Allicdata Part #: | LR1F13K-ND |
Manufacturer Part#: |
LR1F13K |
Price: | $ 0.01 |
Product Category: | Resistors |
Manufacturer: | TE Connectivity Passive Product |
Short Description: | RES 13.0K OHM 0.6W 1% AXIAL |
More Detail: | 13 kOhms ±1% 0.6W Through Hole Resistor Axial Met... |
DataSheet: | LR1F13K Datasheet/PDF |
Quantity: | 1000 |
4000 +: | $ 0.00759 |
Series: | LR, Neohm |
Packaging: | Tape & Box (TB) |
Part Status: | Active |
Resistance: | 13 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: | -- |
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 are an important component in a variety of electrical and electronic devices, as they regulate the flow of electricity in a circuit. The most common type of through-hole resistor is the LR1F13K, which is widely used in small signal, precision, industrial, and some military applications. In order to better understand this resistor and its application fields, we need to first look at its working principles.
The LR1F13K is a through-hole resistor with two terminals that can be soldered into a circuit board. It is made of a ceramic body encased in a metal shell. The body is filled with a resistive material and encased in a shell that provides environmental protection and a barrier to the resistive material. The resistive material is usually composed of a blend of various metals and other materials, which are chosen to produce the desired resistance value.
The LR1F13K functions by allowing a specific amount of electric current to flow through a circuit by creating a resistive impedance. It works through the principle of Ohm’s law, which states that when current is applied to the resistor, the voltage drop is proportional to the resistance value. In other words, the resistor limits the flow of electricity by providing a resistance between two points in a circuit. The resistance value of the LR1F13K can be adjusted by changing the type of material or the composition of the resistive material.
The LR1F13K is an ideal choice for applications where accuracy and precision are important, such as medical, communications, and aerospace applications. It is also widely used in computer motherboards and notebook computers, as its intricate construction provides highly reliable and accurate performance. In order to achieve even higher accuracy, the resistance value of the LR1F13K can be altered by changing the type of material or the composition of the resistive material.
The LR1F13K can also be used in RF applications, as it can provide reliable and accurate performance in the presence of radio frequency (RF) noise and interference. This is due to its ability to filter out the interference and provide a precise resistance level. Its high frequency response enables the LR1F13K to operate without adding consistent noise. In addition, its small physical size makes it a viable solution for designing miniature components.
Aside from the automotive, consumer, and medical industries, the LR1F13K is also used in industrial applications such as instrumentation, control, power control, and automation. Its resistance value can be adjusted to provide different levels of control and precision. For example, the resistor can be used to control the speed of a motor or the duration of a signal. The resistor can also be used in instrumentation applications, as it can provide a wide range of resistance values for measuring signals.
The LR1F13K is a versatile and reliable through-hole resistor that can be used in a wide range of applications, from consumer electronics to industrial automation. The resistor is composed of a ceramic body encased in a metal shell, and it works on the principle of Ohm’s law. Its precise resistance values and high frequency response make it an ideal choice for applications requiring accuracy and high performance.
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...