
Allicdata Part #: | LR1F61K9-ND |
Manufacturer Part#: |
LR1F61K9 |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 61.9K OHM 0.6W 1% AXIAL |
More Detail: | 61.9 kOhms ±1% 0.6W Through Hole Resistor Axial M... |
DataSheet: | ![]() |
Quantity: | 1000 |
4000 +: | $ 0.00723 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 61.9 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 can be divided into many categories, LR1F61K9 is one of the most common ones. In this article, we will explore the application field and working principle of the LR1F61K9 resistor.
The LR1F61K9 resistor is a high rating resistor in the through hole family. It is widely used in applications such as industrial control, electrical instrumentation, and domestic appliances. It is usually mass produced in large quantities, due to its size and form factor.
The LR1F61K9 is constructed from an insulated copper winding with multiple layers of insulation surrounding it. This insulation layer acts as a barrier between the conductor and the outer environment, thereby allowing for a greater heat dissipation capacity than other types of resistors.
In addition to basic electrical resistance, this type of resistor also exhibits electrical noise suppression capabilities. This is because the insulation layer prevents a current from the outside environment from affecting the electrical parameters of the resistor. As such, electrical systems are much more reliable and stable when using LR1F61K9.
The working principle of the LR1F61K9 resistor is fairly simple. The resistance is created by the resistance of the copper winding. When a signal is applied to the resistor, the current will flow through the winding, creating a voltage across it. This voltage is then translated into resistance, which determines the electrical performance of the device. Since the resistance depends on the current, the resistance can be adjusted by simply changing the current. This is why the LR1F61K9 is often used in systems where an adjustable resistance is needed.
Overall, the LR1F61K9 resistant is a high performance through hole resistor which has excellent noise suppression capabilities. Its resistance can be adjusted by changing the current, and its insulation layer prevents interference from external sources. With so many advantages, it is no wonder that the LR1F61K9 is a popular choice for many applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LR1F5K1 | TE Connectiv... | 0.01 $ | 1000 | RES 5.10K OHM 0.6W 1% AXI... |
LR1F487R | TE Connectiv... | 0.01 $ | 1000 | RES 487 OHM 0.6W 1% AXIAL... |
LR1F18K | TE Connectiv... | 0.01 $ | 1000 | RES 18.0K OHM 0.6W 1% AXI... |
LR1F1R1 | TE Connectiv... | 0.01 $ | 1000 | RES 1.10 OHM 0.6W 1% AXIA... |
LR1F1K0 | TE Connectiv... | 0.01 $ | 4000 | RES 1.00K OHM 0.6W 1% AXI... |
LR1F140K | TE Connectiv... | 0.01 $ | 1000 | RES 140K OHM 0.6W 1% AXIA... |
LR1F402R | TE Connectiv... | 0.01 $ | 1000 | RES 402 OHM 0.6W 1% AXIAL... |
LR1F3K92 | TE Connectiv... | 0.01 $ | 1000 | RES 3.92K OHM 0.6W 1% AXI... |
LR1F470K | TE Connectiv... | 0.01 $ | 1000 | RES 470K OHM 0.6W 1% AXIA... |
LR1F115K | TE Connectiv... | 0.01 $ | 1000 | RES 115K OHM 0.6W 1% AXIA... |
LR1F590R | TE Connectiv... | 0.01 $ | 1000 | RES 590 OHM 0.6W 1% AXIAL... |
LR1F2R7 | TE Connectiv... | 0.01 $ | 1000 | RES 2.70 OHM 0.6W 1% AXIA... |
LR1F5K36 | TE Connectiv... | 0.01 $ | 1000 | RES 5.36K OHM 0.6W 1% AXI... |
LR1F330R | TE Connectiv... | 0.01 $ | 4000 | RES 330 OHM 0.6W 1% AXIAL... |
LR1F3K0 | TE Connectiv... | 0.01 $ | 1000 | RES 3.00K OHM 0.6W 1% AXI... |
LR1F91K | TE Connectiv... | 0.01 $ | 1000 | RES 91.0K OHM 0.6W 1% AXI... |
LR1F3M3 | TE Connectiv... | 0.01 $ | 1000 | RES 3.30M OHM 0.6W 1% AXI... |
LR1F5R1 | TE Connectiv... | 0.01 $ | 1000 | RES 5.10 OHM 0.6W 1% AXIA... |
LR1F6K2 | TE Connectiv... | 0.01 $ | 1000 | RES 6.20K OHM 0.6W 1% AXI... |
LR1F56R2 | TE Connectiv... | 0.01 $ | 1000 | RES 56.2 OHM 0.6W 1% AXIA... |
LR1F47R | TE Connectiv... | 0.01 $ | 1000 | RES 47.0 OHM 0.6W 1% AXIA... |
LR1F3R0 | TE Connectiv... | 0.01 $ | 1000 | RES 3.0 OHM 0.6W 1% AXIAL... |
LR1F221K | TE Connectiv... | 0.01 $ | 1000 | RES 221K OHM 0.6W 1% AXIA... |
LR1F1K3 | TE Connectiv... | 0.01 $ | 1000 | RES 1.30K OHM 0.6W 1% AXI... |
LR1F2K2 | TE Connectiv... | 0.01 $ | 1000 | RES 2.20K OHM 0.6W 1% AXI... |
LR1F43R2 | TE Connectiv... | 0.01 $ | 1000 | RES 43.2 OHM 0.6W 1% AXIA... |
LR1F360R | TE Connectiv... | 0.01 $ | 1000 | RES 360 OHM 0.6W 1% AXIAL... |
LR1F36K | TE Connectiv... | 0.01 $ | 1000 | RES 36.0K OHM 0.6W 1% AXI... |
LR1F14K7 | TE Connectiv... | 0.01 $ | 1000 | RES 14.7K OHM 0.6W 1% AXI... |
LR1F100K | TE Connectiv... | 0.01 $ | 8000 | RES 100K OHM 0.6W 1% AXIA... |
LR1F1K21 | TE Connectiv... | 0.01 $ | 1000 | RES 1.21K OHM 0.6W 1% AXI... |
LR1F47K5 | TE Connectiv... | 0.01 $ | 1000 | RES 47.5K OHM 0.6W 1% AXI... |
LR1F200K | TE Connectiv... | 0.01 $ | 1000 | RES 200K OHM 0.6W 1% AXIA... |
LR1F120R | TE Connectiv... | 0.01 $ | 12000 | RES 120 OHM 0.6W 1% AXIAL... |
LR1F56K2 | TE Connectiv... | 0.01 $ | 1000 | RES 56.2K OHM 0.6W 1% AXI... |
LR1F464R | TE Connectiv... | 0.01 $ | 1000 | RES 464 OHM 0.6W 1% AXIAL... |
LR1F30K | TE Connectiv... | 0.01 $ | 1000 | RES 30.0K OHM 0.6W 1% AXI... |
LR1F62K | TE Connectiv... | 0.01 $ | 1000 | RES 62.0K OHM 0.6W 1% AXI... |
LR1F523R | TE Connectiv... | 0.01 $ | 1000 | RES 523 OHM 0.6W 1% AXIAL... |
LR1F422R | TE Connectiv... | 0.01 $ | 1000 | RES 422 OHM 0.6W 1% AXIAL... |
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