Size Dimen­sions L
(mm)
W
(mm)
Fl
(mm)
1010
10 10 8.55
1212
11.5 12 9.1

Characteristics

  • No saturation
  • No core losses
  • Extremely high Q-Factor
  • Ultra low RDC
  • High current capability
  • Inductances from 22 up to 146 nH
  • Operating temperature: -40 °C up to +125 °C

Applications

  • High current DC-DC converters with clocks > 4 MHz
  • RF power amplifiers
  • RF voltage regulators
  • High current RF filters/chokes
  • Power supplies
  • Magnetically-sensitive applications
  • Operating temperature: -40°C up to +125°C

Modelithics Simulation Models

Incorporate this part into your design with Modelithics’ highly accurate measurement-based simulation models. Modelithics libraries are available for Keysight Technologies’ Advanced Design System (ADS), NI/AWR Design Environment/Microwave Office™, Keysight Technologies’ Gensys, ASYSS® HFSS™, Sonnet® and Cadence.

Products

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1010
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Data­sheet
Simu­lation
Downloads
Status
L (nH)
Tol. L
Test Condition L
Qmin.
Test Condition Q
RDC max. (mΩ)
IR (A)
fres (MHz)
Samples
7449152022
22 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 22 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 280 
Q-Factor 100 MHz 
DC Resistance 0.55 mΩ
Rated Current 40 A
Self Resonant Frequency 867 MHz
7449150023
23 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 23 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 191 
Q-Factor 100 MHz 
DC Resistance 1.2 mΩ
Rated Current 30 A
Self Resonant Frequency 867 MHz
7449152042
42 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 42 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 240 
Q-Factor 100 MHz 
DC Resistance 770 mΩ
Rated Current 34 A
Self Resonant Frequency 605 MHz
7449150046
46.5 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 46.5 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 223 
Q-Factor 100 MHz 
DC Resistance 1.62 mΩ
Rated Current 28 A
Self Resonant Frequency 581 MHz
7449152066
66 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 66 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 245 
Q-Factor 100 MHz 
DC Resistance 0.99 mΩ
Rated Current 32 A
Self Resonant Frequency 457 MHz
7449150079
79 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 79 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 184 
Q-Factor 100 MHz 
DC Resistance 2.11 mΩ
Rated Current 23 A
Self Resonant Frequency 422 MHz
7449152090
90 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 90 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 226 
Q-Factor 100 MHz 
DC Resistance 1.21 mΩ
Rated Current 30 A
Self Resonant Frequency 359 MHz
7449150111
111 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 111 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 186 
Q-Factor 100 MHz 
DC Resistance 2.11 mΩ
Rated Current 22 A
Self Resonant Frequency 374 MHz
7449152111
117 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 117 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 211 
Q-Factor 100 MHz 
DC Resistance 1.43 mΩ
Rated Current 32 A
Self Resonant Frequency 345 MHz
7449150146
146 nH, ±20%, 1 MHz
Simu­lation
Status Active i | Production is active. Expected lifetime: >10 years.
Inductance 146 nH
Inductance ±20% 
Inductance 1 MHz 
Q-Factor 163 
Q-Factor 100 MHz 
DC Resistance 3.33 mΩ
Rated Current 19 A
Self Resonant Frequency 332 MHz

Würth Elektronik offers several product series with different construction technology

