Allicdata Part #: | 1944R-09F-ND |
Manufacturer Part#: |
1944R-09F |
Price: | $ 3.12 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | API Delevan Inc. |
Short Description: | FIXED IND 470NH 2A 70 MOHM TH |
More Detail: | 470nH Unshielded Molded Inductor 2A 70 mOhm Max Ax... |
DataSheet: | 1944R-09F Datasheet/PDF |
Quantity: | 1000 |
2500 +: | $ 2.80110 |
Mounting Type: | Through Hole |
Package / Case: | Axial |
Supplier Device Package: | -- |
Size / Dimension: | 0.193" Dia x 0.447" L (4.90mm x 11.35mm) |
Height - Seated (Max): | -- |
Series: | 1944R |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Type: | Molded |
Material - Core: | Phenolic |
Inductance: | 470nH |
Tolerance: | ±1% |
Current Rating: | 2A |
Current - Saturation: | -- |
Shielding: | Unshielded |
DC Resistance (DCR): | 70 mOhm Max |
Q @ Freq: | 55 @ 25MHz |
Frequency - Self Resonant: | 288MHz |
Ratings: | -- |
Operating Temperature: | -55°C ~ 125°C |
Inductance Frequency - Test: | 25MHz |
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 electronic components that play an important role in electronic circuits. They provide inductance and also act as transformers, offering impedance, attenuation, frequency transformation, and even voltage division for an electronic circuit. The 1944R-09F is an example of one of these fixed inductors. This component has a wide range of applications and particular properties that make it a reliable and popular choice for many circuit designs.
The 1944R-09F has an inductance range from 2.7 µH to 4.7 µH, making it ideal for use in low-noise, low-power analog circuits. It is also suited for use in digital circuits, since it provides high-current drives, fast rise and fall times, and excellent protection from electrostatic discharge. The 1944R-09F is also capable of handling up to 350 mA of current with no sign of degradation in performance.
The 1944R-09F also offers a high degree of reliability, due to its inductance stability and its low core loss characteristics. The core material is made of a sintered ferrite and features dual opposite spinning windings. This winding construction ensures uniform magnetic field distribution and, as a result, allows for better current and voltage regulation.
The application of the 1944R-09F can be divided into two main areas. In the first area, the 1944R-09F is used as a filter inductor. In this role, it is used to reduce interference signals in analog and digital circuits. The inductor works by limiting the amount of high-frequency noise that is present in the signal. As a result, the signal is filtered from the noise, making for a higher quality of audio.
The second area of application is for power-line noise suppression. The 1944R-09F works by creating an inductive reactance which helps lower the level of line noise. This helps to keep signals from leaking into other circuits and ensures that the audio being produced by the system is of high quality. This is especially important in digital circuitry, as the interference of line noise can cause resolution loss or even damage to the circuitry.
The 1944R-09F is also used in a wide variety of applications ranging from medical equipment, to cellular phones, to audio systems. Its reliability and limited size make it an ideal candidate for many device designs. It can even be used in RF applications, where it offers a low-loss response in the 10 MHz to 50 MHz range. This makes the 1944R-09F a great choice for both high-speed and low-speed circuits.
The working principle of the 1944R-09F is simple but effective. It contains two coils, which are connected in parallel. When a current is passed through the two coils, an electromagnetic field is created which induces a counter-current in the second coil. This counter-current will attempt to cancel out the current in the first coil, resulting in an inductive reactance that reduces the amount of current that is able to pass through the circuit.
