| Allicdata Part #: | RN50E2002CB14-ND |
| Manufacturer Part#: |
RN50E2002CB14 |
| Price: | $ 0.75 |
| Product Category: | Resistors |
| Manufacturer: | Vishay Dale |
| Short Description: | RES 20K OHM 1/20W .25% AXIAL |
| More Detail: | 20 kOhms ±0.25% 0.05W, 1/20W Through Hole Resistor... |
| DataSheet: | RN50E2002CB14 Datasheet/PDF |
| Quantity: | 1000 |
| 100 +: | $ 0.67851 |
| 300 +: | $ 0.58158 |
| 500 +: | $ 0.48465 |
| 1000 +: | $ 0.42003 |
| 5000 +: | $ 0.40711 |
| Series: | Military, MIL-R-10509/8, RN50 |
| Packaging: | Bulk |
| Part Status: | Active |
| Resistance: | 20 kOhms |
| Tolerance: | ±0.25% |
| Power (Watts): | 0.05W, 1/20W |
| Composition: | Metal Film |
| Features: | Flame Retardant Coating, Military, Moisture Resistant, Safety |
| Temperature Coefficient: | ±25ppm/°C |
| Operating Temperature: | -65°C ~ 175°C |
| Package / Case: | Axial |
| Supplier Device Package: | Axial |
| Size / Dimension: | 0.065" Dia x 0.150" L (1.65mm x 3.81mm) |
| Height - Seated (Max): | -- |
| Number of Terminations: | 2 |
| Failure Rate: | -- |
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Through Hole Resistors provide a variety of features and characteristics, allowing for precise control of current and voltage levels in electronic circuits. The RN50E2002CB14 is a unique through hole resistor that combines a high voltage tolerance, with a low temperature coefficient and an extremely low dielectric absorption ratio, making it an ideal choice for a variety of applications. This article will provide a detailed description of the RN50E2002CB14 application field and working principle.
What is the RN50E2002CB14?
The RN50E2002CB14 is a through hole resistor, which is a type of resistor that is able to handle high power and current levels. The RN50E2002CB14 features a high voltage tolerance, making them particularly well-suited for high-voltage circuit designs. Additionally, the RN50E2002CB14 device has a temperature coefficient of 0.5% per degree Celsius in temperature range, making them suitable for high-power, high-temperature applications, such as those in automotive and other harsh environments. It also has an extremely low dielectric absorption ratio, allowing them to efficiently convert electrical energy into heat.
RN50E2002CB14 Application Field
The RN50E2002CB14 can be applied to a wide range of applications, including: automotive, lighting, telecommunications, audio systems, computerized control systems, power supply systems, RF and microwave systems, and many others. In automotive applications, RN50E2002CB14s can be used to insulate power lines from signals, to protect sensitive components from noise and interference, and to control the voltage level in spark plug circuits. In audio systems, they are often used to attenuate high-frequency signals in order to control feedback and distortion. In computerized control systems, they can be used to regulate the supply voltage of components. In RF and microwave systems, the RN50E2002CB14 can help reduce reflections at components and ensure the desired operating frequencies.
RN50E2002CB14 Working Principle
The RN50E2002CB14 does not actively generate electrical energy. Instead, it is an electrical component that passively converts electrical energy into another form, usually heat or resistance. It works by providing an opposition to the flow of electrons, thus controlling the voltage and current levels. The RN50E2002CB14s are also able to absorb energy from the circuit, which is then converted into heat and dissipated away from the component. This dissipated heat should be taken into account when choosing a suitable resistor for a circuit.
In addition to its high voltage tolerance and low temperature coefficient, the RN50E2002CB14 also provides a range of other advantages. For example, they have a low inductance, meaning that currents flowing through them will not be distorted. Additionally, they are non-polarized, meaning that their polarity does not need to be considered when connecting them to a circuit. This further simplifies the design of these devices, and minimizes the risk of damage due to incorrect connections.
