Allicdata Part #: | 36541E6N8JTDG-ND |
Manufacturer Part#: |
36541E6N8JTDG |
Price: | $ 0.13 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | FIXED IND 6.8NH 1.5A 55 MOHM |
More Detail: | 6.8nH Unshielded Wirewound Inductor 1.5A 55 mOhm M... |
DataSheet: | 36541E6N8JTDG Datasheet/PDF |
Quantity: | 1000 |
2000 +: | $ 0.11747 |
DC Resistance (DCR): | 55 mOhm Max |
Height - Seated (Max): | 0.024" (0.60mm) |
Size / Dimension: | 0.045" L x 0.028" W (1.15mm x 0.70mm) |
Package / Case: | Nonstandard |
Mounting Type: | Surface Mount |
Inductance Frequency - Test: | 250MHz |
Operating Temperature: | -40°C ~ 125°C |
Ratings: | -- |
Frequency - Self Resonant: | 5.8GHz |
Q @ Freq: | -- |
Series: | 3650, Sigma Inductors |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 1.5A |
Tolerance: | ±5% |
Inductance: | 6.8nH |
Material - Core: | -- |
Type: | Wirewound |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
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Fixed inductors are used to store electric charge or energy for a short time. They are typically found in circuits where the flow of current must be controlled or regulated. The 36541E6N8JTDG is a type of fixed inductor, which works by creating an electromagnetic field in a core material and then passing the current through it. This creates a magnetic field around the inductor, which resists changes to the current. If the current is increased, the inductor will oppose it, leading to a drop in voltage. This is known as inductive reactance.
The 36541E6N8JTDG inductor is composed of a core material such as ferrite or powdered metal, a coil winding, and an external casing. The coil winding is typically very thin copper wire. The inductor’s working principle is based on Faraday’s law of induction, which states that when a changing magnetic field is passed through a coil, a voltage is induced in the coil. For the 36541E6N8JTDG inductor, this means that when an electric current passes through the coil, a magnetic field is created in the core material. This magnetic field in turn induces a voltage in the coil, which opposes the current. If the current is increased, the voltage increases as well, leading to a drop in voltage.
The 36541E6N8JTDG inductor is typically used in circulatory circuits such as power supplies, filters, and transformers. It can also be used in antennas, where it is used to tune the antenna and match the radio frequency band. Additionally, the 36541E6N8JTDG inductor can be used in switching power supply circuits to control the voltage of the power supply. It is also commonly used to control the speed of motors or other electrical components.
The 36541E6N8JTDG inductor has a number of advantages over other types of inductors. It is small in size, making it a great choice for applications where space is limited. It also has a low inductance, meaning that it can handle higher frequency signals without suffering from distortion. Additionally, the 36541E6N8JTDG inductor does not suffer from fading, making it reliable over long periods of time. It is also very reliable in terms of its current and voltage ratings, making it a great choice for a variety of applications.
The 36541E6N8JTDG inductor is a reliable and versatile component that is used in a variety of applications. It has a low inductance and is small in size, making it perfect for applications where space is limited. Additionally, its reliable current and voltage rating make it a great choice for power supplies, filters, and transformers. Finally, its ability to resist fading ensures that it remains reliable over long periods of time. For these reasons, the 36541E6N8JTDG inductor is an excellent choice for anyone looking for an effective solution for their circuit needs.
The specific data is subject to PDF, and the above content is for reference
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