Allicdata Part #: | LR1F560K-ND |
Manufacturer Part#: |
LR1F560K |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 560K OHM 0.6W 1% AXIAL |
More Detail: | 560 kOhms ±1% 0.6W Through Hole Resistor Axial Me... |
DataSheet: | LR1F560K Datasheet/PDF |
Quantity: | 1000 |
4000 +: | $ 0.00759 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 560 kOhms |
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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Through-hole resistors are widely used for a variety of applications and offer a number of benefits over surface-mount and axial resistors, including better heat management, wide lead spacing, ease of mounting, and higher voltage and current ratings. The LR1F560K is a through-hole resistor with a wide range of applications, including power supplies, lighting, motor controllers, and instrumentation.
The LR1F560K is a 5W resistor with a resistance of 560K ohms. It features excellent stability and high tolerance levels of 1% and 5%. This resistor is made from a combination of high-grade copper, cardboard, and synthetic materials to ensure maximum reliability and performance. Its insulated metal construction ensures that it can handle temperatures up to 400°F (204°C), while its copper core dissipates heat quickly and efficiently.
The LR1F560K has two lead bonds on it, making it ideal for high-current applications. Its lead spacing is also wide enough to provide proper spacing and spacing between components, as well as providing a low profile for mounting in tight locations. Additionally, this resistor can handle voltages up to 500V.
The LR1F560K resistor works by converting voltage into current. This is done by using the principles of Ohm\'s Law, which states that voltage (V) is equal to current (I) times resistance (R). In a resistor, the resistance (R) is fixed, so when voltage (V) is applied, the current (I) will be equal to V divided by R. The LR1F560K\'s 560K resistance ensures that it will be able to handle the voltage applied to it without dissipating too much power.
The LR1F560K through-hole resistor is an excellent choice for high voltage and current applications, thanks to its excellent stability and wide lead spacing. Its metal construction ensures that it can handle temperatures up to 400°F (204°C), while its copper core dissipates heat quickly and efficiently. Additionally, its high tolerance levels of 1% and 5% make it reliable and provide precise operation.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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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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