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Murata Electronics LQH32MN1R5K23L — Inductors & Chokes

Murata LQH32MN1R5K23L 1.5 µH Unshielded Inductor, 400 mA

MPNLQH32MN1R5K23L
Active

Murata Electronics LQH32 series, Drum Core Wirewound, Unshielded, 1.5 µH, ±10%, 400 mA, 600mOhm Max, 1210 (3225 Metric), Surface Mount.

$0.3000Ref. price · indicative, final on quote
Sourced new & surplus through independent channelsAuthenticity-screened · ESD-safe packingListing updated Aug 2026

Specifications

LQH32MN1R5K23L specifications
ParameterValue
TypeDrum Core, Wirewound
SeriesLQH32
MountingSurface Mount
Current rating400 mA
Frequency - self resonant75MHz
Inductance frequency - test1 MHz
Operating temperature-40°C ~ 85°C
Material - coreFerrite
Size (Dimension)0.126\" L x 0.098\" W (3.20mm x 2.50mm)
Height - seated0.087\" (2.20mm)
PackageTape & Reel (TR) Cut Tape (CT)
Q @ freq20 @ 1MHz
ShieldingUnshielded
Tolerance±10%
Inductance1.5 µH
CaseNonstandard
DC resistance600mOhm Max

Product details

1.5 µH, 400 mA — the DC bias ceiling and the self-resonant floor

The Murata LQH32MN1R5K23L is a 1.5 µH drum-core wirewound inductor in the LQH32 series, built on a ferrite core. The 400 mA current rating is the DC bias limit — push past it and the inductance collapses as the core saturates, so the real-world ceiling for a power rail filter is that 400 mA, not the peak current the load draws in a transient. The self-resonant frequency sits at 75 MHz, which sets the usable bandwidth: below that the part behaves as an inductor; above it the parasitic capacitance dominates and the impedance turns capacitive. For a 1.5 µH value, 75 MHz SRF is typical of a wirewound construction at this footprint — the winding capacitance and core losses define the roll-off.

Unshielded construction — placement matters

This is an unshielded inductor. The magnetic field radiates from the drum core, so adjacent traces, ground pours, and especially other magnetics within a few millimetres will couple. For a 1.5 µH part in a 1210 footprint, keep a keep-out zone of at least one part width around it unless the layout is in a shielded compartment or the coupling is benign (e.g., the inductor is in a low-impedance filter and the neighbour is a DC line). The unshielded construction means the magnetic field extends beyond the package boundary, so a shielded sibling (LQH32P series, same footprint) would be the drop-in replacement if EMI coupling becomes an issue during EMC pre-compliance.

Because the part is active and the LQH32 series is a long-running Murata line, the risk of an abrupt EOL notice is low for the foreseeable future. The 1210 footprint and 1.5 µH value are common enough that a second-source parametric match (same inductance, current rating, DCR, and SRF) exists from other manufacturers if a dual-source BOM hedge is required.

Frequently asked questions

What is the self-resonant frequency of LQH32MN1R5K23L and why does it matter?

The self-resonant frequency is 75 MHz. Above this frequency the inductor behaves capacitively, so the part is usable as an inductor only below 75 MHz. For a 1.5 µH value in a DC-DC converter switching at, say, 2 MHz, the SRF is far above the switching frequency and the inductor maintains its inductive impedance.

What is the DC resistance of LQH32MN1R5K23L and how does it affect efficiency?

The maximum DCR is 600 mΩ. At the rated 400 mA DC current, the I²R loss is 96 mW. In a low-power rail (e.g., 3.3 V at 400 mA, ~1.3 W output), this represents about 7 % loss in the inductor alone — acceptable for many designs but worth derating if the ambient temperature is near the 85°C upper limit.