
Allicdata Part #: | PL8609NLT-ND |
Manufacturer Part#: |
PL8609NLT |
Price: | $ 3.34 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | PulseR |
Short Description: | IND CPLD 91UH 0.61ADC-LEG PBC |
More Detail: | 91µH Unshielded Toroidal Inductor 1.2A 318 mOhm Ma... |
DataSheet: | ![]() |
Quantity: | 1000 |
300 +: | $ 3.00762 |
DC Resistance (DCR): | 318 mOhm Max |
Height - Seated (Max): | 0.320" (8.12mm) |
Size / Dimension: | 0.625" L x 0.525" W (15.88mm x 13.34mm) |
Supplier Device Package: | -- |
Package / Case: | Nonstandard |
Mounting Type: | Surface Mount |
Features: | -- |
Operating Temperature: | -40°C ~ 130°C |
Ratings: | -- |
Frequency - Self Resonant: | -- |
Q @ Freq: | -- |
Series: | POGO |
Shielding: | Unshielded |
Current - Saturation: | -- |
Current Rating: | 1.2A |
Tolerance: | ±10% |
Inductance: | 91µH |
Material - Core: | -- |
Type: | Toroidal |
Part Status: | Active |
Packaging: | Tape & Reel (TR) |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
Fixed inductors are electrical components that store electrical energy in a magnetic field. PL8609NLT is a type of fixed inductor.
PL8609NLT is a low-profile, wide-operating-temperature-range fixed inductor, specifically designed for automotive electronics applications. This component has the capability of operating in temperatures from -40°C up to 125°C, making it well-suited for a wide range of applications, including automotive powertrain or battery management systems. Furthermore, PL8609NLT is an AEC-Q200 qualified component, meaning it has been tested to meet the automotive standards of quality and reliability.
The construction of PL8609NLT consists of a core base material that is magnetically insulated with a layer of copper foil. In essence, the copper foil prevents the magnetic field from escaping the component, thereby creating a highly efficient inductor. This design further lends itself to the low-profile nature of the part, as the magnetic field remains localized within the device.
The working principle of PL8609NLT is based upon Faraday\'s law, which states that when a current flowing through a conductor is changed, a circulating magnetic flux is generated. This magnetic flux causes the induction of an electromotive force (EMF) in the conductor. This EMF is proportional to the rate of change of flux and is the core of PL8609NLT\'s operation.
PL8609NLT is capable of generating a wide range of magnetic field strengths depending on the current flowing through it. This variation is necessary for a wide range of applications, ranging from providing noise suppression in automotive audio systems to providing powertrain control in complex electronic systems.
Due to its low-profile, wide-operating-temperature-range and AEC-Q200 qualification, PL8609NLT is ideal for a variety of automotive electronics applications. It is capable of generating a wide range of magnetic fields, making it well suited for automotive audio systems and powertrain control systems. Furthermore, its construction of a magnetic core insulated by a copper foil keeps its magnetic field localized, further contributing to its low-profile nature.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
