| Brand Name: | Hoan |
| Model Number: | HALA1200503R |
| MOQ: | 10 Pieces |
| Payment Terms: | L/C,D/A,D/P,T/T,Western Union |
Wire diameter is the single most consequential design parameter in a micro air core inductor — and the difference between 0.03mm and 0.05mm is far greater than the numbers suggest. Cross-sectional area scales with the square of diameter: a 0.05mm wire has (50/30)² = 2.78* the copper cross-section of a 0.03mm wire. DC resistance is inversely proportional to cross-sectional area, so the 0.05mm wire has approximately 64% lower DCR. At 400mA, the 0.03mm HALA1200303R is limited to 200mA not by any magnetic constraint (the air core cannot saturate), but by the I²R self-heating of the thinner copper filament. The 0.05mm HALA1200503R doubles the current ceiling — 400mA continuous, with sufficient thermal margin for GaN PA bias networks operating at 28-50V drain with 200-400mA bias current.
The HALA1200503R 17nH ±20% 12-turn air core inductor intentionally trades maximum inductance density (26nH for the 0.03mm version) for current-handling headroom (400mA vs 200mA). With 2.78* the copper cross-section, the thicker wire also produces a slightly wider turn-to-turn pitch that reduces proximity-effect AC resistance at high frequencies. In the 10-20GHz band where skin depth in copper is only 0.46-0.66µm, the current flows exclusively in the conductor surface — and the 0.05mm wire provides more surface area per unit length than the 0.03mm wire, further reducing high-frequency ESR. This is why the HALA1200503R's frequency range extends to 20GHz (vs 18GHz for the 0.03mm version) — the lower AC resistance from the thicker wire preserves Q factor deeper into the K-band.
Parasitic capacitance in an inductor is the enemy of wideband operation. Every adjacent turn pair forms a parasitic capacitor; the total parasitic capacitance degrades SRF, distorts the frequency response, and creates a non-flat passband. The HALA1200503R minimizes this capacitance through three design choices:
The inter-turn insulation in the HALA1200503R is provided by the polyurethane enamel coating on the 0.05mm copper wire. This coating serves three critical functions simultaneously:
Radiation hardness is not achieved through shielding or special processing — it is inherent to the physics of the air-core inductor. The governing equation L = μ₀ * N² * A / l contains only free-space constants (μ₀) and physical geometry (turns N, area A, length l). Total ionizing dose (TID) up to hundreds of kilorads creates no trapped charge because there are no semiconductor junctions. Displacement damage creates no lattice defects that affect inductance because there is no crystal lattice whose properties determine μ. Single-event effects create no current transients because there is no active device to be triggered. The inductor is as radiation-immune as the laws of electromagnetism themselves.
This inherent immunity extends to all harsh-environment conditions: thermal shock (-55°C to +125°C, 1000+ cycles), condensing humidity, salt fog, and low-pressure (high-altitude) operation. The air core has no CTE mismatch to manage, no porous material to absorb moisture, and no volatile compounds to outgas under vacuum. For equipment deployed in environments where repair is difficult or impossible, the HALA1200503R eliminates passive-component degradation as a failure mechanism.
| Parameter | HALA1200503R (0.05mm) | HALA1200303R (0.03mm) |
|---|---|---|
| Inductance | 17nH | 26nH |
| Max Current | 400mA | 200mA |
| Frequency | 2-20GHz | 1.5-18GHz |
| DCR | Lower (~64% reduction) | Higher |
| Best For | PA bias networks, high-current DC feed | Maximum inductance density, space-constrained |
| Parameter | Value | Notes |
|---|---|---|
| Inductance | 17 nH ±20% | @10MHz-20GHz |
| Turns | 12 | Precision helical |
| Wire | 0.05mm enameled Cu | 2.78* cross-section vs 0.03mm |
| ID | 0.30mm | Hollow air core |
| Current | 400mA DC | Continuous, zero saturation |
| Frequency | 2-20GHz | Into K-band microwave |
| Temp | -55°C to +125°C | Full parametric |
This is the most frequent question from engineers comparing the two HALA120 variants. Both have 12 turns, yet the HALA1200503R produces 17nH while the HALA1200303R produces 26nH — a 35% difference. The answer lies in the turn-to-turn pitch. The 0.05mm wire is 67% thicker than the 0.03mm wire, which increases the center-to-center spacing between adjacent turns. This wider pitch reduces the mutual inductive coupling coefficient (k) between turns. In a multi-turn air-core solenoid, the total inductance L = L_self * N² where L_self includes both self-inductance per turn and the mutual coupling between all turn pairs. With wider pitch from the thicker wire, the mutual coupling term decreases, and the total inductance drops from 26nH to 17nH. This is not a manufacturing error — it is an intentional trade-off that buys you 2* the current handling (400mA vs 200mA) and 2GHz of additional high-frequency bandwidth (20GHz vs 18GHz) through reduced AC resistance.
Contact us for evaluation samples, S2P Touchstone data, or to discuss your specific bias network requirements.