Allicdata Part #: | LR2F270R-ND |
Manufacturer Part#: |
LR2F270R |
Price: | $ 0.02 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 270 OHM 3/4W 1% AXIAL |
More Detail: | 270 Ohms ±1% 0.75W, 3/4W Through Hole Resistor Axi... |
DataSheet: | LR2F270R Datasheet/PDF |
Quantity: | 1000 |
1000 +: | $ 0.01994 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 270 Ohms |
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 are among the most commonly used passive components in electronic technology. In this article, I will describe the application field and working principle of LR2F270R through hole resistor, in order to gain a better understanding of the resistors.
LR2F270R is ideal for use in various applications, such as power electronics, automotive electronics, instrumentations, communication electronics, consumer and industrial electronics. It is used in environments ranging from leisure and entertainment, to mission-critical industrial control. Due to its ability to operate reliably over a wide temperature range, LR2F270R is also often used in outdoor or remote sensor applications, as well as complex automotive infotainment systems. Additionally, with its wide variety of packages, LR2F270R offers solutions for almost any design.
LR2F270R works through the Joule Effect. The Joule Effect is a phenomenon that occurs when a current passes through a conductor and produces heat energy. This heat energy is a mechanical energy that can be converted into electrical energy. When a resistor is placed between two points of an electrical circuit, the electrons will move through the resistor and produce a voltage drop between those two points. The higher the resistance, the more voltage drop occurs. This permits the user to adjust the voltage and current levels of the electrical components in a circuit.
In an LR2F270R through-hole resistor, the resistor is enclosed inside a shell that is made of insulating material such as ceramic. The resistor itself is composed of various layers of materials, such as metal, ceramic, and dielectric material. The resistor is wired to two ends of the shell, where one end is connected to either the negative or positive side of the circuit. The other end is connected to the ground. When an electrical current is passed through the resistor, electrons move through the resistor and produce a voltage drop, thus decreasing the amount of current and voltage in the circuit.
LR2F270R through hole resistors have a wide range of applications. They are used in various power electronics, automotive electronics, instrumentations, communication electronics, consumer and industrial electronics. Additionally, they can be used in outdoor or remote sensor applications, as well as in complex automotive infotainment systems. The wide variety of packages makes the LR2F270R solutions ideal for virtually any design.
To sum up, LR2F270R is a through hole resistor that has a wide range of applications and is used in various electronic technology. Through the Joule effect, the resistor is able to convert mechanical energy to electrical energy, and adjust the voltage and current levels of electrical components in a circuit. With its wide variety of packages and temperature range, the LR2F270R through hole resistor is a reliable and viable solution for any design.
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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