| Allicdata Part #: | 732-7225-2-ND |
| Manufacturer Part#: |
74404041033 |
| Price: | $ 0.41 |
| Product Category: | Inductors, Coils, Chokes |
| Manufacturer: | Wurth Electronics Inc. |
| Short Description: | FIXED IND 3.3UH 1.75A 69 MOHM |
| More Detail: | 3.3µH Shielded Wirewound Inductor 1.75A 69 mOhm No... |
| DataSheet: |  74404041033 Datasheet/PDF |
| Quantity: | 4500 |
| 4500 +: | $ 0.37422 |
Specifications
| DC Resistance (DCR): | 69 mOhm |
| Height - Seated (Max): | 0.047" (1.20mm) |
| Size / Dimension: | 0.157" L x 0.157" W (4.00mm x 4.00mm) |
| Supplier Device Package: | -- |
| Package / Case: | Nonstandard |
| Mounting Type: | Surface Mount |
| Inductance Frequency - Test: | 100kHz |
| Operating Temperature: | -40°C ~ 125°C |
| Ratings: | -- |
| Frequency - Self Resonant: | 78MHz |
| Q @ Freq: | -- |
| Series: | WE-LQS |
| Shielding: | Shielded |
| Current - Saturation: | 2.1A |
| Current Rating: | 1.75A |
| Tolerance: | ±20% |
| Inductance: | 3.3µH |
| Material - Core: | -- |
| Type: | Wirewound |
| Part Status: | Active |
| Packaging: | Tape & Reel (TR) |
Description
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- Introduction:
The 74404041033 is a fixed inductor. It is a passive two-terminal electrical component which typically consists of an insulated wire or coil wound around a core with a ferrous performance. It is used to store energy in the form of electric current and magnetic field, and they can act as filters, buffers or resonators in various electronic circuits. - Application Field:
Inductors are among the most common components used in low frequency analog electronic circuits. They can be found in many different types of applications such as rectifiers, voltage regulators, power supplies, and motor control circuits. Additionally, they are often used in RF applications such as antennas, transmitters and receivers. - Working Principle:
The 74404041033 consists of an insulated wire or coil, wound around a core composed of a ferrous performance such as iron or ferrite. When current passes through the coil, it creates a magnetic field. This magnetic field carries energy which can then be stored in the inductor.
During this process, the inductor will experience a certain degree of resistance. This resistance is known as inductive reactance and is measured in ohms. The inductive reactance of an inductor is inversely proportional to the amount of current flowing through it. As the current increases, the inductive reactance will decrease, and vice versa.
Additionally, the inductor will also experience an increase in voltage as the current increases. This phenomenon is known as "voltage across an inductor". This voltage will increase as the current increases, and vice versa.
The specific data is subject to PDF, and the above content is for reference
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