Allicdata Part #: | LR2F91K-ND |
Manufacturer Part#: |
LR2F91K |
Price: | $ 0.02 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 91.0K OHM 3/4W 1% AXIAL |
More Detail: | 91 kOhms ±1% 0.75W, 3/4W Through Hole Resistor Axi... |
DataSheet: | LR2F91K Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 0.01994 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 91 kOhms |
Tolerance: | ±1% |
Power (Watts): | 0.75W, 3/4W |
Composition: | Metal Film |
Features: | -- |
Temperature Coefficient: | ±100ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.138" Dia x 0.382" L (3.50mm x 9.70mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through Hole Resistors carry a level of importance and significance in circuit boards, power supplies, and other electrical systems. The LR2F91K is a particularly unique resistor that come with higher resistance values than traditional through hole components. Combined with the fact that it’s a two-in-one type, these small resistors have interesting applications and are widely used in the electronics world.
The LR2F91K is used primarily in the production of control resistors and variable resistors. This small resistor is composed of two small resistors welded together. By etching a patterned mesh into the surface of the resistor, these electrically connected resistors can alter the resistance value without having to alter any of the components. This makes them great options when stability and precise measurement is desired.
Additionally, this type of double resistor comes with improved power and lower noise levels. This makes them perfect for amplifiers, audio systems, and other high power applications. With a maximum resistance of 100K, LR2F91K resistors can be used for even the most power-hungry applications.
To understand how the LR2F91K works, it’s important to first understand the principles of resistors. When an electrical current passes through a resistor, it experiences a small amount of resistance. This causes the current to be limited, and the voltage is then reduced. By altering the resistance value, the current can be limited and controlled further.
The LR2F91K works like a typical resistor in the sense that the electric current must pass through the resistor to experience resistance. However, since it’s composed of two small resistors, the resistance can be more precisely controlled and altered. By etching a respective pattern onto each side of the resistor, the resistance can be increased or decreased without having to manipulate the components.
This double resistor can come with resistance values ranging from 1K to 100K, making it a flexible and versatile part in many circuits. As mentioned earlier, the LR2F91K can be used in power supplies, audio systems, and amplifiers, as well as in control resistors and variable resistors. Its wide range of resistance values make it a popular choice in many projects.
Likewise, these resistors are also low-noise and offer excellent temperature stability. This is especially important since many circuits are sensitive to noise and temperature fluctuations. The low noise and high tolerance of the LR2F91K make it ideal for these types of projects. Most LR2F91K resistors are lead-free and halogen-free, making them perfect for those projects that require it.
