
Allicdata Part #: | A138082TB-ND |
Manufacturer Part#: |
ROX2SJ4K3 |
Price: | $ 0.03 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 4.30K OHM 2W 5% AXIAL |
More Detail: | 4.3 kOhms ±5% 2W Through Hole Resistor Axial Flame... |
DataSheet: | ![]() |
Quantity: | 1000 |
1000 +: | $ 0.02285 |
2000 +: | $ 0.02094 |
5000 +: | $ 0.01904 |
10000 +: | $ 0.01777 |
25000 +: | $ 0.01753 |
Series: | ROX, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 4.3 kOhms |
Tolerance: | ±5% |
Power (Watts): | 2W |
Composition: | Metal Oxide Film |
Features: | Flame Proof, Pulse Withstanding, Safety |
Temperature Coefficient: | ±350ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.197" Dia x 0.472" L (5.00mm x 12.00mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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 are one of the most common components used in electronic circuits. The ROX2SJ4K3 is a resistor of this type, and it has several characteristics which make it different from most other resistors. This article will explore the application field and working principle of the ROX2SJ4K3 resistor.
Application Field
The ROX2SJ4K3 is a through hole resistor rated for use in industrial and military applications. Its high thermal stability and low temperature coefficient of resistance make it an ideal choice for applications where it will be exposed to extreme temperatures and environments. It has high accuracy and stability, making it suitable for precision measurement applications. The ROX2SJ4K3 is also able to operate at high frequencies, making it ideal for use in working with RF signals. It is widely used in military and aerospace applications.
Working Principle
The ROX2SJ4K3 is a resistor that operates on the principle of resistance of electric current. In general, resistance is determined by the material from which the resistor is made and its geometrical shape. The ROX2SJ4K3 is made of the material bismuth-telluride and has a cylindrical shape. When an electrical current is applied to the resistor, the bismuth-telluride material will resist the flow of current and create an electrical potential difference. This potential difference is what determines the amount of resistance that the resistor will offer.
The ROX2SJ4K3 resistor also has a temperature coefficient of resistance. This is a measure of how much the resistance of the resistor changes as the temperature of its surroundings changes. The ROX2SJ4K3 has a very low temperature coefficient, which makes it suitable for use in applications where the temperature may fluctuate significantly over time.
The ROX2SJ4K3 is also able to operate in high-frequency conditions. High frequency operation is determined by the speed with which the electrical current passes through the resistor. The resistance of the ROX2SJ4K3 is high enough to prevent the current from passing too quickly, but low enough to allow a sufficient amount of current to pass. This makes it suitable for use in high-frequency applications where the frequency of the current is very high.
The ROX2SJ4K3 is a popular choice for use in industrial and military applications due to its high accuracy and stability. Its low temperature coefficient of resistance and high frequency capability make it an ideal choice for precision measurements and for working with RF signals. Its cylindrical shape and high thermal stability enable it to withstand extreme temperatures and environments, making it an ideal choice for tough applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
