Coilcraft, Inc. Datasheets for Inductors, Coils, and Chokes
Inductors coils and chokes are passive components that are designed to resist changes in current and store energy in the form of a magnetic field.
Inductors, Coils, and Chokes: Learn more
| Product Name | Notes |
|---|---|
| Automotive Audio Bus (A2B®) by Analog Devices transmits audio and control data in vehicles, reducing wiring complexity and improving sound quality. Our 1210uT inductors filter high-frequency... | |
| Coilcraft 1008PS Series shielded power inductors offer a unique construction that achieves exceptionally high self resonant frequencies (SRFs). Full magnetic shielding assures the lowest possible EMI. Higher SRF series High... | |
| Coilcraft 1111SQ Series square air core inductors have extremely high Q factors and very tight inductance tolerances, making them suitable for narrowband RF amplifier matching and tuning applications. As their... | |
| Coilcraft 1515SQ, 2222SQ, 2929SQ Series square air core inductors have extremely high Q factors and very tight inductance tolerances, making them suitable for narrowband RF amplifier matching and tuning applications. | |
| Coilcraft 1812FS (4532) Series wirewound ferrite beads provide high performance in transmit and receive filters. They are magnetically shielded to minimize EMI and have low DC resistance for minimal insertion... | |
| Coilcraft 1812FS Series shielded power inductors offer a unique construction that achieves exceptionally high self resonant frequencies (SRFs). Full magnetic shielding assures the lowest possible EMI. 5% tolerance parts in... | |
| Our 1008LS Series wirewound chip inductors have a ferrite-ceramic core construction that gives higher current handling and lower DCR in an 1008 (2520) chip size. Inductance values range from 1... | |
| Our 1008LS Series wirewound ferrite beads have a ferrite core construction that achieves high current handing and low DCR. Impedance ranges from 64 Ohms to 7500 Ohms at 10 MHz,... | |
| Our 1206CS Series wirewound chip inductors come in a wide range of values and have exceptionally high Q factors compared to non-wirewound inductors. The ceramic construction gives the highest possible... | |
| Our 1206USB Series was designed for common mode noise suppression in high-speed differential signal lines (USB2.0, IEEE1394, and LVDS) for up to 2.7 GHz differential mode 3 dB cutoff frequency. | |
| Our 1210CAN Series filters a broad frequency range of common mode noise with 50% lower DCR and higher current handling than other CANbus chokes in the market. They are designed... | |
| Our 132-xxSM Series Maxi Spring™ air core inductors have exceptionaly high Q factors and very tight inductance tolerances, making them suitable for narrowband RF amplifier matching and tuning applications. As... | |
| Our 1508/2508 Series low-profile Mini Spring™ air core inductors are AEC-Q200 qualified and provide exceptionally high Q over a wide frequency range, while being less than 2/3 the height of... | |
| Our 1812CAN Series filters a broad frequency range of common mode noise with 50% lower DCR and higher current handling than other CANbus chokes in the market. They are designed... | |
| Our 1812CS Series of wirewound ceramic chip inductors have exceptionally high Q and excellent current handling compared to non-wirewound inductors of the same size. The ceramic construction withstands high peak... | |
| Our 1812FS Series is a unique magnetically shielded chip inductor designed for filtering. The low-DCR inductors achieve high performance in transmit and receive applications. Inductance values cover a wide range... | |
| Our 1812LS Series wirewound chip inductors have a ferrite-ceramic core construction that gives excellent current handling and low DCR in an 1812 (4532) chip size. They are offered in a... | |
| Our 1812LS Series wirewound ferrite beads have a ferrite core construction that achieves high current handing and low DCR. Impedance ranges from 770 Ohms to 191 kOhms at 10 MHz,... | |
| Our VS high-current, high-power air core inductors can handle up to 57 Amps with no core loss. Their size results in excellent Q factors – up to 230 at 400... | |
| RF // Air-Core-Inductors // 0906-1606 // 1606-10 | |
| RF // Air-Core-Inductors // 0906-1606 // 1606-6 | |
| RF // Air-Core-Inductors // 0906-1606 // 1606-7 | |
| RF // Air-Core-Inductors // 0906-1606 // 1606-8 | |
| RF // Air-Core-Inductors // 0906-1606 // 1606-9 | |
| RF // Air-Core-Inductors // 1010VS-1212VS-2014VS // 1212VS-111 | |
| RF // Air-Core-Inductors // 1010VS-1212VS-2014VS // 1212VS-22N | |
| RF // Air-Core-Inductors // 1010VS-1212VS-2014VS // 1212VS-42N | |
| RF // Air-Core-Inductors // 1010VS-1212VS-2014VS // 1212VS-66N | |
| RF // Air-Core-Inductors // 1010VS-1212VS-2014VS // 1212VS-90N | |
| RF // Tunable-RF-Inductors // Uni10 // 142-01J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-02J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-03J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-04J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-05J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-06J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-07J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-08J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-09J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 