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High Current Power Inductors

High Current Power Inductors

High Current Power Inductors

·For DC/DC converter applications.

·Low DC resistance and high DC current capability.

·Magnetically shielded with low magnetic flux leakage.

·Wide band has good impedance characteristics, which can effectively 

suppress high frequency clutter.

·It is widely used in power supplier, VTR, OA equipment, LCD television set, 

Notebook, Portable communication equipment, etc.

·RoHS compliant.

High Current Power Inductors
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CLB

  • Type Photos Dimension Inductance Range µH Rated Current-A pdf
    L mm W mm H mm Lmin Lmax Isat-min Isat-max Irms-max Irms-min Download
    CLB070605 CLB070605 7.00 6.60 5.50 90.00 150.00 28.00 50.00 41.00 41.00
    CLB100705 CLB100705 10.50 7.20 5.20 0.008 0.22 26.00 64.00 41.00 41.00
    CLB100706 CLB100706 10.50 7.20 6.50 0.085 0.22 28.00 70.00 41.00 41.00
    CLB100707 CLB100707 10.50 7.20 7.50 0.12 0.47 18.00 56.00 41.00 41.00
    CLB706035W CLB706035W 7.00 7.80 6.00 -- -- -- -- -- --
    CLB855630W CLB855630W 8.50 8.90 5.60 -- -- -- -- -- --
  • -

    CEPH

  • Type Photos Dimension Inductance Range µH Rated Current-A pdf
    L mm W mm H mm Lmin Lmax Isat-min Isat-max Irms-max Irms-min Download
    CEPH1205 CEPH1205 12.90 12.90 5.60 0.35 10.00 5.00 35.00 7.60 18.50
    CEPH1209 CEPH1209 12.60 12.70 9.00 10.00 47.00 3.60 10.00 6.20 8.30
    CEPH1304 CEPH1304 13.90 13.90 4.90 0.30 8.00 6.10 32.00 6.50 18.20
  • -

    CPQH

  • Type Photos Dimension Inductance Range µH Rated Current-A pdf
    L mm W mm H mm Lmin Lmax Isat-min Isat-max Irms-max Irms-min Download
    CPQH2013 HCPQ2013 21.50 21.50 14.00 0.70 47.00 8.40 98.50 13.20 39.40
    CPQH2016 HCPQ2016 21.50 21.50 17.00 1.50 47.00 8.70 73.70 15.00 31.10
    CPQH2615 HCPQ2615 27.50 29.00 15.50 1.00 47.00 4.40 210.00 31.90 34.40
    CPQH2617 HCPQ2617 27.50 29.00 17.50 1.00 47.00 7.10 250.00 31.00 32.50
    CPQH2620 HCPQ2620 27.50 29.00 20.50 3.30 100.00 4.90 132.00 4.00 28.00
    CPQH2625 HCPQ2625 27.50 29.00 25.50 6.80 220.00 2.80 96.90 19.50 22.80