Allicdata Part #: | H8390RFZA-ND |
Manufacturer Part#: |
H8390RFZA |
Price: | $ 0.20 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 390 OHM 1/4W 1% AXIAL |
More Detail: | 390 Ohms ±1% 0.25W, 1/4W Through Hole Resistor Axi... |
DataSheet: | H8390RFZA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.18059 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 390 Ohms |
Tolerance: | ±1% |
Power (Watts): | 0.25W, 1/4W |
Composition: | Metal Film |
Features: | Pulse Withstanding |
Temperature Coefficient: | ±100ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.098" Dia x 0.283" L (2.50mm x 7.20mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through Hole Resistors are essential components in electronic circuits; they are used to control the amount of current flowing between the terminals of a component or circuit. The H8390RFZA is a special form of through hole resistor that is specifically designed for high frequency applications. This type of resistor is particularly used in RF signal processing due to its low inductive reactance.
The H8390RFZA works by using non-inductive winding in a slender shape. This allows for a better magnetic permeability as compared to other types of resistors. The winding is formed by enamel-coated fine wire strands and is often soldered directly to the circuit board. The winding has a number of turns that determine its resistance; as different turns are used the resistance can vary dramatically.
The H8390RFZA has a wide range of applications which include wireless communication, transmission control system, and frequency response control. Additionally, it is used in the manufacturing of electronic enclosures, aerial masts, amplifiers, and many other commercial consumer products. Typically, this type of resistor is used in association with antenna systems, RF filter circuits, and dual axis antennas. It is also frequently added to oscillators, receivers, and other wireless systems as a means of providing attenuation and control of the signal strength.
The principle working of the H8390RFZA is based on the principle of Faraday\'s law. This law states that a current will be induced in a conductor when an external magnetic field is applied. The magnetic field surrounding the resistor is produced by the electrical energy which is produced when current passes through it. The resulting current flowing through the resistor is known as eddy currents, which in turn creates a secondary electromagnetic field.
In order to reduce the eddy currents, special designs are used in the construction of the resistor. The winding is designed in such a way as to create an open-ended magnetic field by decreasing the number of turns. In this way, the width of the magnetic field is also reduced. The reduction in number of turns also reduces the current that is produced by the resistor, thus reducing interference and providing a more stable operation. This is a key factor that makes the H8390RFZA so suitable for use in RF applications.
In conclusion, the H8390RFZA is a through-hole resistor that is widely used in RF applications due to its unique properties. It works on the principle of Faraday\'s law, and utilizes a winding design to reduce eddy currents and resulting magnetic fields. The result is a resistor with reduced interference and better stability.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
