| Allicdata Part #: | H4P442KDZA-ND |
| Manufacturer Part#: |
H4P442KDZA |
| Price: | $ 0.35 |
| Product Category: | Resistors |
| Manufacturer: | TE Connectivity Passive Product |
| Short Description: | RES 442K OHM 1W 0.5% AXIAL |
| More Detail: | 442 kOhms ±0.5% 1W Through Hole Resistor Axial Pul... |
| DataSheet: | H4P442KDZA Datasheet/PDF |
| Quantity: | 1000 |
| 250 +: | $ 0.31880 |
| Series: | Holco, Holsworthy |
| Packaging: | Bulk |
| Part Status: | Active |
| Resistance: | 442 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
Resistors are one of the most common components in electronic circuits. They are used when it is necessary to control the voltage or current in a circuit, or to limit the amount of power dissipated in a circuit. Through hole type resistors, also known as leaded resistors, are the most common type of resistors used today. They consist of a resistor body, usually made of ceramic, in which a spiral of ceramic material is embedded. The spiral is the resistor element, and is made by depositing a metallic film of either copper or nickel over a ceramic substrate. At each end of the resistor body are two metal leads, which connect the resistor element to the rest of the circuit.
A H4P442KDZA is one type of through hole resistor. It is an axial type resistor, and it is designed to dissipate heat quickly and efficiently. The most common applications of such a resistor are in power transmission and control circuits, or in applications where there is a large current flow. It is also used in light bulb filaments, and is often used in automotive electrical systems. It is often used in medium power circuits, and is particularly useful when large current flows are present.
The body of the H4P442KDZA is a hollow ceramic cylinder, and the resistor element consists of a spiral of nickel-plated copper, which is then coated with an insulation material. Two metal leads, made of either copper or nickel plated copper, are fed through the two ends of the cylinder, and the resistor element is connected to the leads. The resistance is determined by the physical dimensions of the resistor element, and is usually marked on the side of the body. The voltage rating of the resistor is usually between 6 and 15 volts.
The working principle of a H4P442KDZA is based on the fact that resistors, usually made of carbon, reduce the amount of current flowing in a given circuit. When the voltage is applied to the resistor, a voltage drop occurs across the resistor, reducing the current in the circuit. The amount of current is determined by the resistance of the resistor. The resistance of a H4P442KDZA is controlled by the dimensions of the resistor element, and the voltage rating determines the maximum voltage that can be applied to the resistor.
H4P442KDZA through hole resistors are highly reliable, and can be used in a wide range of applications. They are also relatively inexpensive, so they are an economical choice for many different applications. In addition, they can be easily mounted in a variety of ways, such as soldering, press-fitting, or with the use of Mica washers, which are used to provide additional insulation. Because of their reliability and low cost, they are one of the most popular types of resistors used today.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| H4P47KFCA | TE Connectiv... | 0.29 $ | 1000 | RES 47.0K OHM 1W 1% AXIAL... |
