Allicdata Part #: | RSF1WSJR-52-390K-ND |
Manufacturer Part#: |
RSF1WSJR-52-390K |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | Yageo |
Short Description: | RES METAL OXIDE 1W 5% AXIAL |
More Detail: | 390 kOhms ±5% 1W Through Hole Resistor Axial Flame... |
DataSheet: | RSF1WSJR-52-390K Datasheet/PDF |
Quantity: | 1000 |
5000 +: | $ 0.00959 |
Series: | RSF |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Resistance: | 390 kOhms |
Tolerance: | ±5% |
Power (Watts): | 1W |
Composition: | Metal Oxide Film |
Features: | Flame Proof, Safety |
Temperature Coefficient: | ±300ppm/°C |
Operating Temperature: | -55°C ~ 235°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.130" Dia x 0.354" L (3.30mm x 9.00mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
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Through Hole Resistors
Through-hole resistors are electronic components that control the flow of current in a circuit by resisting the current flow, the RSF1WSJR-52-390K being one of the most popular varieties of through-hole resistors in the market today. This type of resistor is a wire wound resistor with four-terminal connection and is made out of two spirally wound manganin elements in parallel, making it highly resistant to thermal and electrical stresses. It is also made of phenolic-impregnated paper, with an superior heat and moisture resistance, making it highly durable and reliable.
The RSF1WSJR-52-390K is a very powerful device that can handle high amounts of power. Due to its construction of four-terminal connections, it is highly effective in minimizing the thermal magnetic effect of the current. It can handle high amounts of power since it is made up of two separate spirally wound elements in paralle. This makes it more efficient in dissipating heat which occurs due to current flowing through it, so that the through-hole resistor is able to handle more power without getting destroyed.
The RSF1WSJR-52-390K has a variety of application fields such as in automotive electronics, industrial electronics, home appliances, and even medical equipment. It is also used in a number of electronic circuits such as power amplifiers, timer circuits, motor control, computer interface, and audio amplifiers, as well as in telecommunication and data communication systems. Its primary function in all these applications is to control the flow of current, preventing it from becoming too powerful.
The RSF1WSJR-52-390K has an interesting working principle. As mentioned before, it is a four-terminal device, with two separate windings spread in parallel. That means that when a current runs through the windings, both of them create a voltage drop across their individual resistances, resulting in a decrease in the voltage over the entire resistor. For a single circuit, this voltage drop results in a reduction in the current, thus controlling it.
What sets the RSF1WSJR-52-390K apart from other types of through-hole resistors is its unique combination of features such as a low actual value, high residual power, low dissipation, and high insulation resistance. All of these features make it especially suitable for high power applications, as its low residual power guarantee a long-term stability of the current, while its high insulation resistance ensures additional protection against short-circuits caused by high voltages.