142-10J08SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-09J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-10J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-11J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-12J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-13J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-14J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-15J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-16J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-17J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-18J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-19J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 143-20J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-01J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-02J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-03J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-04J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-05J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-06J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-07J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-08J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-09J12SL | |
| RF // Tunable-RF-Inductors // Uni10 // 144-10J12SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-01A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-02A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-03A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-04A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-05A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-06A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-07A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-08A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-09A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-10A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 164-11A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-00A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-01A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-02A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-03A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-04A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-05A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-06A06SL | |
| RF // Tunable-RF-Inductors // Uni5 // 165-07A06SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-01J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-02J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-03J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-04J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-05J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-06J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-07J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-08J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-09J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 146-10J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-01J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-02J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-03J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-04J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-05J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-06J08SL | |
| RF // Tunable-RF-Inductors // Uni7 // 150-07J08SL | |
| The 1210ETH common mode choke series is optimized for Single Pair Ethernet (SPE), with dedicated values for 100BASE-T1 and 10BASE-T1S. Supporting PoDL for power and data over the same pair,... | |
| With a maximum height of only 0.045 inches, our 1008HT Series has the lowest profile of all our 1008-sized chip inductors. Available in a wide range of standard values, these... | |
| 0.300″ / 7,6 height is ideal for low profile applications Windings are precision molded into plastic for mechanical and electrical stability Threaded Carbonyl J core with a slotted socket Extremely... | |
| Inductance values from 2.5 nH to 150 nH (tolerances as low as 2%) Tight tolerance can eliminate circuit tuning Acrylic jacket provides a flat top for pick and place Exceptionally... | |
| Optimized for AEC-Q200 power over coax (PoC) applications Small size to reduce board area of overall system solutions AEC-Q200 Grade 1 (−40°C to +125°C) High impedance (≥ 1kOhm) maintained over... | |
| Optimized for AEC-Q200 power over coax (PoC) applications Small size to reduce board area of overall system solutions Board area is only 3.87mm 2 AEC-Q200 Grade 1 (−40°C to +125°C)... | |
| Small size to minimize the board area of overall system solutions, with a low profile of only 2.5 mm High impedance (≥ 1kOhm) maintained over a wide band frequency range... | |
| Small size to reduce board area of overall system solutions, with a low profile of only 2.0 mm High impedance (≥ 1kOhm) maintained over a wide band frequency range to... | |
| These high Q parts have a 5% inductance tolerance Precision insert molding ensures constant winding pitch RoHS-compliant. Matte tin over copper (132-01 through 132-06), Tin-silver over copper (132-07 through 132-20). | |
| Two balanced inductors in a single package Magnetically shielded Only 0.150 inch (3.81 mm) high Optimized for xDSL filtering applications Custom versions available RoHS Compliant. 260°C compatible. Gold over nickel... | |
| Windings are precision molded into plastic for mechanical and electrical stability Tuning is done by means of a threaded powdered iron core with a hex socket Optional plated brass shield... | |
| Windings are precision molded into plastic for mechanical and electrical stability Tuning is done by means of an aluminum core Optional plated brass shield cans with solderable tabs provide integral... | |
| Windings are precision molded into polypropylene for mechanical and electrical stability Tuning is done by means of a threaded powdered iron core with a slotted socket Optional plated brass shield... |
| << Prev | Next >> |