Overall, the LR2F91K is an incredibly useful resistor with applications in power supplies, audio systems, amplifiers, control resistors, and variable resistors. It’s composed of two small resistors that can be etched with a particular pattern for peak performance. With resistance values ranging from 1K to 100K, these double resistors are great for projects that require precise measurements and consistent performance.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LR2F1K0 | TE Connectiv... | 0.02 $ | 1000 | RES 1.00K OHM 3/4W 1% AXI... |
LR2F510K | TE Connectiv... | 0.02 $ | 1000 | RES 510K OHM 3/4W 1% AXIA... |
LR2F330RJIT | TE Connectiv... | 0.02 $ | 1000 | RES 330 OHM 3/4W 1% AXIAL... |
LR2F390R | TE Connectiv... | 0.02 $ | 1000 | RES 390 OHM 3/4W 1% AXIAL... |
LR2F100K | TE Connectiv... | 0.02 $ | 1000 | RES 100K OHM 3/4W 1% AXIA... |
LR2F100R | TE Connectiv... | 0.02 $ | 1000 | RES 100 OHM 3/4W 1% AXIAL... |
LR2F10K | TE Connectiv... | 0.02 $ | 1000 | RES 10.0K OHM 3/4W 1% AXI... |
LR2F110K | TE Connectiv... | 0.02 $ | 1000 | RES 110K OHM 3/4W 1% AXIA... |
LR2F110R | TE Connectiv... | 0.02 $ | 1000 | RES 110 OHM 3/4W 1% AXIAL... |
LR2F11K | TE Connectiv... | 0.02 $ | 1000 | RES 11.0K OHM 3/4W 1% AXI... |
LR2F11R | TE Connectiv... | 0.02 $ | 1000 | RES 11.0 OHM 3/4W 1% AXIA... |
LR2F120K | TE Connectiv... | 0.02 $ | 1000 | RES 120K OHM 3/4W 1% AXIA... |
LR2F120R | TE Connectiv... | 0.02 $ | 1000 | RES 120 OHM 3/4W 1% AXIAL... |
LR2F12K | TE Connectiv... | 0.02 $ | 1000 | RES 12.0K OHM 3/4W 1% AXI... |
LR2F12R | TE Connectiv... | 0.02 $ | 1000 | RES 12.0 OHM 3/4W 1% AXIA... |
LR2F130K | TE Connectiv... | 0.02 $ | 1000 | RES 130K OHM 3/4W 1% AXIA... |
LR2F130R | TE Connectiv... | 0.02 $ | 1000 | RES 130 OHM 3/4W 1% AXIAL... |
LR2F13K | TE Connectiv... | 0.02 $ | 1000 | RES 13.0K OHM 3/4W 1% AXI... |
LR2F13R | TE Connectiv... | 0.02 $ | 1000 | RES 13.0 OHM 3/4W 1% AXIA... |
LR2F150K | TE Connectiv... | 0.02 $ | 1000 | RES 150K OHM 3/4W 1% AXIA... |
LR2F150R | TE Connectiv... | 0.02 $ | 1000 | RES 150 OHM 3/4W 1% AXIAL... |
LR2F15K | TE Connectiv... | 0.02 $ | 1000 | RES 15.0K OHM 3/4W 1% AXI... |
LR2F15R | TE Connectiv... | 0.02 $ | 1000 | RES 15.0 OHM 3/4W 1% AXIA... |
LR2F160K | TE Connectiv... | 0.02 $ | 1000 | RES 160K OHM 3/4W 1% AXIA... |
LR2F160R | TE Connectiv... | 0.02 $ | 1000 | RES 160 OHM 3/4W 1% AXIAL... |
LR2F16K | TE Connectiv... | 0.02 $ | 1000 | RES 16.0K OHM 3/4W 1% AXI... |
LR2F16R | TE Connectiv... | 0.02 $ | 1000 | RES 16.0 OHM 3/4W 1% AXIA... |
LR2F180K | TE Connectiv... | 0.02 $ | 1000 | RES 180K OHM 3/4W 1% AXIA... |
LR2F180R | TE Connectiv... | 0.02 $ | 1000 | RES 180 OHM 3/4W 1% AXIAL... |
LR2F18K | TE Connectiv... | 0.02 $ | 1000 | RES 18.0K OHM 3/4W 1% AXI... |
LR2F18R | TE Connectiv... | 0.02 $ | 1000 | RES 18.0 OHM 3/4W 1% AXIA... |
LR2F1K1 | TE Connectiv... | 0.02 $ | 1000 | RES 1.10K OHM 3/4W 1% AXI... |
LR2F1K2 | TE Connectiv... | 0.02 $ | 1000 | RES 1.20K OHM 3/4W 1% AXI... |
LR2F1K5 | TE Connectiv... | 0.02 $ | 1000 | RES 1.50K OHM 3/4W 1% AXI... |
LR2F1K6 | TE Connectiv... | 0.02 $ | 1000 | RES 1.60K OHM 3/4W 1% AXI... |
LR2F1K8 | TE Connectiv... | 0.02 $ | 1000 | RES 1.80K OHM 3/4W 1% AXI... |
LR2F1M0 | TE Connectiv... | 0.02 $ | 1000 | RES 1.00M OHM 3/4W 1% AXI... |
LR2F200K | TE Connectiv... | 0.02 $ | 1000 | RES 200K OHM 3/4W 1% AXIA... |
LR2F200R | TE Connectiv... | 0.02 $ | 1000 | RES 200 OHM 3/4W 1% AXIAL... |
LR2F20K | TE Connectiv... | 0.02 $ | 1000 | RES 20.0K OHM 3/4W 1% AXI... |
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