Allicdata Part #: | LR1F499R-ND |
Manufacturer Part#: |
LR1F499R |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 499 OHM 0.6W 1% AXIAL |
More Detail: | 499 Ohms ±1% 0.6W Through Hole Resistor Axial Met... |
DataSheet: | LR1F499R Datasheet/PDF |
Quantity: | 1000 |
4000 +: | $ 0.00723 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 499 Ohms |
Tolerance: | ±1% |
Power (Watts): | 0.6W |
Composition: | Metal Film |
Features: | -- |
Temperature Coefficient: | ±50ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.091" Dia x 0.244" L (2.30mm x 6.20mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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The LR1F499R is a type of through hole resistors. It is designed to function as a bulk type of resistance for any application, from power supplies to high voltage circuit lines. It is a product of Sanyo, one of the largest electronics manufacturers in Japan.
LR1F499R resistors are known for their reliability and high performance. They are constructed of a spiral-carved ceramic. The ceramic is then layered with a mixture of manganese and nickel oxide to provide a durable and reliable connection. This design ensures that the resistors have a long life and stay operational even in extreme temperatures.
When it comes to the primary application fields of LR1F499R, these resistors are commonly utilized in high-power circuits. Some examples include power supplies, audio amplifiers, and motors. They are also suitable for other applications where a high level of resistance is required without a significant drop in voltage. In addition, they are an excellent choice for noise suppression due to their noise-reducing features.
When it comes to the working principle of the LR1F499R, this type of resistance is based on the temperature coefficient of resistance. This property of electrons can be used to increase or decrease the voltage output of a circuit. As temperature increases, the electrons move faster, resulting in an increase in voltage. Conversely, when the temperature decreases, the resistance of the electrons decreases, resulting in a decrease in voltage.
Overall, the LR1F499R is an excellent choice for many types of applications. Its durability, performance, and temperature coefficient of resistance make it a go-to option for many electronics projects. Its construction ensures that it will remain reliable and operational over long periods of time, and its noise-reducing features make it an excellent choice for noise suppression.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LR1F180R | TE Connectiv... | 0.01 $ | 1000 | RES 180 OHM 0.6W 1% AXIAL... |
LR1F110K | TE Connectiv... | 0.01 $ | 1000 | RES 110K OHM 0.6W 1% AXIA... |
LR1F110R | TE Connectiv... | 0.01 $ | 1000 | RES 110 OHM 0.6W 1% AXIAL... |
LR1F11K | TE Connectiv... | 0.01 $ | 1000 | RES 11.0K OHM 0.6W 1% AXI... |
LR1F11R | TE Connectiv... | 0.01 $ | 1000 | RES 11.0 OHM 0.6W 1% AXIA... |
LR1F120K | TE Connectiv... | 0.01 $ | 1000 | RES 120K OHM 0.6W 1% AXIA... |
LR1F12K | TE Connectiv... | 0.01 $ | 1000 | RES 12.0K OHM 0.6W 1% AXI... |
LR1F12R | TE Connectiv... | 0.01 $ | 1000 | RES 12.0 OHM 0.6W 1% AXIA... |
LR1F130K | TE Connectiv... | 0.01 $ | 1000 | RES 130K OHM 0.6W 1% AXIA... |
LR1F130R | TE Connectiv... | 0.01 $ | 1000 | RES 130 OHM 0.6W 1% AXIAL... |
LR1F13K | TE Connectiv... | 0.01 $ | 1000 | RES 13.0K OHM 0.6W 1% AXI... |
LR1F13R | TE Connectiv... | 0.01 $ | 1000 | RES 13.0 OHM 0.6W 1% AXIA... |
LR1F150K | TE Connectiv... | 0.01 $ | 1000 | RES 150K OHM 0.6W 1% AXIA... |
LR1F15K | TE Connectiv... | 0.01 $ | 1000 | RES 15.0K OHM 0.6W 1% AXI... |
LR1F15R | TE Connectiv... | 0.01 $ | 1000 | RES 15.0 OHM 0.6W 1% AXIA... |
LR1F160K | TE Connectiv... | 0.01 $ | 1000 | RES 160K OHM 0.6W 1% AXIA... |
LR1F160R | TE Connectiv... | 0.01 $ | 1000 | RES 160 OHM 0.6W 1% AXIAL... |
LR1F16K | TE Connectiv... | 0.01 $ | 1000 | RES 16.0K OHM 0.6W 1% AXI... |
LR1F16R | TE Connectiv... | 0.01 $ | 1000 | RES 16.0 OHM 0.6W 1% AXIA... |
LR1F180K | TE Connectiv... | 0.01 $ | 1000 | RES 180K OHM 0.6W 1% AXIA... |
LR1F18K | TE Connectiv... | 0.01 $ | 1000 | RES 18.0K OHM 0.6W 1% AXI... |
LR1F18R | TE Connectiv... | 0.01 $ | 1000 | RES 18.0 OHM 0.6W 1% AXIA... |
LR1F1K1 | TE Connectiv... | 0.01 $ | 1000 | RES 1.10K OHM 0.6W 1% AXI... |
LR1F1K2 | TE Connectiv... | 0.01 $ | 1000 | RES 1.20K OHM 0.6W 1% AXI... |
LR1F1K3 | TE Connectiv... | 0.01 $ | 1000 | RES 1.30K OHM 0.6W 1% AXI... |
LR1F1K6 | TE Connectiv... | 0.01 $ | 1000 | RES 1.60K OHM 0.6W 1% AXI... |
LR1F200K | TE Connectiv... | 0.01 $ | 1000 | RES 200K OHM 0.6W 1% AXIA... |
LR1F200R | TE Connectiv... | 0.01 $ | 1000 | RES 200 OHM 0.6W 1% AXIAL... |
LR1F20R | TE Connectiv... | 0.01 $ | 1000 | RES 20.0 OHM 0.6W 1% AXIA... |
LR1F220K | TE Connectiv... | 0.01 $ | 1000 | RES 220K OHM 0.6W 1% AXIA... |
LR1F220R | TE Connectiv... | 0.01 $ | 1000 | RES 220 OHM 0.6W 1% AXIAL... |
LR1F22R | TE Connectiv... | 0.01 $ | 1000 | RES 22.0 OHM 0.6W 1% AXIA... |
LR1F240K | TE Connectiv... | 0.01 $ | 1000 | RES 240K OHM 0.6W 1% AXIA... |
LR1F24K | TE Connectiv... | 0.01 $ | 1000 | RES 24.0K OHM 0.6W 1% AXI... |
LR1F24R | TE Connectiv... | 0.01 $ | 1000 | RES 24.0 OHM 0.6W 1% AXIA... |
LR1F270K | TE Connectiv... | 0.01 $ | 1000 | RES 270K OHM 0.6W 1% AXIA... |
LR1F27K | TE Connectiv... | 0.01 $ | 1000 | RES 27.0K OHM 0.6W 1% AXI... |
LR1F27R | TE Connectiv... | 0.01 $ | 1000 | RES 27.0 OHM 0.6W 1% AXIA... |
LR1F2K0 | TE Connectiv... | 0.01 $ | 1000 | RES 2.00K OHM 0.6W 1% AXI... |
LR1F2K4 | TE Connectiv... | 0.01 $ | 1000 | RES 2.40K OHM 0.6W 1% AXI... |
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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...