ROX2SJ56R | TE Connectiv... | 0.03 $ | 1000 | RES 56.0 OHM 2W 5% AXIAL5... |
ROX2SJ390R | TE Connectiv... | 0.03 $ | 2000 | RES 390 OHM 2W 5% AXIAL39... |
ROX2SG100K | TE Connectiv... | 0.05 $ | 1000 | RES 100K OHM 2W 2% AXIAL1... |
ROX2SJ2K2 | TE Connectiv... | 0.03 $ | 2000 | RES 2.20K OHM 2W 5% AXIAL... |
ROX2SJ270K | TE Connectiv... | 0.03 $ | 2000 | RES 270K OHM 2W 5% AXIAL2... |
ROX2SJ470R | TE Connectiv... | 0.03 $ | 1000 | RES 470 OHM 2W 5% AXIAL47... |
ROX2SJ82R | TE Connectiv... | 0.03 $ | 1000 | RES 82.0 OHM 2W 5% AXIAL8... |
ROX2SJ10R | TE Connectiv... | 0.03 $ | 5000 | RES 10.0 OHM 2W 5% AXIAL1... |
ROX2SJ1R2 | TE Connectiv... | 0.03 $ | 2000 | RES 1.20 OHM 2W 5% AXIAL1... |
ROX2SJ6K8 | TE Connectiv... | 0.19 $ | 1998 | RES 6.80K OHM 2W 5% AXIAL... |
ROX2SJR47 | TE Connectiv... | 0.18 $ | 1000 | RES 0.47 OHM 2W 5% AXIAL4... |
ROX2SJ220R | TE Connectiv... | 0.03 $ | 2000 | RES 220 OHM 2W 5% AXIAL22... |
ROX2SG6R8TR | TE Connectiv... | 0.05 $ | 1000 | RES 6.80 OHM 2W 2% AXIAL6... |
ROX2SJ47K | TE Connectiv... | 0.03 $ | 1000 | RES 47.0K OHM 2W 5% AXIAL... |
ROX2001M00FKEL | Vishay Dale | 5.31 $ | 1000 | RES 1M OHM 6W 1% AXIAL1 M... |
ROX2SJ1K0 | TE Connectiv... | 0.03 $ | 2000 | RES 1.00K OHM 2W 5% AXIAL... |
ROX2SJ47R | TE Connectiv... | 0.03 $ | 1000 | RES 47.0 OHM 2W 5% AXIAL4... |
ROX2SJ1K8 | TE Connectiv... | 0.03 $ | 2000 | RES 1.80K OHM 2W 5% AXIAL... |
ROX2SJ270R | TE Connectiv... | 0.03 $ | 2000 | RES 270 OHM 2W 5% AXIAL27... |
ROX2SJ3K9 | TE Connectiv... | 0.03 $ | 2000 | RES 3.90K OHM 2W 5% AXIAL... |
ROX2SJ5K6 | TE Connectiv... | 0.03 $ | 2000 | RES 5.60K OHM 2W 5% AXIAL... |
ROX2003M40FKEL | Vishay Dale | 5.31 $ | 13 | RES 3.4M OHM 6W 1% AXIAL3... |
ROX2SJ1R0 | TE Connectiv... | 0.03 $ | 6000 | RES 1.00 OHM 2W 5% AXIAL1... |
ROX2SJ39R | TE Connectiv... | 0.03 $ | 10000 | RES 39.0 OHM 2W 5% AXIAL3... |
ROX2SG300R | TE Connectiv... | 0.05 $ | 1000 | RES 300 OHM 2W 2% AXIAL30... |
ROX2SJ6R8 | TE Connectiv... | 0.03 $ | 2000 | RES 6.80 OHM 2W 5% AXIAL6... |
ROX2SJ12R | TE Connectiv... | 0.03 $ | 2000 | RES 12.0 OHM 2W 5% AXIAL1... |
ROX2SJ220K | TE Connectiv... | 0.03 $ | 1000 | RES 220K OHM 2W 5% AXIAL2... |
ROX2SJ1K2 | TE Connectiv... | 0.03 $ | 2000 | RES 1.20K OHM 2W 5% AXIAL... |
ROX2SJ150R | TE Connectiv... | 0.03 $ | 1000 | RES 150 OHM 2W 5% AXIAL15... |
ROX2SJ1M0 | TE Connectiv... | 0.03 $ | 1000 | RES 1.00M OHM 2W 5% AXIAL... |
ROX2SJ2R0 | TE Connectiv... | 0.03 $ | 1000 | RES 2.0 OHM 2W 5% AXIAL2 ... |
ROX2SJR22 | TE Connectiv... | 0.18 $ | 1000 | RES 0.22 OHM 2W 5% AXIAL2... |
ROX2SJ120K | TE Connectiv... | 0.03 $ | 2000 | RES 120K OHM 2W 5% AXIAL1... |
ROX2SJ330K | TE Connectiv... | 0.03 $ | 2000 | RES 330K OHM 2W 5% AXIAL3... |
ROX2SF1R8 | TE Connectiv... | 0.04 $ | 1000 | RES 1.8 OHM 2W 1% AXIAL1.... |
ROX2SJ4K3 | TE Connectiv... | 0.03 $ | 1000 | RES 4.30K OHM 2W 5% AXIAL... |
ROX2J100R | TE Connectiv... | 0.04 $ | 1000 | RES 100 OHM 2W 5% AXIAL10... |
ROX2J180R | TE Connectiv... | 0.04 $ | 1000 | RES 180 OHM 2W 5% AXIAL18... |
ROX2SJ470K | TE Connectiv... | 0.03 $ | 2000 | RES 470K OHM 2W 5% AXIAL4... |
RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...

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

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...