| H4P4K64DCA | TE Connectiv... | 0.39 $ | 1000 | RES 4.64K OHM 1W 0.5% AXI... |
| H4P4K02DZA | TE Connectiv... | 0.35 $ | 1000 | RES 4.02K OHM 1W 0.5% AXI... |
| H4P43KFZA | TE Connectiv... | 0.24 $ | 1000 | RES 43K OHM 1W 1% AXIAL43... |
| H4P43RFZA | TE Connectiv... | 0.24 $ | 1000 | RES 43 OHM 1W 1% AXIAL43 ... |
| H4P46R4DCA | TE Connectiv... | 0.39 $ | 1000 | RES 46.4 OHM 1W 0.5% AXIA... |
| H4P470RFCA | TE Connectiv... | 0.29 $ | 1000 | RES 470 OHM 1W 1% AXIAL47... |
| H4P46R4DZA | TE Connectiv... | 0.35 $ | 1000 | RES 46.4 OHM 1W 0.5% AXIA... |
| H4P40R2DZA | TE Connectiv... | 0.35 $ | 1000 | RES 40.2 OHM 1W 0.5% AXIA... |
| H4P46K4DCA | TE Connectiv... | 0.39 $ | 1000 | RES 46.4K OHM 1W 0.5% AXI... |
| H4P430RFCA | TE Connectiv... | 0.29 $ | 1000 | RES 430 OHM 1W 1% AXIAL43... |
| H4P40K2DZA | TE Connectiv... | 0.35 $ | 1000 | RES 40.2K OHM 1W 0.5% AXI... |
| H4P442KDZA | TE Connectiv... | 0.35 $ | 1000 | RES 442K OHM 1W 0.5% AXIA... |
| H4P47RFZA | TE Connectiv... | 0.44 $ | 499 | RES 47 OHM 1W 1% AXIAL47 ... |
| H4P4K7FCA | TE Connectiv... | 0.29 $ | 1000 | RES 4.70K OHM 1W 1% AXIAL... |
| H4P464RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 464 OHM 1W 0.5% AXIAL... |
| H4P4M0DCA | TE Connectiv... | 0.72 $ | 488 | RES 4M OHM 1W 0.5% AXIAL4... |
| H4P48K7DZA | TE Connectiv... | 0.35 $ | 1000 | RES 48.7K OHM 1W 0.5% AXI... |
| H4P48R7DCA | TE Connectiv... | 0.39 $ | 1000 | RES 48.7 OHM 1W 0.5% AXIA... |
| H4P44R2DCA | TE Connectiv... | 0.39 $ | 1000 | RES 44.2 OHM 1W 0.5% AXIA... |
| H4P430KFZA | TE Connectiv... | 0.24 $ | 1000 | RES 430K OHM 1W 1% AXIAL4... |
| H4P487RDCA | TE Connectiv... | 0.39 $ | 1000 | RES 487 OHM 1W 0.5% AXIAL... |
| H4P4K3FCA | TE Connectiv... | 0.29 $ | 1000 | RES 4.30K OHM 1W 1% AXIAL... |
| H4P464KDCA | TE Connectiv... | 0.39 $ | 1000 | RES 464K OHM 1W 0.5% AXIA... |
| H4P48K7DCA | TE Connectiv... | 0.39 $ | 1000 | RES 48.7K OHM 1W 0.5% AXI... |
| H4P470KFCA | TE Connectiv... | 0.29 $ | 1000 | RES 470K OHM 1W 1% AXIAL4... |
| H4P442RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 442 OHM 1W 0.5% AXIAL... |
| H4P48R7DZA | TE Connectiv... | 0.35 $ | 1000 | RES 48.7 OHM 1W 0.5% AXIA... |
| H4P42R2DCA | TE Connectiv... | 0.39 $ | 1000 | RES 42.2 OHM 1W 0.5% AXIA... |
| H4P4K02DCA | TE Connectiv... | 0.39 $ | 1000 | RES 4.02K OHM 1W 0.5% AXI... |
| H4P4K42DCA | TE Connectiv... | 0.39 $ | 1000 | RES 4.42K OHM 1W 0.5% AXI... |
| H4P470RFZA | TE Connectiv... | 0.24 $ | 1000 | RES 470 OHM 1W 1% AXIAL47... |
| H4P44K2DZA | TE Connectiv... | 0.35 $ | 1000 | RES 44.2K OHM 1W 0.5% AXI... |
| H4P43RFCA | TE Connectiv... | 0.29 $ | 1000 | RES 43.0 OHM 1W 1% AXIAL4... |
| H4P402RDCA | TE Connectiv... | 0.39 $ | 1000 | RES 402 OHM 1W 0.5% AXIAL... |
| H4P4R7FZA | TE Connectiv... | 0.24 $ | 960 | RES 4.7 OHM 1W 1% AXIAL4.... |
| H4P422KDZA | TE Connectiv... | 0.35 $ | 1000 | RES 422K OHM 1W 0.5% AXIA... |
| H4P487RDZA | TE Connectiv... | 0.35 $ | 1000 | RES 487 OHM 1W 0.5% AXIAL... |
| H4P464KDZA | TE Connectiv... | 0.35 $ | 1000 | RES 464K OHM 1W 0.5% AXIA... |
| H4P422RDCA | TE Connectiv... | 0.39 $ | 1000 | RES 422 OHM 1W 0.5% AXIAL... |
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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...
H4P442KDZA Datasheet/PDF