The 1944R-09F is a reliable and popular choice for many electronics circuits due to its wide range of applications, inductance range, and current rating. Its dual coil design promotes an even magnetic field distribution, while its high current rating makes it suitable for controlling the power flow in various audio systems. Its working principle works by inductive reactance, which helps to reduce line noise and regulate the current within a circuit. All of these qualities make the 1944R-09F an ideal choice for many of today’s electronics applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
19440031150 | HARTING | 53.08 $ | 6 | 3A INOX (STAINLESS STEEL)... |
19440035425 | HARTING | 31.19 $ | 3 | HAN INOX 3A COVER FOR FEM... |
19440035422 | HARTING | 28.6 $ | 2 | HAN INOX 3A COVER FOR MAL... |
19440035426 | HARTING | 29.25 $ | 2 | HAN INOX 3A COVER FOR MAL... |
19440035421 | HARTING | 33.43 $ | 4 | HAN INOX 3A COVER FOR FEM... |
19443105421 | HARTING | 76.36 $ | 4 | PROTECT COVER HAN-INOX FO... |
19440031643 | HARTING | 43.83 $ | 1000 | CONN HOOD SIDE ENTRY SZ3A... |
19440031250 | HARTING | 49.25 $ | 10 | CONN BASE SIDE ENTRY SZ3A... |
19440031750 | HARTING | 51.7 $ | 6 | HAN-INOX 3A-HCC-M20 |
19443100303 | HARTING | 155.93 $ | 2 | CONN BASE BOTTOM ENTRY SZ... |
19440030301 | HARTING | 29.35 $ | 2 | CONN BASE BOTTOM ENTRY SZ... |
19440031640 | HARTING | 45.07 $ | 7 | CONN HOOD SIDE ENTRY SZ3A... |
19440035427 | HARTING | 0.0 $ | 1000 | 3A INOX (STAINLESS STEEL)... |
19440035428 | HARTING | 0.0 $ | 1000 | 3A INOX (STAINLESS STEEL)... |
19440035429 | HARTING | 0.0 $ | 1000 | HAN-INOX 3A-AK FKM SEAL |
19440005083 | HARTING | 52.17 $ | 1000 | M25 STAINLESS STEEL CABLE... |
19440005084 | HARTING | 57.32 $ | 1000 | GABLE GLAND M20 6-13 MM P... |
19443105423 | HARTING | 80.17 $ | 1000 | 10B INOX (STAINLESS STEEL... |
19440005085 | HARTING | 89.19 $ | 1000 | M40 STAINLESS STEEL CABLE... |
19440005082 | HARTING | 39.61 $ | 25 | GABLE GLAND M20 13-21 MM ... |
19443105422 | HARTING | 111.92 $ | 3 | PROTECT COVER HAN-INOX FO... |
19440009902 | HARTING | 1.33 $ | 148 | HAN INOX 10B GASKET |
19443100757 | HARTING | 121.02 $ | 1000 | CONN HOOD CPLNG BOTTOM SZ... |
19440031440 | HARTING | 38.78 $ | 19 | CONN HOOD TOP ENTRY SZ3A ... |
19440031443 | HARTING | 40.36 $ | 13 | CONN HOOD TOP ENTRY SZ3A ... |
19440030801 | HARTING | 44.2 $ | 1000 | CONN BASE SIDE ENTRY SZ3A |
19443100305 | HARTING | 88.36 $ | 5 | CONN BASE BOTTOM ENTRY SZ... |
19443100447 | HARTING | 112.91 $ | 2 | CONN HOOD TOP ENTRY SZ10B... |
19443100547 | HARTING | 113.31 $ | 5 | CONN HOOD SIDE ENTRY SZ10... |
88-194440-87 | Amphenol Ind... | 554.77 $ | 1000 | CONN ADAPTER 7P-7P F-M PN... |
10-194428-22 | Amphenol Ind... | 603.37 $ | 1000 | CONN ADAPTER 6P-6P F-M PN... |
10-194418-22 | Amphenol Ind... | 627.58 $ | 1000 | CONN ADAPTER 3P-3P F-M PN... |
88-194440-82 | Amphenol Ind... | 648.0 $ | 1000 | CONN ADAPTER 62P-62P F-M ... |
10-194428-51 | Amphenol Ind... | 671.29 $ | 1000 | CONN ADAPTER 12P-12P F-M ... |
10-194422-18 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 8P-8P F-M PN... |
10-194422-9 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 3P-3P F-M PN... |
88-194432-017 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 4P-4P F-M PN... |
10-194428-66 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 16P-16P F-M ... |
88-194440-56 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 85P-85P F-M ... |
88-194428-12 | Amphenol Ind... | 0.69 $ | 1000 | CONN ADAPTER 26P-26P F-M ... |
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...