Allicdata Part #: | LT50J-1.0-ND |
Manufacturer Part#: |
LTO050F1R000JTE3 |
Price: | $ 3.81 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | RES 1 OHM 50W 5% TO220 |
More Detail: | 1 Ohms ±5% 50W Through Hole Resistor TO-220-2 Non-... |
DataSheet: | LTO050F1R000JTE3 Datasheet/PDF |
Quantity: | 3 |
1 +: | $ 3.46050 |
10 +: | $ 3.24225 |
100 +: | $ 2.30553 |
1000 +: | $ 1.89943 |
Series: | LTO 50 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 1 Ohms |
Tolerance: | ±5% |
Power (Watts): | 50W |
Composition: | Thick Film |
Features: | Non-Inductive |
Temperature Coefficient: | ±150ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | TO-220-2 |
Supplier Device Package: | TO-220 |
Size / Dimension: | 0.409" L x 0.126" W (10.40mm x 3.20mm) |
Height - Seated (Max): | 0.650" (16.50mm) |
Number of Terminations: | 2 |
Failure Rate: | -- |
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A through hole resistor is an electronic component that is frequently used in the production of electronic circuits. The LTO050F1R000JE3 is a through hole resistor that provides resistance across a range of operating frequencies. It is designed for use in a wide range of applications, from low frequency to high frequency. The resistor is available in two different types: Type 1- is for low frequency applications, and Type 2- is for high frequency applications.
LTO050F1R000JE3 application field
The LTO050F1R000JE3 through hole resistor offers a wide range of applications, from low to high frequency, such as low-power audio amps, low voltage circuitry, general-purpose logic, and RF circuitries. It is used most often in low-frequency applications such as consumer electronics and small electronic devices. It is also used in the manufacture of components for medical equipment, automotive electronics, and instrumentation equipment. This type of resistor is also used in precision industrial, military, and aerospace electronic applications, as it has the ability to withstand high voltage and power.
LTO050F1R000JE3 working principle
The resistance value of the LTO050F1R000JE3 through hole resistor is determined by the thickness of the metal film used in the construction. This metal film is connected between the two terminals of the component. The current flows through the resistor and is transferred from one terminal to the other. This is how resistance is introduced to the circuit. The larger the thickness of the film, the higher the resistance value. So, depending on the desired resistance value, a different thickness of material can be used.
The LTO050F1R000JE3 through hole resistor is designed to tolerate high voltage and power levels and is suitable for use in various types of circuitry. It supports a wide frequency range and provides excellent resistance stability over this range. With its exceptional quality and wide-ranging applications, LTO050F1R000JE3 is an ideal component for use in various industries from military to general circuit design.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LTO030F5R000JTE3 | Vishay Sfern... | -- | 1000 | RES 5 OHM 30W 5% TO2205 O... |
LTO030F10000JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 1K OHM 30W 5% TO2201 ... |
LTO030F2R200JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 2.2 OHM 30W 5% TO2202... |
LTO030FR4700JTE3 | Vishay Sfern... | 2.6 $ | 1000 | RES 0.47 OHM 30W 5% TO220... |
LTO050F10R00JTE3 | Vishay Sfern... | -- | 4709 | RES 10 OHM 50W 5% TO22010... |
LTO050F10000JTE3 | Vishay Sfern... | 3.81 $ | 1381 | RES 1K OHM 50W 5% TO2201 ... |
LTO050FR0100JTE3 | Vishay Sfern... | 5.48 $ | 172 | RES 0.01 OHM 50W 5% TO220... |
LTO050F100R0JTE3 | Vishay Sfern... | 3.81 $ | 2637 | RES 100 OHM 50W 5% TO2201... |
LTO050F4R700JTE3 | Vishay Sfern... | 3.81 $ | 1609 | RES 4.7 OHM 50W 5% TO2204... |
LTO050F10001JTE3 | Vishay Sfern... | 3.81 $ | 520 | RES 10K OHM 50W 5% TO2201... |
LTO050F5R000JTE3 | Vishay Sfern... | 4.19 $ | 468 | RES 5 OHM 50W 5% TO2205 O... |
LTO050F2R200FTE3 | Vishay Sfern... | 5.71 $ | 268 | RES 2.2 OHM 50W 1% TO2202... |
LTO030F15R00JTE3 | Vishay Sfern... | 3.38 $ | 766 | RES 15 OHM 30W 5% TO22015... |
LTO030F22R00JTE3 | Vishay Sfern... | 3.38 $ | 137 | RES 22 OHM 30W 5% TO22022... |
LTO030F10R00JTE3 | Vishay Sfern... | 3.38 $ | 118 | RES 10 OHM 30W 5% TO22010... |
LTO030F4R700JTE3 | Vishay Sfern... | 3.38 $ | 102 | RES 4.7 OHM 30W 5% TO2204... |
LTO030FR1000JTE3 | Vishay Sfern... | 3.75 $ | 104 | RES 0.1 OHM 30W 5% TO2201... |
LTO050F22R00JTE3 | Vishay Sfern... | 3.81 $ | 1985 | RES 22 OHM 50W 5% TO22022... |
LTO050F2R200JTE3 | Vishay Sfern... | 3.81 $ | 1521 | RES 2.2 OHM 50W 5% TO2202... |
LTO050F47R00JTE3 | Vishay Sfern... | 3.81 $ | 286 | RES 47 OHM 50W 5% TO22047... |
LTO050FR4700JTE3 | Vishay Sfern... | 3.81 $ | 199 | RES 0.47 OHM 50W 5% TO220... |
LTO030FR0150JTE3 | Vishay Sfern... | 4.5 $ | 157 | RES 0.015 OHM 30W 5% TO22... |
LTO030FR0100JTE3 | Vishay Sfern... | -- | 111 | RES 0.01 OHM 30W 5% TO220... |
LTO030FR0100FTE3 | Vishay Sfern... | 6.19 $ | 226 | RES 0.01 OHM 30W 1% TO220... |
LTO050FR1000FTE3 | Vishay Sfern... | 6.28 $ | 488 | RES 0.1 OHM 50W 1% TO2201... |
LTO050FR0100FTE3 | Vishay Sfern... | 7.53 $ | 194 | RES 0.01 OHM 50W 1% TO220... |
LTO030F47R00JTE3 | Vishay Sfern... | 3.38 $ | 154 | RES 47 OHM 30W 5% TO22047... |
LTO030F1R000JTE3 | Vishay Sfern... | -- | 1 | RES 1 OHM 30W 5% TO2201 O... |
LTO050F1R000JTE3 | Vishay Sfern... | 3.81 $ | 3 | RES 1 OHM 50W 5% TO2201 O... |
LTO030F100R0JTE3 | Vishay Sfern... | 3.38 $ | 96 | RES 100 OHM 30W 5% TO2201... |
LTO030FR0500JTE3 | Vishay Sfern... | 4.12 $ | 46 | RES 0.05 OHM 30W 5% TO220... |
LTO050FR0680JTE3 | Vishay Sfern... | -- | 47 | RES 0.068 OHM 50W 5% TO22... |
LTO050F100R0FTE3 | Vishay Sfern... | 5.71 $ | 66 | RES 100 OHM 50W 1% TO2201... |
LTO030F10001JTE3 | Vishay Sfern... | -- | 83 | RES 10K OHM 30W 5% TO2201... |
LTO030FR0470JTE3 | Vishay Sfern... | -- | 99 | RES 0.047 OHM 30W 5% TO22... |
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