The RSF1WSJR-52-390K is often used in various placed due to its versatility and reliable performance. It is also highly cost-effective compared to other varieties of resistors in the market due to its easy availability. Although its performance can be affected by environmental conditions such as temperature, humidity, dust, etc, its high reliability and excellent durability make it an ideal choice for a number of applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
RSF100JB-73-390K | Yageo | 0.12 $ | 4512 | RES 390K OHM 1W 5% AXIAL3... |
RSF12JT5R60 | Stackpole El... | 0.01 $ | 1000 | RES 5.6 OHM 1/2W 5% AXIAL... |
RSF1JTR430 | Stackpole El... | 0.02 $ | 1000 | RES 0.43 OHM 1W 5% AXIAL4... |
RSF100JR-73-47R | Yageo | 0.02 $ | 1000 | RES METAL OXIDE 1W 5% AXI... |
RSF100JR-73-0R18 | Yageo | 0.02 $ | 1000 | RES METAL OXIDE 1W 5% AXI... |
RSF1FT3R57 | Stackpole El... | 0.03 $ | 1000 | RES 3.57 OHM 1W 1% AXIAL3... |
RSF1JTR120 | Stackpole El... | 0.03 $ | 1000 | RES 0.12 OHM 1W 5% AXIAL1... |
RSF1FB2K00 | Stackpole El... | 0.03 $ | 1000 | RES 2K OHM 1W 1% AXIAL2 k... |
RSF116404 | Amphenol Pcd | 22.42 $ | 1000 | FRONT RELEASE LC |
RSF1JBR100 | Stackpole El... | 0.03 $ | 1000 | RES 0.1 OHM 1W 5% AXIAL10... |
RSF12FT110K | Stackpole El... | 0.03 $ | 1000 | RES 110K OHM 1/2W 1% AXIA... |
RSF12FTR402 | Stackpole El... | 0.03 $ | 1000 | RES 0.402 OHM 1/2W 1% AXI... |
RSF12FTR511 | Stackpole El... | 0.03 $ | 1000 | RES 0.511 OHM 1/2W 1% AXI... |
RSF12FT1R00 | Stackpole El... | 0.03 $ | 1000 | RES 1 OHM 1/2W 1% AXIAL1 ... |
RSF12FT1R05 | Stackpole El... | 0.03 $ | 1000 | RES 1.05 OHM 1/2W 1% AXIA... |
RSF12FT10K0 | Stackpole El... | 0.03 $ | 1000 | RES 10K OHM 1/2W 1% AXIAL... |
RSF12FT15R0 | Stackpole El... | 0.03 $ | 1000 | RES 15 OHM 1/2W 1% AXIAL1... |
RSF12FT150R | Stackpole El... | 0.03 $ | 1000 | RES 150 OHM 1/2W 1% AXIAL... |
RSF12FT16K9 | Stackpole El... | 0.03 $ | 1000 | RES 16.9K OHM 1/2W 1% AXI... |
RSF12FT2K05 | Stackpole El... | 0.03 $ | 1000 | RES 2.05K OHM 1/2W 1% AXI... |
RSF12FT2K21 | Stackpole El... | 0.03 $ | 1000 | RES 2.21K OHM 1/2W 1% AXI... |
RSF12FT2R49 | Stackpole El... | 0.03 $ | 1000 | RES 2.49 OHM 1/2W 1% AXIA... |
RSF12FT2K49 | Stackpole El... | 0.03 $ | 1000 | RES 2.49K OHM 1/2W 1% AXI... |
RSF12FT23K2 | Stackpole El... | 0.03 $ | 1000 | RES 23.2K OHM 1/2W 1% AXI... |
RSF12FT24R3 | Stackpole El... | 0.03 $ | 1000 | RES 24.3 OHM 1/2W 1% AXIA... |
RSF12FT24R9 | Stackpole El... | 0.03 $ | 1000 | RES 24.9 OHM 1/2W 1% AXIA... |
RSF12FT24K9 | Stackpole El... | 0.03 $ | 1000 | RES 24.9K OHM 1/2W 1% AXI... |
RSF12FT26K7 | Stackpole El... | 0.03 $ | 1000 | RES 26.7K OHM 1/2W 1% AXI... |
RSF12FT294R | Stackpole El... | 0.03 $ | 1000 | RES 294 OHM 1/2W 1% AXIAL... |
RSF12FT3R01 | Stackpole El... | 0.03 $ | 1000 | RES 3.01 OHM 1/2W 1% AXIA... |
RSF12FT34R0 | Stackpole El... | 0.03 $ | 1000 | RES 34 OHM 1/2W 1% AXIAL3... |
RSF12FT4K12 | Stackpole El... | 0.03 $ | 1000 | RES 4.12K OHM 1/2W 1% AXI... |
RSF12FT49R9 | Stackpole El... | 0.03 $ | 1000 | RES 49.9 OHM 1/2W 1% AXIA... |
RSF12FT562R | Stackpole El... | 0.03 $ | 1000 | RES 562 OHM 1/2W 1% AXIAL... |
RSF12FT604R | Stackpole El... | 0.03 $ | 1000 | RES 604 OHM 1/2W 1% AXIAL... |
RSF12FT105R | Stackpole El... | 0.03 $ | 1000 | RES 105 OHM 1/2W 1% AXIAL... |
RSF12FT113R | Stackpole El... | 0.03 $ | 1000 | RES 113 OHM 1/2W 1% AXIAL... |
RSF12FT118R | Stackpole El... | 0.03 $ | 1000 | RES 118 OHM 1/2W 1% AXIAL... |
RSF12FT11K8 | Stackpole El... | 0.03 $ | 1000 | RES 11.8K OHM 1/2W 1% AXI... |
RSF12FT124R | Stackpole El... | 0.03 $ | 1000 | RES 124 OHM 1/2W 1% AXIAL... |
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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...