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Murata Electronics LQH43NN152J03L — Inductors & Chokes

Murata LQH43NN152J03L Drum Core Inductor, 1.5 mH, 40 mA

MPNLQH43NN152J03L
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Murata Electronics LQH43 series, Drum Core Wirewound Inductor, LQH43NN152J03L, 1.5 mH, ±5%, 40 mA, 37 Ohm DCR, 1812 (4532 Metric), Unshielded, Ferrite Core.

$0.2818Ref. price · indicative, final on quote
Sourced new & surplus through independent channelsAuthenticity-screened · ESD-safe packingListing updated Aug 2026

Specifications

LQH43NN152J03L specifications
ParameterValue
TypeDrum Core, Wirewound
SeriesLQH43
MountingSurface Mount
Current rating40 mA
Frequency - self resonant1.6MHz
Inductance frequency - test1 kHz
Operating temperature-40°C ~ 105°C
Material - coreFerrite
Size (Dimension)0.177\" L x 0.126\" W (4.50mm x 3.20mm)
Height - seated0.110\" (2.80mm)
PackageTape & Reel (TR) Cut Tape (CT)
Q @ freq40 @ 252kHz
ShieldingUnshielded
Tolerance±5%
Inductance1.5 mH
Case1812 (4532 Metric)
DC resistance37Ohm Max

Product details

1.5 mH wirewound inductor for filtering and energy storage

The Murata LQH43NN152J03L is a drum core, wirewound inductor in the LQH43 series, rated 1.5 mH ±5% with a 40 mA DC current rating. The 37 Ohm maximum DCR sets the I²R loss floor — at 40 mA the self-heating is about 59 mW, negligible for most filter stages, but the DCR matters for series-pass applications where the voltage drop across the inductor must stay within the rail budget. The unshielded ferrite core construction means the magnetic field extends beyond the component body — keep sensitive traces or low-level analog circuits at least one part-width away to avoid coupling. The 1.6 MHz self-resonant frequency (SRF) is the upper bound for useful inductance; above SRF the part behaves capacitively, so it suits DC-DC converter output filters and EMI suppression below 1 MHz.

Q factor and frequency response for tuned circuits

A Q factor of 40 at 252 kHz tells you the inductor's reactance-to-resistance ratio at that test frequency — high enough for resonant tank circuits in LC oscillators or bandpass filters where selectivity matters. Below 252 kHz the Q drops as the core losses increase; above it the winding AC resistance rises with skin effect, so the peak Q sits near the test point. The inductance is tested at 1 kHz, a standard low-frequency reference point. At the SRF (1.6 MHz) the effective inductance has already rolled off; for a filter designed at 100 kHz, expect the actual inductance to be within a few percent of the 1.5 mH nominal, but always verify with the impedance curve from the full datasheet if the operating frequency approaches 500 kHz.