Allicdata Part #: | H426R7BYA-ND |
Manufacturer Part#: |
H426R7BYA |
Price: | $ 0.57 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 26.7 OHM 1/2W 0.1% AXIAL |
More Detail: | 26.7 Ohms ±0.1% 0.5W, 1/2W Through Hole Resistor A... |
DataSheet: | H426R7BYA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.51966 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 26.7 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 electronic components that are designed to provide electrical resistance. They are usually made from metal, ceramic, or plastic and they are commonly used to regulate current flow or to adjust signal levels. The H426R7BYA resistor is a through-hole resistor with a maximum power rating of 7 watts.
The primary application of the H426R7BYA resistor is to reduce power to a minimal level. It is typically used in power supplies, signal generators, amplifiers, and other applications where high power dissipation is a concern. It is also commonly used in electronic circuits where large amounts of power are to be dissipated, such as in high-power switching applications.
The H426R7BYA resistor is designed to have an electrical resistance that is adjustable. It is typically composed of a metal core, which is wrapped in a ceramic or plastic shell. This shell is then filled with a carbon or metal powder. By varying the amount of powder in the shell, the resistance value can be changed. The resistance value of the H426R7BYA resistor can be adjusted by changing either the internal resistance of the resistor or the external resistance of the circuit.
The working principle of the H426R7BYA resistor is simple. It works by dissipating excess energy, which is released as heat. When electricity passes through the H426R7BYA resistor, it produces an electric current, which causes electrons to move. This movement of electrons results in the dissipation of energy, which is released as heat. The excess heat is then dispersed from the resistor, effectively lowering the current flow and voltage to the desired level.
Through hole resistors like the H426R7BYA have many advantages over other types of resistors. They are able to handle higher power fluctuations and are less susceptible to temperature variations. They are also very reliable and relatively inexpensive. The H426R7BYA resistor is a great choice for many electronic applications where accurate current control is required.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
H4261KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 261K OHM 1/2W 0.1% AX... |
H4267KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 267K OHM 1/2W 0.1% AX... |
H426R1BDA | TE Connectiv... | 0.51 $ | 1000 | RES 26.1 OHM 1/2W 0.1% AX... |
H426R7BDA | TE Connectiv... | 0.51 $ | 1000 | RES 26.7 OHM 1/2W 0.1% AX... |
H4261RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 261 OHM 1/2W 0.1% AXI... |
H4267RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 267 OHM 1/2W 0.1% AXI... |
H426K1BDA | TE Connectiv... | 0.51 $ | 1000 | RES 26.1K OHM 1/2W 0.1% A... |
H426K7BDA | TE Connectiv... | 0.51 $ | 1000 | RES 26.7K OHM 1/2W 0.1% A... |
H426R1BYA | TE Connectiv... | 0.57 $ | 1000 | RES 26.1 OHM 1/2W 0.1% AX... |
H426R7BYA | TE Connectiv... | 0.57 $ | 1000 | RES 26.7 OHM 1/2W 0.1% AX... |
H4261RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 261 OHM 1/2W 0.1% AXI... |
H4267RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 267 OHM 1/2W 0.1% AXI... |
H426K1BYA | TE Connectiv... | 0.57 $ | 1000 | RES 26.1K OHM 1/2W 0.1% A... |
H426K7BYA | TE Connectiv... | 0.57 $ | 1000 | RES 26.7K OHM 1/2W 0.1% A... |
H4261KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 261K OHM 1/2W 0.1% AX... |
H4267KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 267K OHM 1/2W 0.1% AX... |
H426R1DYA | TE Connectiv... | 0.46 $ | 1000 | RES 26.1 OHM 1/2W 0.5% AX... |
H4261RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 261 OHM 1/2W 0.5% AXI... |
H426K1DYA | TE Connectiv... | 0.46 $ | 1000 | RES 26.1K OHM 1/2W 0.5% A... |
H4261KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 261K OHM 1/2W 0.5% AX... |
H426R1BCA | TE Connectiv... | 0.48 $ | 1000 | RES 26.1 OHM 1/2W 0.1% AX... |
H426R7BCA | TE Connectiv... | 0.48 $ | 1000 | RES 26.7 OHM 1/2W 0.1% AX... |
H4261RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 261 OHM 1/2W 0.1% AXI... |
H4267RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 267 OHM 1/2W 0.1% AXI... |
H426K1BCA | TE Connectiv... | 0.48 $ | 1000 | RES 26.1K OHM 1/2W 0.1% A... |
H426K7BCA | TE Connectiv... | 0.48 $ | 1000 | RES 26.7K OHM 1/2W 0.1% A... |
H4261KBCA | TE Connectiv... | 0.48 $ | 1000 | RES 261K OHM 1/2W 0.1% AX... |
H4267KBCA | TE Connectiv... | 0.48 $ | 1000 | RES 267K OHM 1/2W 0.1% AX... |
H426R1BZA | TE Connectiv... | 0.41 $ | 1000 | RES 26.1 OHM 1/2W 0.1% AX... |
H426R7BZA | TE Connectiv... | 0.41 $ | 1000 | RES 26.7 OHM 1/2W 0.1% AX... |
H4261RBZA | TE Connectiv... | 0.41 $ | 1000 | RES 261 OHM 1/2W 0.1% AXI... |
H4267RBZA | TE Connectiv... | 0.41 $ | 1000 | RES 267 OHM 1/2W 0.1% AXI... |
H426K1BZA | TE Connectiv... | 0.41 $ | 1000 | RES 26.1K OHM 1/2W 0.1% A... |
H426K7BZA | TE Connectiv... | 0.41 $ | 1000 | RES 26.7K OHM 1/2W 0.1% A... |
H4261KBZA | TE Connectiv... | 0.41 $ | 1000 | RES 261K OHM 1/2W 0.1% AX... |
H4267KBZA | TE Connectiv... | 0.41 $ | 1000 | RES 267K OHM 1/2W 0.1% AX... |
H4261RFYA | TE Connectiv... | 0.29 $ | 1000 | RES 261 OHM 1/2W 1% AXIAL... |
H426R7FYA | TE Connectiv... | 0.29 $ | 1000 | RES 26.7 OHM 1/2W 1% AXIA... |
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RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...
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