Allicdata Part #: | IR02BH1R2J-ND |
Manufacturer Part#: |
IR02BH1R2J |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IR-2 1.2 5% B08 |
More Detail: | 1.2µH Unshielded Inductor 590mA 180 mOhm Max Axia... |
DataSheet: | IR02BH1R2J Datasheet/PDF |
Quantity: | 1000 |
1 +: | 0.00000 |
Q @ Freq: | 25 @ 7.9MHz |
Height - Seated (Max): | -- |
Size / Dimension: | 0.120" Dia x 0.260" L (3.02mm x 6.60mm) |
Supplier Device Package: | Axial |
Package / Case: | Axial |
Mounting Type: | Through Hole |
Features: | -- |
Inductance Frequency - Test: | 7.9MHz |
Operating Temperature: | -55°C ~ 105°C |
Ratings: | -- |
Frequency - Self Resonant: | 150MHz |
Series: | IR |
DC Resistance (DCR): | 180 mOhm Max |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 590mA |
Tolerance: | ±5% |
Inductance: | 1.2µH |
Material - Core: | Iron |
Type: | -- |
Part Status: | Obsolete |
Packaging: | -- |
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Fixed inductors are electronic components which are designed to store electrical energy in the form of a magnetic field. IR02BH1R2J is a type of fixed inductor made of a non-magnetic core, windings and magnetic shunt. It is typically used in power supplies, DC/DC converters, DC-to-AC inverters, and many other applications.
The IR02BH1R2J inductor works based on Faraday’s law of induction. When a conductor is exposed to an alternating current, a voltage is induced in the conductor as the field around it fluctuates. This induced field then generates a magnetic field around the inductor as these voltage and magnetic flux interact. This magnetic flux creates a current flow in the opposite direction of the alternating current. This is called self-inductance or inductive reactance.
The IR02BH1R2J inductor can also store energy electromagnetically in two ways. First, when an AC current flows through it, the magnetic flux between the core and windings builds up and stores energy. This energy is released when the current stops flowing – a process called “inductance”. Secondly, the IR02BH1R2J inductor has a voltage drop that is inversely proportional to the rate at which the current changes. This is called “magnetic hysteresis”.
The most common applications for an IR02BH1R2J fixed inductor are in DC-to-DC converters, AC-to-DC power supplies, and power inverter applications. Its primary functions in such applications include providing continuous electrical current in the form of a DC voltage. Other uses include providing additional current spikes to devices such as motors and lights, providing boost voltages to electronic components, and ripple filtering.
The IR02BH1R2J inductor features a non-magnetic core, windings and a magnetic shunt, providing a low-impedance solution for inductive applications. Its copper winding provides a low total inductance, allowing for efficient current transfer from one part of the circuit to another. The windings can be designed to have a broad range of inductances, allowing the inductor to be customized for various applications.
The IR02BH1R2J is designed with a very high saturation current rating, allowing it to handle extremely high current levels without compromising its operating efficiency. Additionally, its magnetic shunt is able to reduce the total inductance in certain load conditions, providing a fast operation with low EMI or noise. The inductor can also be used in high-frequency switching applications due to its high-frequency characteristic.
In conclusion, the IR02BH1R2J is a type of fixed inductor commonly used in a variety of applications, such as DC-to-DC converters, AC-to-DC power supplies, and power inverters. It works based on Faraday’s law of induction, and features a non-magnetic core, windings and a magnetic shunt, providing a low-impedance solution for inductive applications. Its saturation current rating is very high, making it suitable for use in high current applications, and its high-frequency characteristic makes it suitable for high-frequency switching applications.
The specific data is subject to PDF, and the above content is for reference
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IR02BH101K | Vishay Dale | 0.0 $ | 1000 | IR-2 100 10% B08100H Unsh... |
IR02BH102K | Vishay Dale | 0.0 $ | 1000 | IR-2 1K 10% B081mH Unshie... |
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IR02BH151K | Vishay Dale | 0.0 $ | 1000 | IR-2 150 10% B08150H Unsh... |
IR02BH180K | Vishay Dale | 0.0 $ | 1000 | IR-2 18 10% B0818H Unshie... |
IR02BH181K | Vishay Dale | 0.0 $ | 1000 | IR-2 180 10% B08180H Unsh... |
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IR02BH1R0K | Vishay Dale | 0.0 $ | 1000 | IR-2 1 10% B081H Unshield... |
IR02BH1R2F | Vishay Dale | 0.0 $ | 1000 | IR-2 1.2 1% B081.2H Unshi... |
IR02BH1R2J | Vishay Dale | 0.0 $ | 1000 | IR-2 1.2 5% B081.2H Unshi... |
IR02BH1R2K | Vishay Dale | 0.0 $ | 1000 | IR-2 1.2 10% B081.2H Unsh... |
IR02BH1R5F | Vishay Dale | 0.0 $ | 1000 | IR-2 1.5 1% B081.5H Unshi... |
IR02BH1R5H | Vishay Dale | 0.0 $ | 1000 | IR-2 1.5 3% B081.5H Unshi... |
IR02BH1R5J | Vishay Dale | 0.0 $ | 1000 | IR-2 1.5 5% B081.5H Unshi... |
IR02BH1R5K | Vishay Dale | 0.0 $ | 1000 | IR-2 1.5 10% B081.5H Unsh... |
IR02BH1R8F | Vishay Dale | 0.0 $ | 1000 | IR-2 1.8 1% B081.8H Unshi... |
IR02BH1R8K | Vishay Dale | 0.0 $ | 1000 | IR-2 1.8 10% B081.8H Unsh... |
IR02BH220F | Vishay Dale | 0.0 $ | 1000 | IR-2 22 1% B0822H Unshiel... |
IR02BH220J | Vishay Dale | 0.0 $ | 1000 | IR-2 22 5% B0822H Unshiel... |
IR02BH220K | Vishay Dale | 0.0 $ | 1000 | IR-2 22 10% B0822H Unshie... |
IR02BH221K | Vishay Dale | 0.0 $ | 1000 | IR-2 220 10% B08220H Unsh... |
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IR02BH270K | Vishay Dale | 0.0 $ | 1000 | IR-2 27 10% B0827H Unshie... |
IR02BH271K | Vishay Dale | 0.0 $ | 1000 | IR-2 270 10% B08270H Unsh... |
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IR02BH2R7K | Vishay Dale | 0.0 $ | 1000 | IR-2 2.7 10% B082.7H Unsh... |
IR02BH330K | Vishay Dale | 0.0 $ | 1000 | IR-2 33 10% B0833H Unshie... |
IR02BH331K | Vishay Dale | 0.0 $ | 1000 | IR-2 330 10% B08330H Unsh... |
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FIXED IND 10UH 590MA 350 MOHM10H Unshiel...
FIXED IND 22NH 1.4A 70 MOHM SMD22nH Unsh...
FIXED IND 13NH 600MA SMD13nH Unshielded ...
FIXED IND 680UH 210MA 4.6 OHM680H Unshie...
FIXED IND 470UH 1.3A 280 MOHM TH470H Uns...
FIXED IND 8.2UH 165MA 2.2 OHM TH8.2H Uns...