In Summary
The RN50E2002CB14 is a unique through hole resistor that can be used in a wide range of applications due to its high voltage tolerance, low temperature coefficient, and low dielectric absorption ratio. It works by providing an opposition to the flow of electrons, which convert electrical energy into another form. It has a range of advantages, including low inductance and non-polarity, which makes it well-suited for a range of control systems, audio systems, and RF and microwave systems.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| RN50C13R3FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 13.3 OHM 1/20W 1% AXI... |
| RN50C95R3FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 95.3 OHM 1/20W 1% AXI... |
| RN50C6811FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 6.81K OHM 1/20W 1% AX... |
| RN50C3092FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 30.9K OHM 1/20W 1% AX... |
| RN50C1062FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 10.6K OHM 1/20W 1% AX... |
| RN50C6900FB14 | Vishay Dale | 0.1 $ | 1000 | RES 690 OHM 1/20W 1% AXIA... |
| RN50C3221FB14 | Vishay Dale | 0.1 $ | 1000 | RES 3.22K OHM 1/20W 1% AX... |
| RN50E9092BRE6 | Vishay Dale | 0.33 $ | 1000 | RES 90.9K OHM 1/20W .1% A... |
| RN50E8660FRSL | Vishay Dale | 0.34 $ | 1000 | RES 866 OHM 1/20W 1% AXIA... |
| RN50C4070BRSL | Vishay Dale | 0.4 $ | 1000 | RES 407 OHM 1/20W .1% AXI... |
| RN50E2002FB14 | Vishay Dale | 0.63 $ | 1000 | RES 20K OHM 1/20W 1% AXIA... |
| RN50C8251FB14 | Vishay Dale | 0.63 $ | 1000 | RES 8.25K OHM 1/20W 1% AX... |
| RN50C1402FB14 | Vishay Dale | 0.63 $ | 1000 | RES 14K OHM 1/20W 1% AXIA... |
| RN50C2673FB14 | Vishay Dale | 0.63 $ | 1000 | RES 267K OHM 1/20W 1% AXI... |
| RN50C4020FB14 | Vishay Dale | 0.63 $ | 1000 | RES 402 OHM 1/20W 1% AXIA... |
| RN50C8061FBSL | Vishay Dale | 0.75 $ | 1000 | RES 8.06K OHM 1/20W 1% AX... |
| RN50C4422DBSL | Vishay Dale | 0.75 $ | 1000 | RES 44.2K OHM 1/20W .5% A... |
| RN50E1021BB14 | Vishay Dale | 0.8 $ | 1000 | RES 1.02K OHM 1/20W .1% A... |
| RN50E6811BB14 | Vishay Dale | 0.8 $ | 1000 | RES 6.81K OHM 1/20W .1% A... |
| RN50E7322BBSL | Vishay Dale | 0.96 $ | 1000 | RES 73.2K OHM 1/20W .1% A... |
| RN50C1502FB14 | Vishay Dale | 0.93 $ | 175 | RES 15K OHM 1/20W 1% AXIA... |
| RN50C4990FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 499 OHM 1/20W 1% AXIA... |
| RN50C2102FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 21K OHM 1/20W 1% AXIA... |
| RN50C2212FRE6 | Vishay Dale | 0.1 $ | 1000 | RES 22.1K OHM 1/20W 1% AX... |
| RN50C8002FB14 | Vishay Dale | 0.1 $ | 1000 | RES 80K OHM 1/20W 1% AXIA... |
| RN50C3163FRE6 | Vishay Dale | 0.16 $ | 1000 | RES 316K OHM 1/20W 1% AXI... |
| RN50E1051FRE6 | Vishay Dale | 0.2 $ | 1000 | RES 1.05K OHM 1/20W 1% AX... |
| RN50C7870FRSL | Vishay Dale | 0.21 $ | 1000 | RES 787 OHM 1/20W 1% AXIA... |
| RN50C3683DRE6 | Vishay Dale | 0.21 $ | 1000 | RES 368K OHM 1/20W .5% AX... |
| RN50C2212BR36 | Vishay Dale | 0.23 $ | 1000 | RES 22.1K OHM 1/20W .1% A... |
| RN50C1821BRE6 | Vishay Dale | 0.24 $ | 1000 | RES 1.82K OHM 1/20W .1% A... |
| RN50C6801BRE6 | Vishay Dale | 0.24 $ | 1000 | RES 6.8K OHM 1/20W .1% AX... |
| RN50E6812FRSL | Vishay Dale | 0.34 $ | 1000 | RES 68.1K OHM 1/20W 1% AX... |
| RN50E5621BRSL | Vishay Dale | 0.55 $ | 1000 | RES 5.62K OHM 1/20W .1% A... |
| RN50C1693FB14 | Vishay Dale | 0.63 $ | 1000 | RES 169K OHM 1/20W 1% AXI... |
| RN50C5491FB14 | Vishay Dale | 0.63 $ | 1000 | RES 5.49K OHM 1/20W 1% AX... |
| RN50C28R7FB14 | Vishay Dale | 0.63 $ | 1000 | RES 28.7 OHM 1/20W 1% AXI... |
| RN50C4322FB14 | Vishay Dale | 0.63 $ | 1000 | RES 43.2K OHM 1/20W 1% AX... |
| RN50C1132BB14 | Vishay Dale | 0.69 $ | 1000 | RES 11.3K OHM 1/20W .1% A... |
| RN50C8661FBSL | Vishay Dale | 0.75 $ | 1000 | RES 8.66K OHM 1/20W 1% AX... |
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RN50E2002CB14 Datasheet/PDF