RN50E2002CB14 Allicdata Electronics
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 datasheetRN50E2002CB14 Datasheet/PDF
Quantity: 1000
100 +: $ 0.67851
300 +: $ 0.58158
500 +: $ 0.48465
1000 +: $ 0.42003
5000 +: $ 0.40711
Stock 1000Can Ship Immediately
$ 0.75
Specifications
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: --
Description

Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us:   sales@allicdata.com

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

Related Products
Search Part number : "RN50" Included word is 40
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...
Latest Products
SQM700JB-68K

RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...

SQM700JB-68K Allicdata Electronics
SQM700JB-1R3

RES WW 7W 5% TH1.3 Ohms 5% 7W Through Ho...

SQM700JB-1R3 Allicdata Electronics
RNC60J24R9FSB14

RES 24.9 OHM 1/4W 1% AXIAL24.9 Ohms 1% 0...

RNC60J24R9FSB14 Allicdata Electronics
RWR89S2R80DRS70

RES 2.8 OHM 3W 0.5% WW AXIAL2.8 Ohms 0.5...

RWR89S2R80DRS70 Allicdata Electronics
RNC60J7503FSB14

RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...

RNC60J7503FSB14 Allicdata Electronics
RWR81S3400FSB12

RES 340 OHM 1W 1% WW AXIAL340 Ohms 1% 1W...

RWR81S3400FSB12 Allicdata Electronics