
|
8.193 μH
|
|
|
10 μH
20% Murata
LQH3N100M04
|
10.27 μH
|
A
|
|
10 μH
10% TDK
MLF2012E-100KT000
|
9.943 μH
|
A
|
|
47 μH
10% TDK
ML322522T-470K
|
45.50 μH
|
A
|
|
56 μH
20% Murata
LQH3N560M04
|
56.10 μH
|
A
|
|
100 μH
5% TAIYO
LEM2520T-101J
|
101.7 μH
|
A
|
|
100 μH
5% TDK
NL322522T-101J
|
99.93 μH
|
A
|
|
100 μH
10% Murata
LQH3C101M04
|
98.98 μH
|
A
|
|
220 μH
10% TDK
NLC453232T-221K
|
220.3 μH
|
Ls 224.6# μH 100kHz
+2.3%
|
|
330 μH
10% Murata
LQH3C331K04
|
328.0 μH
|
Ls 325.9# μH 100kHz
+1.2%
|
|
680 μH SMD
680 μH
Although it is small, it has a large number of windings, so the parasitic capacitance is large, and the effect on the resonance frequency is large.
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Lx Mode 676.0 μH
The more turns an SMD inductor has, the greater its parasitic capacitance.
Large L Mode 666.6 μH
|
661.2x μH -1.4%
Ls 664.## μH 10kHz -1.1%
|
|
1 mH
10% Panasonic
ELJ-FB102KF 4532
|
1.068 μH Lx Nomal mode
1.061 μH (More accurate values) Large L mode
|
Ls 1.0550 mH 100kHz -0.5%
??? 30kHz
Ls 1.0709 mH 10kHz +0.9%
|
|
1 mH
SMD 30mA 40Ω
1 mH 5% TDK
NL453232T-102J 4532
Because the volume is small and the parasitic capacity is not large, there is a difference of about 0.3%, but the value measured in Large L Mode is more accurate.
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Lx Mode 1.020 mH
Large L Mode 1.017 mH
|
Ls 1.0352 mH 100kHz+0.9%
Ls 1.0788 mH 10kHz +0.9%
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