Allicdata Part #: | H414RBDA-ND |
Manufacturer Part#: |
H414RBDA |
Price: | $ 0.51 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 14.0 OHM 1/2W 0.1% AXIAL |
More Detail: | 14 Ohms ±0.1% 0.5W, 1/2W Through Hole Resistor Axi... |
DataSheet: | H414RBDA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.46438 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 14 Ohms |
Tolerance: | ±0.1% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Metal Film |
Features: | Pulse Withstanding |
Temperature Coefficient: | ±25ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.146" Dia x 0.394" L (3.70mm x 10.00mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through Hole Resistors, H414RBDA, are an important component of electrical circuits. They are used to control and reduce electrical current in order to ensure the safe operation of a circuit. H414RBDA is one of the most commonly used type of resistors in circuit designs. It is a four-terminal, pre-wired component that comes pre-packaged with a variety of pin configurations.
The H414RBDA has a wide range of applications in the field of electronics, such as in signal processing, audio amplifier circuits, and in automotive applications. One of the main advantages of using H414RBDA is that it has a low resistance value (1.5 ohms), making it suitable for applications that require the transmission of high frequency signals.
The working principle of H414RBDA is quite simple. When an electrical current passes through the resistor, some of the energy is dissipated as heat. The amount of energy that is dissipated from the resistor is proportional to the resistance value of the resistor. The higher the resistor value, the more energy is dissipated. Therefore, by adjusting the resistance value of the resistor, we can control the amount of energy that is dissipated from the resistor.
H414RBDA is an effective way of controlling electric current and is commonly used in a wide variety of applications. It has a low resistance value which makes it ideal for high frequency applications, and it is available in a variety of pin configurations, making it suitable for any circuit design. By understanding the working principle of H414RBDA, circuit designers can effectively control the flow of electric current in their applications and achieve their desired performance.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
H4140KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 140K OHM 1/2W 0.1% AX... |
H4143KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 143K OHM 1/2W 0.1% AX... |
H4147KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 147K OHM 1/2W 0.1% AX... |
H414RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.0 OHM 1/2W 0.1% AX... |
H414R3BDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.3 OHM 1/2W 0.1% AX... |
H414R7BDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.7 OHM 1/2W 0.1% AX... |
H4140RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 140 OHM 1/2W 0.1% AXI... |
H4143RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 143 OHM 1/2W 0.1% AXI... |
H4147RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 147 OHM 1/2W 0.1% AXI... |
H414KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.0K OHM 1/2W 0.1% A... |
H414K3BDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.3K OHM 1/2W 0.1% A... |
H414K7BDA | TE Connectiv... | 0.51 $ | 1000 | RES 14.7K OHM 1/2W 0.1% A... |
H414RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.0 OHM 1/2W 0.1% AX... |
H414R3BYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.3 OHM 1/2W 0.1% AX... |
H414R7BYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.7 OHM 1/2W 0.1% AX... |
H4140RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 140 OHM 1/2W 0.1% AXI... |
H4143RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 143 OHM 1/2W 0.1% AXI... |
H4147RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 147 OHM 1/2W 0.1% AXI... |
H414KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.0K OHM 1/2W 0.1% A... |
H414K3BYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.3K OHM 1/2W 0.1% A... |
H414K7BYA | TE Connectiv... | 0.57 $ | 1000 | RES 14.7K OHM 1/2W 0.1% A... |
H4140KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 140K OHM 1/2W 0.1% AX... |
H4143KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 143K OHM 1/2W 0.1% AX... |
H4147KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 147K OHM 1/2W 0.1% AX... |
H414RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 14.0 OHM 1/2W 0.5% AX... |
H414R7DYA | TE Connectiv... | 0.46 $ | 1000 | RES 14.7 OHM 1/2W 0.5% AX... |
H4140RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 140 OHM 1/2W 0.5% AXI... |
H4147RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 147 OHM 1/2W 0.5% AXI... |
H414KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 14.0K OHM 1/2W 0.5% A... |
H414K7DYA | TE Connectiv... | 0.46 $ | 1000 | RES 14.7K OHM 1/2W 0.5% A... |
H4140KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 140K OHM 1/2W 0.5% AX... |
H4147KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 147K OHM 1/2W 0.5% AX... |
H414RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 14.0 OHM 1/2W 0.1% AX... |
H414R7BCA | TE Connectiv... | 0.48 $ | 1000 | RES 14.7 OHM 1/2W 0.1% AX... |
H4140RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 140 OHM 1/2W 0.1% AXI... |
H4143RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 143 OHM 1/2W 0.1% AXI... |
H4147RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 147 OHM 1/2W 0.1% AXI... |
H414KBCA | TE Connectiv... | 0.48 $ | 1000 | RES 14.0K OHM 1/2W 0.1% A... |
H414K3BCA | TE Connectiv... | 0.48 $ | 1000 | RES 14.3K OHM 1/2W 0.1% A... |
H414K7BCA | TE Connectiv... | 0.48 $ | 1000 | RES 14.7K OHM 1/2W 0.1% A... |
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RES 24.9 OHM 1/4W 1% AXIAL24.9 Ohms 1% 0...
RES 2.8 OHM 3W 0.5% WW AXIAL2.8 Ohms 0.5...
RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...
RES 340 OHM 1W 1% WW AXIAL340 Ohms 1% 1W...