RF Inductors selection guide

WE-KI SMT Wire Wound Ceramic Inductor
WE-KI SMT Wire Wound Ceramic Inductor
  • Inductance values from 1nH up to 1800nH
  • High Q factor
  • Up to 12.5GHz self resonant frequency
  • Up to ± 2% inductance tolerance
  • High thermal stability
  • Design Kits available for the different sizes
WE-KI HC SMT High Current Wire Wound Ceramic Inductor
WE-KI High Current Wire Wound Ceramic Inductor
  • Inductance values from 1nH up to 390nH
  • Excellent Q factor
  • High current up to 2.3 A
  • ± 2% Inductance Tolerance
  • High thermal stability
  • Design Kit available
WE-MK Multilayer Ceramic SMT Inductor
WE-MK Multilayer Ceramic Inductor
  • Inductance values from 1nH up to 470nH
  • Extremly small size (up to 0201)
  • Up to ±2% (or ±0.1nH) inductance tolerance
  • Robust structure
  • Polarity marking available 
  • Design Kits available for the different sizes
  • High thermal stability
WE-CAIR Air Coil
WE-CAIR Air Core Inductor
  • Inductance values from 1.65nH up to 538nH
  • Extremly high Q factor (Q>100)
  • Very high current up to 4 A
  • High self resonant frequency
  • Design Kit available
  • High thermal stability
WE-TCI Thinfilm Chip Inductor
WE-TCI Thin Film Inductor
  • Inductance values from 1nH up to 27nH
  • High self resonant frequency
  • Tight tolerance of 2 % (1% on request) or ± 0.1
  • Very small size (up to 0201)
WE-RFI Ferrite SMT Inductor
WE-RFI Wire Wound ferrite inductor
  • High inductance values available from 20 nH up to 47 µH
  • Operating temperature:–40 °C to +85 °C
  • Size: 0402 to 1008
  • Design Kit available  

What is the Quality Factor Q?

What is the Quality Factor Q?

The quality factor Q is an essential characteristic parameter and one of the first creterias that every RF engineer should take into account. The Q factor is given either as minimum or as typical value at a defined frequency point. In the case of Würth Elektronik, the Q factor is given as the minimum value in order to guarantee customers a reliable minimum level.

Basically, the Q factor is the ratio between the inductive reactance XL and the losses RS and is an indicator of how ideal an inductor is. For inductors with air or ceramic cores, the resistance RS is mainly due to the resistivity of the conductor in the inductor device. A higher Q factor means less losses in the component.

Self Resonant Frequency

Self Resonant Frequency

Because the winding structure of any coil of wire will exhibit some capacitance, the inductor will serve as a parallel resonant tank circuit with an associated self-resonance frequency (SRF). As with conventional inductors, SRF indicates up to which frequency the inductor behaves as an inductor.

Exactly at the SRF the inductor with its parasitic capacitance behaves as a resonance circuit with an almost infinite high impedance, only circuit losses limit the high value of the impedance. Beyond the SRF the “inductor” behaves like a capacitor

Increasing the inductance and/or the parasitic capacitance lowers the SRF, and vice versa. This is the reason why the higher the inductance value, the lower the SRF.

In case of choke applications in which inductors are used, the best signal blocking occurs shortly below the SRF, where the impedance is very high and thus the attenuation reaches its maximum. For filter or impedance-matching applications, it is more important to have constant inductance in the relevant frequency range, which means the SRF of the inductor should be well above the operating frequency of the circuit.

CM RF Inductors Self Resonant Frequency

Rated Current in high frequency application

Rated Current in high frequency application

The rated current is specified as the maximum DC current (A or mA) that causes a defined temperature rise (i.e. ΔT = 40 K). The temperature rise plus the ambient temperature must not exceed the maximum operating temperature. For high current applications, please select the specific air core inductors: WE-KI HC, WE-ACHC and WE-CAIR.

RF Inductors Rated Current in high frequency application

RF inductors and Antenna Matching

How Antenna Matching works

RF inductors and Antenna Matching

How Antenna Matching works

With the help of the Smith chart, the complex antenna feed point impedance, consisting of resistive and reactive values, can be represented graphically. In a matched antenna, the impedance at the operating frequency is close to the middle of the Smith chart and therefore close to the impedance of 50 Ω. This can be achieved by using RF inductors and RF capacitors. A pi matching network is particularly useful for this purpose, since it can be used flexibly for antenna matching from almost any other impedance. In practice, antenna matching works through iterative steps.

In addition to the WE-MCA Antennas, we offer our customers a development-accompanying antenna service. We support from the antenna selection over the antenna placement up to the antenna matching.

Website: www.we-online.com/antennamatching

E-Mail: antenna.matching@we-online.com

We are also offering an Antenna Matching Design Kit that contains all the components needed for your antenna matching. This Design Kit with order code 748001, contains chip antennas WE-MCA, multilayer ceramic inductors WE-MK size 0402, high frequency chip capacitors WCAP-CSRF in size 0402 and RF coaxial cables WR-CXARY working up to 18 GHz