Allicdata Part #: | H411RBYA-ND |
Manufacturer Part#: |
H411RBYA |
Price: | $ 0.57 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 11.0 OHM 1/2W 0.1% AXIAL |
More Detail: | 11 Ohms ±0.1% 0.5W, 1/2W Through Hole Resistor Axi... |
DataSheet: | H411RBYA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.51966 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 11 Ohms |
Tolerance: | ±0.1% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Metal Film |
Features: | Pulse Withstanding |
Temperature Coefficient: | ±15ppm/°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 are generally used in electronic systems to limit electrical flow. This could be done by increasing resistance, or by reducing current flow. H411RBYA is a type of through-hole resistor that is made of high-precision hot-molded silver wire wrapped on a ceramic core. This type of resistor is mainly used in aerospace and military applications, usually when higher temperatures or better performance is required.
The H411RBYA through-hole resistor works on the principle of increasing the resistance of the electric current as it passes through the resistor. This is achieved by using hot-molded silver wire to increase the electrical resistance of the resistor. Hot-molded silver wire is much more electrically resistant than traditional wire, making H411RBYA suitable for high temperature and high-performance applications. The increased electrical resistance provided by the hot-molded silver wire prevents electrical current from flowing uninterruptedly.
The way that H411RBYA works is simple. As the electrical current passes through the resistor, it encounters the hot-molded silver wire which increases its resistance. The current keeps flowing, but its rate of flow is reduced, thus decreasing the current’s overall power. This is achieved by the wire’s resistance to the electrical current, and by the ceramic core holding the resistor in place.
This resistor is suitable for use in a variety of applications, especially in aerospace and military applications. This is due to the increased resistance provided by the hot-molded silver wire and the better performance of the core material, which resists temperatures up to 400 degrees Celsius. The resistor is also able to handle high power applications as it has a high power handling capacity.
The H411RBYA is an excellent choice for those who need a more reliable and resilient resistor that can handle high temperatures and powerful applications. Not only does this resistor provide excellent performance, but it also offers the added benefit of being a high-precision component that helps to guarantee a reliable and consistent performance.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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H4110KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 110K OHM 1/2W 0.1% AX... |
H4113KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 113K OHM 1/2W 0.1% AX... |
H4115KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 115K OHM 1/2W 0.1% AX... |
H4118KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 118K OHM 1/2W 0.1% AX... |
H411RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.0 OHM 1/2W 0.1% AX... |
H411R3BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.3 OHM 1/2W 0.1% AX... |
H411R5BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.5 OHM 1/2W 0.1% AX... |
H411R8BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.8 OHM 1/2W 0.1% AX... |
H4110RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 110 OHM 1/2W 0.1% AXI... |
H4113RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 113 OHM 1/2W 0.1% AXI... |
H4115RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 115 OHM 1/2W 0.1% AXI... |
H4118RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 118 OHM 1/2W 0.1% AXI... |
H411KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.0K OHM 1/2W 0.1% A... |
H411K3BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.3K OHM 1/2W 0.1% A... |
H411K5BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.5K OHM 1/2W 0.1% A... |
H411K8BDA | TE Connectiv... | 0.51 $ | 1000 | RES 11.8K OHM 1/2W 0.1% A... |
H411RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.0 OHM 1/2W 0.1% AX... |
H411R3BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.3 OHM 1/2W 0.1% AX... |
H411R5BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.5 OHM 1/2W 0.1% AX... |
H411R8BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.8 OHM 1/2W 0.1% AX... |
H4110RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 110 OHM 1/2W 0.1% AXI... |
H4113RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 113 OHM 1/2W 0.1% AXI... |
H4115RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 115 OHM 1/2W 0.1% AXI... |
H4118RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 118 OHM 1/2W 0.1% AXI... |
H411KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.0K OHM 1/2W 0.1% A... |
H411K3BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.3K OHM 1/2W 0.1% A... |
H411K5BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.5K OHM 1/2W 0.1% A... |
H411K8BYA | TE Connectiv... | 0.57 $ | 1000 | RES 11.8K OHM 1/2W 0.1% A... |
H4110KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 110K OHM 1/2W 0.1% AX... |
H4113KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 113K OHM 1/2W 0.1% AX... |
H4115KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 115K OHM 1/2W 0.1% AX... |
H4118KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 118K OHM 1/2W 0.1% AX... |
H411RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 11.0 OHM 1/2W 0.5% AX... |
H411R5DYA | TE Connectiv... | 0.46 $ | 1000 | RES 11.5 OHM 1/2W 0.5% AX... |
H4110RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 110 OHM 1/2W 0.5% AXI... |
H4115RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 115 OHM 1/2W 0.5% AXI... |
H411KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 11.0K OHM 1/2W 0.5% A... |
H411K5DYA | TE Connectiv... | 0.46 $ | 1000 | RES 11.5K OHM 1/2W 0.5% A... |
H4110KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 110K OHM 1/2W 0.5% AX... |
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