ECW-H8393HA | Panasonic El... | 0.46 $ | 1377 | CAP FILM 0.039UF 3% 800VD... |
H839R2BCA | TE Connectiv... | 0.35 $ | 1000 | RES 39.2 OHM 1/4W 0.1% AX... |
H8392RBCA | TE Connectiv... | 0.35 $ | 1000 | RES 392 OHM 1/4W 0.1% AXI... |
H839K2BCA | TE Connectiv... | 0.35 $ | 1000 | RES 39.2K OHM 1/4W 0.1% A... |
H8392KBCA | TE Connectiv... | 0.35 $ | 1000 | RES 392K OHM 1/4W 0.1% AX... |
H8392KBDA | TE Connectiv... | 0.39 $ | 1000 | RES 392K OHM 1/4W 0.1% AX... |
H839KBDA | TE Connectiv... | 0.39 $ | 1000 | RES 39.0K OHM 1/4W 0.1% A... |
H8390RBYA | TE Connectiv... | 0.4 $ | 1000 | RES 390 OHM 1/4W 0.1% AXI... |
H839RBYA | TE Connectiv... | 0.4 $ | 1000 | RES 39.0 OHM 1/4W 0.1% AX... |
H839R2BZA | TE Connectiv... | 0.31 $ | 1000 | RES 39.2 OHM 1/4W 0.1% AX... |
H8392RBZA | TE Connectiv... | 0.31 $ | 1000 | RES 392 OHM 1/4W 0.1% AXI... |
H839K2BZA | TE Connectiv... | 0.31 $ | 1000 | RES 39.2K OHM 1/4W 0.1% A... |
H8392KBZA | TE Connectiv... | 0.31 $ | 1000 | RES 392K OHM 1/4W 0.1% AX... |
H839R2BDA | TE Connectiv... | 0.39 $ | 1000 | RES 39.2 OHM 1/4W 0.1% AX... |
H8392RBDA | TE Connectiv... | 0.39 $ | 1000 | RES 392 OHM 1/4W 0.1% AXI... |
H839K2BDA | TE Connectiv... | 0.39 $ | 1000 | RES 39.2K OHM 1/4W 0.1% A... |
H839R2BYA | TE Connectiv... | 0.4 $ | 1000 | RES 39.2 OHM 1/4W 0.1% AX... |
H8392RBYA | TE Connectiv... | 0.4 $ | 1000 | RES 392 OHM 1/4W 0.1% AXI... |
H839K2BYA | TE Connectiv... | 0.4 $ | 1000 | RES 39.2K OHM 1/4W 0.1% A... |
H8392KBYA | TE Connectiv... | 0.4 $ | 1000 | RES 392K OHM 1/4W 0.1% AX... |
ECW-H8392JL | Panasonic El... | 0.0 $ | 1000 | CAP FILM 3900PF 5% 800VDC... |
ECW-H8393JL | Panasonic El... | 0.0 $ | 1000 | CAP FILM 0.039UF 5% 800VD... |
ECW-H8392HL | Panasonic El... | 0.0 $ | 1000 | CAP FILM 3900PF 3% 800VDC... |
ECW-H8393HL | Panasonic El... | 0.0 $ | 1000 | CAP FILM 0.039UF 3% 800VD... |
H839RFZA | TE Connectiv... | 0.2 $ | 1000 | RES 39.0 OHM 1/4W 1% AXIA... |
H8390RFZA | TE Connectiv... | 0.2 $ | 1000 | RES 390 OHM 1/4W 1% AXIAL... |
H839KFZA | TE Connectiv... | 0.2 $ | 1000 | RES 39.0K OHM 1/4W 1% AXI... |
H8390KFZA | TE Connectiv... | 0.2 $ | 1000 | RES 390K OHM 1/4W 1% AXIA... |
H839RFYA | TE Connectiv... | 0.27 $ | 1000 | RES 39.0 OHM 1/4W 1% AXIA... |
H8390RFYA | TE Connectiv... | 0.27 $ | 1000 | RES 390 OHM 1/4W 1% AXIAL... |
H839KFYA | TE Connectiv... | 0.27 $ | 1000 | RES 39.0K OHM 1/4W 1% AXI... |
H8390KFYA | TE Connectiv... | 0.27 $ | 1000 | RES 390K OHM 1/4W 1% AXIA... |
H839RFDA | TE Connectiv... | 0.25 $ | 1000 | RES 39.0 OHM 1/4W 1% AXIA... |
H8390RFDA | TE Connectiv... | 0.25 $ | 1000 | RES 390 OHM 1/4W 1% AXIAL... |
H839KFDA | TE Connectiv... | 0.25 $ | 1000 | RES 39.0K OHM 1/4W 1% AXI... |
H8390KFDA | TE Connectiv... | 0.25 $ | 1000 | RES 390K OHM 1/4W 1% AXIA... |
H839RFCA | TE Connectiv... | 0.23 $ | 1000 | RES 39.0 OHM 1/4W 1% AXIA... |
H8390RFCA | TE Connectiv... | 0.23 $ | 1000 | RES 390 OHM 1/4W 1% AXIAL... |
H839KFCA | TE Connectiv... | 0.23 $ | 1000 | RES 39.0K OHM 1/4W 1% AXI... |
H8390KFCA | TE Connectiv... | 0.23 $ | 1000 | RES 390K OHM 1/4W 1% AXIA... |
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