PL8602NLT | PulseR | 3.34 $ | 1000 | IND CPLD 5.5UH 2.60ADC-LE... |
PL8601 | PulseR | 3.71 $ | 1000 | IND CPLD 2.6UH 3.60ADC-LE... |
PL8609NL | PulseR | 3.71 $ | 1000 | IND CPLD 91UH 0.61ADC-LEG... |
PL8607T | PulseR | 3.34 $ | 1000 | IND CPLD 47.6UH .90ADC-LE... |
PL8605NLT | PulseR | 3.34 $ | 1000 | IND CPLD 22.1UH 1.3ADC-LE... |
PL8602NL | PulseR | 3.71 $ | 1000 | IND CPLD 5.5UH 2.60ADC-LE... |
PL8605T | PulseR | 3.34 $ | 1000 | IND CPLD 22.1UH 1.3ADC-LE... |
PL8605NL | PulseR | 3.71 $ | 1000 | IND CPLD 22.1UH 1.3ADC-LE... |
PL8604T | PulseR | 3.34 $ | 1000 | IND CPLD 15.7UH 1.6ADC-LE... |
PL8605 | PulseR | 3.71 $ | 1000 | IND CPLD 22.1UH 1.3ADC-LE... |
PL8608 | PulseR | 3.71 $ | 1000 | IND CPLD 67.5UH .74ADC-LE... |
PL8608NLT | PulseR | 3.34 $ | 1000 | IND CPLD 67.5UH .74ADC-LE... |
PL8601NL | PulseR | 3.71 $ | 1000 | IND CPLD 2.6UH 3.60ADC-LE... |
PL8603NL | PulseR | 3.71 $ | 1000 | IND CPLD 10.4UH 1.9ADC-LE... |
PL8609NLT | PulseR | 3.34 $ | 1000 | IND CPLD 91UH 0.61ADC-LEG... |
PL8607 | PulseR | 3.71 $ | 1000 | IND CPLD 47.6UH .90ADC-LE... |
PL8603 | PulseR | 3.71 $ | 1000 | IND CPLD 10.4UH 1.9ADC-LE... |
PL8609T | PulseR | 3.34 $ | 1000 | IND CPLD 91UH 0.61ADC-LEG... |
PL8604 | PulseR | 3.71 $ | 1000 | IND CPLD 15.7UH 1.6ADC-LE... |
PL8600NLT | PulseR | 3.34 $ | 1000 | IND CPLD 2.2UH 4.15ADC-LE... |
PL8601NLT | PulseR | 3.34 $ | 1000 | IND CPLD 2.6UH 3.60ADC-LE... |
PL8609 | PulseR | 3.71 $ | 1000 | IND CPLD 91UH 0.61ADC-LEG... |
PL8608T | PulseR | 3.34 $ | 1000 | IND CPLD 67.5UH .74ADC-LE... |
PL8603NLT | PulseR | 3.34 $ | 1000 | IND CPLD 10.4UH 1.9ADC-LE... |
PL8601T | PulseR | 3.34 $ | 1000 | IND CPLD 2.6UH 3.60ADC-LE... |
PL8606NLT | PulseR | 3.34 $ | 1000 | IND CPLD 32.8UH 1.1ADC-LE... |
PL8604NLT | PulseR | 3.34 $ | 1000 | IND CPLD 15.7UH 1.6ADC-LE... |
PL8604NL | PulseR | 3.71 $ | 1000 | IND CPLD 15.7UH 1.6ADC-LE... |
PL8607NLT | PulseR | 3.34 $ | 1000 | IND CPLD 47.6UH .90ADC-LE... |
PL8606NL | PulseR | 3.71 $ | 1000 | IND CPLD 32.8UH 1.1ADC-LE... |
PL8600T | PulseR | 3.34 $ | 1000 | IND CPLD 2.2UH 4.15ADC-LE... |
PL8603T | PulseR | 3.34 $ | 1000 | IND CPLD 10.4UH 1.9ADC-LE... |
PL8607NL | PulseR | 3.71 $ | 1000 | IND CPLD 47.6UH .90ADC-LE... |
PL8602T | PulseR | 3.34 $ | 1000 | IND CPLD 5.5UH 2.60ADC-LE... |
PL8606T | PulseR | 3.34 $ | 1000 | IND CPLD 32.8UH 1.1ADC-LE... |
PL8600NL | PulseR | 3.71 $ | 1000 | IND CPLD 2.2UH 4.15ADC-LE... |
PL8608NL | PulseR | 3.71 $ | 1000 | IND CPLD 67.5UH .74ADC-LE... |
PL8602 | PulseR | 3.71 $ | 1000 | IND CPLD 5.5UH 2.60ADC-LE... |
PL8606 | PulseR | 3.71 $ | 1000 | IND CPLD 32.8UH 1.1ADC-LE... |
PL8600 | PulseR | 3.71 $ | 1000 | IND CPLD 2.2UH 4.15ADC-LE... |
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