Allicdata Part #: | H4P1K27DZA-ND |
Manufacturer Part#: |
H4P1K27DZA |
Price: | $ 0.35 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 1.27K OHM 1W 0.5% AXIAL |
More Detail: | 1.27 kOhms ±0.5% 1W Through Hole Resistor Axial Pu... |
DataSheet: | H4P1K27DZA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.31880 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 1.27 kOhms |
Tolerance: | ±0.5% |
Power (Watts): | 1W |
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: | 0.146" 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 commonly used in a wide variety of electronic circuits. The H4P1K27DZA is a Through Hole Resistor that is designed for high-frequency applications. This resistor is commonly found in power supplies, switching regulators, and high-power automotive and industrial applications.
The H4P1K27DZA is a metal-oxide resistor and is available in a variety of sizes, which allow them to be used in various applications that require higher resistance ratings. These resistors are made up of two layers; the first layer is a ceramic layer to provide insulation and the second is a metal-oxide layer that reduces the contact resistance between the two layers. The ceramic material also offers high temperature resistance and better reliability compared to other metal-oxide based resistors.
The H4P1K27DZA has a high power dissipation rating, which means that it can handle more wattage than other resistors. This allows it to be used in high-power applications where conventional resistors may not be able to withstand the high power demands. It also has a very low failure rate and is extremely reliable.
The working principle of the H4P1K27DZA is simple. When a current is applied to the resistor, it causes electrons to flow through the layers of the resistor, creating a resistance. This resistance creates a voltage drop between the two electrodes, which is used to limit the current flowing through the resistor. By adjusting the current applied to the resistor, the resistor can be finely tuned to meet the needs of the application.
The H4P1K27DZA Through Hole Resistor is ideal for a wide range of applications, ranging from automotive to industrial. It is a dependable and reliable resistor that is capable of handling high power demands and is ideal for high-frequency applications. With a low failure rate and high power dissipation rating, the H4P1K27DZA Through Hole Resistor is a great choice for any electronic circuit.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
H4P150KDZA | TE Connectiv... | 0.35 $ | 1000 | RES 150K OHM 1W 0.5% AXIA... |
H4P15KDZA | TE Connectiv... | 0.35 $ | 1000 | RES 15.0K OHM 1W 0.5% AXI... |
H4P1K5DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.50K OHM 1W 0.5% AXI... |
H4P1K8DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.80K OHM 1W 0.5% AXI... |
H4P10RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 10.0 OHM 1W 0.5% AXIA... |
H4P10R5DZA | TE Connectiv... | 0.35 $ | 1000 | RES 10.5 OHM 1W 0.5% AXIA... |
H4P11RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 11.0 OHM 1W 0.5% AXIA... |
H4P11R5DZA | TE Connectiv... | 0.35 $ | 1000 | RES 11.5 OHM 1W 0.5% AXIA... |
H4P12R1DZA | TE Connectiv... | 0.35 $ | 1000 | RES 12.1 OHM 1W 0.5% AXIA... |
H4P12R7DZA | TE Connectiv... | 0.35 $ | 1000 | RES 12.7 OHM 1W 0.5% AXIA... |
H4P13R3DZA | TE Connectiv... | 0.35 $ | 1000 | RES 13.3 OHM 1W 0.5% AXIA... |
H4P14RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 14.0 OHM 1W 0.5% AXIA... |
H4P14R7DZA | TE Connectiv... | 0.35 $ | 1000 | RES 14.7 OHM 1W 0.5% AXIA... |
H4P15R4DZA | TE Connectiv... | 0.35 $ | 1000 | RES 15.4 OHM 1W 0.5% AXIA... |
H4P16R2DZA | TE Connectiv... | 0.35 $ | 1000 | RES 16.2 OHM 1W 0.5% AXIA... |
H4P16R9DZA | TE Connectiv... | 0.35 $ | 1000 | RES 16.9 OHM 1W 0.5% AXIA... |
H4P17R8DZA | TE Connectiv... | 0.35 $ | 1000 | RES 17.8 OHM 1W 0.5% AXIA... |
H4P18R7DZA | TE Connectiv... | 0.35 $ | 1000 | RES 18.7 OHM 1W 0.5% AXIA... |
H4P19R6DZA | TE Connectiv... | 0.35 $ | 1000 | RES 19.6 OHM 1W 0.5% AXIA... |
H4P100RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 100 OHM 1W 0.5% AXIAL... |
H4P105RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 105 OHM 1W 0.5% AXIAL... |
H4P115RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 115 OHM 1W 0.5% AXIAL... |
H4P121RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 121 OHM 1W 0.5% AXIAL... |
H4P127RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 127 OHM 1W 0.5% AXIAL... |
H4P133RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 133 OHM 1W 0.5% AXIAL... |
H4P140RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 140 OHM 1W 0.5% AXIAL... |
H4P147RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 147 OHM 1W 0.5% AXIAL... |
H4P154RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 154 OHM 1W 0.5% AXIAL... |
H4P162RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 162 OHM 1W 0.5% AXIAL... |
H4P169RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 169 OHM 1W 0.5% AXIAL... |
H4P178RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 178 OHM 1W 0.5% AXIAL... |
H4P187RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 187 OHM 1W 0.5% AXIAL... |
H4P196RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 196 OHM 1W 0.5% AXIAL... |
H4P1K0DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.00K OHM 1W 0.5% AXI... |
H4P1K05DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.05K OHM 1W 0.5% AXI... |
H4P1K1DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.10K OHM 1W 0.5% AXI... |
H4P1K15DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.15K OHM 1W 0.5% AXI... |
H4P1K21DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.21K OHM 1W 0.5% AXI... |
H4P1K27DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.27K OHM 1W 0.5% AXI... |
H4P1K33DZA | TE Connectiv... | 0.35 $ | 1000 | RES 1.33K OHM 1W 0.5% AXI... |
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