
Allicdata Part #: | IMS05WDRU470J40-ND |
Manufacturer Part#: |
IMS05WDRU470J40 |
Price: | $ 0.00 |
Product Category: | Inductors, Coils, Chokes |
Manufacturer: | Vishay Dale |
Short Description: | IMS-5WD-40 47 5% R36 |
More Detail: | 47µH Shielded Inductor 420mA 1.8 Ohm Max Axial |
DataSheet: | ![]() |
Quantity: | 1000 |
1 +: | 0.00000 |
Q @ Freq: | 46 @ 2.5MHz |
Height - Seated (Max): | -- |
Size / Dimension: | 0.164" Dia x 0.450" L (4.17mm x 11.43mm) |
Supplier Device Package: | Axial |
Package / Case: | Axial |
Mounting Type: | Through Hole |
Features: | -- |
Inductance Frequency - Test: | 2.5MHz |
Operating Temperature: | -55°C ~ 125°C |
Ratings: | -- |
Frequency - Self Resonant: | 26MHz |
Series: | IMS-5WD-40 |
DC Resistance (DCR): | 1.8 Ohm Max |
Shielding: | Shielded |
Current - Saturation: | 177mA |
Current Rating: | 420mA |
Tolerance: | ±10% |
Inductance: | 47µH |
Material - Core: | Ferrite |
Type: | -- |
Part Status: | Obsolete |
Packaging: | -- |
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Fixed inductors are used in electrical engineering, mainly in the application of electronics and automotive systems. The IMS05WDRU470J40 is an example of this type of inductor, which is an SMD power inductor with a high rated current of 4.7 A. This type of inductor is an important component in many types of circuits and can be used in a variety of ways.
The IMS05WDRU470J40 has a core material of nanocrystallite-based amorphous material, which gives it a wide inductance range and makes it suitable for working in a wide range of temperatures and current rates. The inductance of this inductor varies with the rate of current, so it can be used in many applications. The inductance range of this inductor is from 0.2 to 4.5 mH.
The IMS05WDRU470J40 can be used in a variety of applications, including switched-mode power supplies, DC/DC converters, and Buck, Boost, and SEPIC converters. In switched-mode power supplies, the IMS05WDRU470J40 can be used to filter the current waveforms and reduce ripple and noise, helping to prevent the output voltage from fluctuating due to load variations. This type of inductor is also commonly used in DC/DC converters where the energy transfer between two DC circuits must be accurately controlled.
The working principle of the IMS05WDRU470J40 is based on the theory of inductance, which states that a magnetic field is produced when a current is passed through a conductor. This magnetic field then induces a voltage in any adjacent conductors due to the changing current rates, as explained by Faraday’s law of induction. This voltage will increase in proportion to the rate of change in the current flow.
Since the magnetic field of the IMS05WDRU470J40 is proportional to the current rate, the size of the inductor increases at higher current rates. This allows the inductor to absorb or store more energy and be used in applications with higher levels of power density. The inductance value of the IMS05WDRU470J40 is also adjustable, which makes it very versatile and allows for fine-tuning in different applications.
In conclusion, the IMS05WDRU470J40 is a fixed inductor that is used in many electronics and automotive applications. This type of inductor works on the principle of induction, as explained by Faraday’s law of induction. Its wide inductance range and adjustable inductance value make it suitable for a variety of applications, including switched-mode power supplies, DC/DC converters, and Buck, Boost, and SEPIC converters.
The specific data is subject to PDF, and the above content is for reference
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IMS02EB6R8K | Vishay Dale | 0.0 $ | 1000 | IMS-2 6.8 10% EB E36.8H S... |
IMS02WWDBH1R5K40 | Vishay Dale | 0.0 $ | 1000 | IMS-2WWD-40 1.5 10% B081.... |
IMS05BH150K | Vishay Dale | 0.0 $ | 1000 | IMS-5 15 10% B0815H Shiel... |
IMS05EB392K | Vishay Dale | 0.0 $ | 1000 | IMS-5 3.9K 10% EB E23.9mH... |
IMS05SH101J | Vishay Dale | 0.0 $ | 1000 | IMS-5 100 5% RJ1100H Shie... |
IMS05RU3R9K | Vishay Dale | 0.0 $ | 1000 | IMS-5 3.9 10% R363.9H Shi... |
IMS05WDBH471K40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 470 10% B08470... |
IMS05WDRU151J40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 150 5% R36150H... |
IMS02BHR56K | Vishay Dale | 0.0 $ | 1000 | IMS-2 .56 10% B08560nH Sh... |
IMS02WWDEB100K40 | Vishay Dale | 0.0 $ | 1000 | IMS-2WWD-40 10 10% EB E21... |
IMS02WWDM9R18K40 | Vishay Dale | 0.0 $ | 1000 | IMS-2WWD-40 .18 10% M2918... |
IMS05BH120K | Vishay Dale | 0.0 $ | 1000 | IMS-5 12 10% B0812H Shiel... |
IMS05BH390K | Vishay Dale | 0.0 $ | 1000 | IMS-5 39 10% B0839H Shiel... |
IMS05RUR15J | Vishay Dale | 0.0 $ | 1000 | IMS-5 .15 5% R36150nH Shi... |
IMS05SH561K | Vishay Dale | 0.0 $ | 1000 | IMS-5 560 10% RJ1560H Shi... |
IMS05ST3R3K | Vishay Dale | 0.0 $ | 1000 | IMS-5 3.3 10% RJ43.3H Shi... |
IMS05WDEBR22K40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 .22 10% EB E22... |
IMS05WDSH272K40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 2.7K 10% RJ12.... |
IMS02SH1R8J | Vishay Dale | 0.0 $ | 1000 | IMS-2 1.8 5% RJ11.8H Shie... |
IMS02STR15K | Vishay Dale | 0.0 $ | 1000 | IMS-2 .15 10% RJ4150nH Sh... |
IMS05BH1R8K | Vishay Dale | 0.0 $ | 1000 | IMS-5 1.8 10% B081.8H Shi... |
IMS05BH330K | Vishay Dale | 0.0 $ | 1000 | IMS-5 33 10% B0833H Shiel... |
IMS05BH682J | Vishay Dale | 0.0 $ | 1000 | IMS-5 6.8K 5% B086.8mH Sh... |
IMS05SH330K | Vishay Dale | 0.0 $ | 1000 | IMS-5 33 10% RJ133H Shiel... |
IMS05WDBH221J40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 220 5% B08220H... |
IMS05WDST470K40 | Vishay Dale | 0.0 $ | 1000 | IMS-5WD-40 47 10% RJ447H ... |
IMS05EB2R2K | Vishay Dale | 0.0 $ | 1000 | FIXED IND 2.2UH 650MA 190... |
IMS02SH270J | Vishay Dale | 0.0 $ | 1000 | IMS-2 27 5% RJ127H Shield... |
IMS02ST1R5K | Vishay Dale | 0.0 $ | 1000 | IMS-2 1.5 10% RJ41.5H Shi... |
IMS02WWDBH271K40 | Vishay Dale | 0.0 $ | 1000 | IMS-2WWD-40 270 10% B0827... |
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...
