Allicdata Part #: | H4562KBDA-ND |
Manufacturer Part#: |
H4562KBDA |
Price: | $ 0.51 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 562K OHM 1/2W 0.1% AXIAL |
More Detail: | 562 kOhms ±0.1% 0.5W, 1/2W Through Hole Resistor A... |
DataSheet: | H4562KBDA Datasheet/PDF |
Quantity: | 1000 |
250 +: | $ 0.46438 |
Series: | Holco, Holsworthy |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 562 kOhms |
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 are components that are used mainly to extend or limit the current in a circuit. The resistor is typically fabricated from metal and ceramic and serves a wide range of applications. H4562KBDA is a type of through-hole resistor that is mainly used for frequency measuring and frequency matching applications.
Features of H4562KBDA include:
- A resistive element with low temperature coefficient;
- Wide resistance range with low resistance values;
- Provides high stability and accuracy;
- Compact packages with low height; and
- Low EMI, high efficiency, and low noise level.
The main application areas for H4562KBDA are measurement instruments, communication devices, high-speed sampling/sampling comparators, and image processing systems. The component can be used in oscillation circuits, precision current limiting circuits, signal generator circuits, and signal transistors. In addition, it can be used to reduce noise or reduce current signals with high gain.
The working principle of H4562KBDA is essentially based on Ohm\'s Law. This law states that the current through a conductor between two points is directly proportional to the potential difference across the two points. In other words, the current, I, between two points with voltage, V, can be calculated using the following formula:
I = V/R
Where R is the resistance of the H4562KBDA resistor. When the voltage applied to a resistor increases, a higher amount of current will flow through the component proportional to the resistance of the resistor. Conversely, when the voltage is reduced, the current will correspondingly reduce.
In addition, the voltage-current relationship of a resistor can be described using V-I curves. This curve is created for a particular value of resistance to illustrate the response of the resistor at various voltages. The V-I curve for a H4562KBDA is non-linear and exhibits a low temperature coefficient.
For example, when the voltage is applied to the component, the initial current is lower than the final current, and this is known as the “ramp-up” characteristic. This characteristic is important to ensure a smooth and linear output of the resistor. When the current is increased, the current level eventually reaches a peak and the voltage begins to drop, this is known as the “saturating” characteristic.
In short, the H4562KBDA is a through-hole resistor that is mainly used for frequency measuring and frequency matching applications. The component utilizes Ohm\'s law and V-I curves to accurately regulate the current and voltage of the signal. It is characterized by low temperature coefficient, wide resistance range, high stability and accuracy, compact packages, low EMI, high efficiency and low noise level. The H4562KBDA is suitable for various applications including oscillation circuits, precision current limiting circuits, signal generator circuits, and signal transistors.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
H4562KBDA | TE Connectiv... | 0.51 $ | 1000 | RES 562K OHM 1/2W 0.1% AX... |
H4560RABA | TE Connectiv... | 1.28 $ | 1000 | RES 560 OHM 1/2W 0.05% AX... |
H456R2BDA | TE Connectiv... | 0.51 $ | 1000 | RES 56.2 OHM 1/2W 0.1% AX... |
H4562RBDA | TE Connectiv... | 0.51 $ | 1000 | RES 562 OHM 1/2W 0.1% AXI... |
H456K2BDA | TE Connectiv... | 0.51 $ | 1000 | RES 56.2K OHM 1/2W 0.1% A... |
H456R2BYA | TE Connectiv... | 0.57 $ | 1000 | RES 56.2 OHM 1/2W 0.1% AX... |
H456K2BYA | TE Connectiv... | 0.57 $ | 1000 | RES 56.2K OHM 1/2W 0.1% A... |
H4562KBYA | TE Connectiv... | 0.57 $ | 1000 | RES 562K OHM 1/2W 0.1% AX... |
H456R2DYA | TE Connectiv... | 0.46 $ | 1000 | RES 56.2 OHM 1/2W 0.5% AX... |
H4562RDYA | TE Connectiv... | 0.46 $ | 1000 | RES 562 OHM 1/2W 0.5% AXI... |
H456K2DYA | TE Connectiv... | 0.46 $ | 1000 | RES 56.2K OHM 1/2W 0.5% A... |
H4562KDYA | TE Connectiv... | 0.46 $ | 1000 | RES 562K OHM 1/2W 0.5% AX... |
H456R2BCA | TE Connectiv... | 0.48 $ | 1000 | RES 56.2 OHM 1/2W 0.1% AX... |
H4562RBCA | TE Connectiv... | 0.48 $ | 1000 | RES 562 OHM 1/2W 0.1% AXI... |
H456K2BCA | TE Connectiv... | 0.48 $ | 1000 | RES 56.2K OHM 1/2W 0.1% A... |
H4562KBCA | TE Connectiv... | 0.48 $ | 1000 | RES 562K OHM 1/2W 0.1% AX... |
H456R2BZA | TE Connectiv... | 0.41 $ | 1000 | RES 56.2 OHM 1/2W 0.1% AX... |
H4562RBZA | TE Connectiv... | 0.41 $ | 1000 | RES 562 OHM 1/2W 0.1% AXI... |
H456K2BZA | TE Connectiv... | 0.41 $ | 1000 | RES 56.2K OHM 1/2W 0.1% A... |
H4562KBZA | TE Connectiv... | 0.41 $ | 1000 | RES 562K OHM 1/2W 0.1% AX... |
H4562RBYA | TE Connectiv... | 0.57 $ | 1000 | RES 562 OHM 1/2W 0.1% AXI... |
H4562KFYA | TE Connectiv... | 0.29 $ | 1000 | RES 562K OHM 1/2W 1% AXIA... |
H456RFZA | TE Connectiv... | 0.24 $ | 1000 | RES 56 OHM 1/2W 1% AXIAL5... |
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