Allicdata Part #: | LR1F261R-ND |
Manufacturer Part#: |
LR1F261R |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 261 OHM 0.6W 1% AXIAL |
More Detail: | 261 Ohms ±1% 0.6W Through Hole Resistor Axial Met... |
DataSheet: | LR1F261R Datasheet/PDF |
Quantity: | 1000 |
4000 +: | $ 0.00723 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 261 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: | -- |
Due to market price fluctuations, if you need to purchase or consult the price. You can contact us or emial to us: sales@allicdata.com
Through Hole Resistors LR1F261R application field and working principle
A through hole resistor, also known as a leaded resistor, is an electronic component composed of a resistive element, and two wire terminals for connection to a circuit. It is designed for through hole mounting in printed circuit boards, plug-in boards, and other electronic devices. Through hole resistors are widely used in a variety of applications, from basic circuits such as switch circuits, to high speed signal conditioning, to linear current sensing.
LR1F261R Characteristics
The LR1F261R is a through hole resistor designed by Panasonic. It is a non-inductive, high-power resistor with a low voltage drop and high heat dissipation. The LR1F261R is resistor is rated for a maximum operating temperature of +150°C, and a voltage rating of 250V. It has low thermal resistance and a maximum resistance of 1.2kΩ. It also features low power dissipation, low thermal noise, and a high accuracy tolerance.
Applications
The LR1F261R is mostly used in high power applications such as power supplies, power converters, and motor control systems. It is also used for current sensing, voltage limiting, ringing suppression, power inrush, PTC, and transient voltage suppression applications. It is also capable of replacing other through hole resistors in applications such as current measurement, soft-start, and current sensing applications.
Working Principle
The working principle of a through hole resistor is based on Ohm\'s Law. The electrical resistor consists of a resistive element that limits the flow of electric current through it. The resistance of the resistor is proportional to the amount of current flowing through it, and it is inversely proportional to the voltage applied across it. As the current passing through the resistor increases, the voltage drop across it increases. As the voltage increases, the heat dissipation will also increase due to the resistive nature of the element.
The power dissipation of a resistor is the product of the voltage and the current passing through it. When the voltage across the resistor equals the rated voltage of the resistor, the power dissipation reaches its peak and the resistor begins to heat up. When the power dissipation is higher than the resistance\'s rated power dissipation, the resistor will begin to overheat and damage can occur.
The LR1F261R is designed with a low voltage drop and high heat dissipation, so it is capable of dissipating high amounts of power without overheating. It is also designed with low thermal resistance and a maximum resistance of 1.2kΩ, making it suitable for high power applications.
In conclusion, the LR1F261R is a through hole resistor by Panasonic designed for high power applications. It has a low voltage drop and high heat dissipation. It is capable of dissipating high amounts of power without overheating and can be used in a variety of applications.
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... |
RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...
RES WW 7W 5% TH1.3 Ohms 5% 7W Through Ho...
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...