Allicdata Part #: | LT30J-.47-ND |
Manufacturer Part#: |
LTO030FR4700JTE3 |
Price: | $ 2.60 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | RES 0.47 OHM 30W 5% TO220 |
More Detail: | 470 mOhms ±5% 30W Through Hole Resistor TO-220-2 N... |
DataSheet: | LTO030FR4700JTE3 Datasheet/PDF |
Quantity: | 1000 |
50 +: | $ 2.36412 |
Series: | LTO 30 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 470 mOhms |
Tolerance: | ±5% |
Power (Watts): | 30W |
Composition: | Thick Film |
Features: | Non-Inductive |
Temperature Coefficient: | ±250ppm/°C |
Operating Temperature: | -55°C ~ 150°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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Through Hole Resistors are a type of resistive component commonly used in industrial, automotive, consumer and military applications. The LTO030FR4700JTE3 is a through-hole resistor component that can be used in electronic circuits to provide a resistance to the flow of electricity. It is constructed with a metal film resistor element and polyester substrate. It is a non-inductive type with flame-retardant coating and can withstand high temperature. The resistance value can be adjusted when necessary with a potentiometer.
The LTO030FR4700JTE3 is used for power supply applications, such as voltage stabilizers, DC-DC converters and motor control. It is also used in circuit protection, such as EMI/ESD filtering and lightning suppression. It is often used in automotive and military applications because of its flame retardant coating and high temperature resistance.
The LTO030FR4700JTE3 has an operating temperature range of -40°C to +105°C and an insulation resistance of 1,000MΩ minimum at 500V DC. It can withstand any charged or static component that might be present in the system without damage. It is very reliable and low TCR, and its response is fast and predictable. It also has high power dissipation.
The working principle of the LTO030FR4700JTE3 is simple. It works by providing an electrical resistance to the flow of electricity. This resistance, which is measured in ohms, is necessary for ensuring that an electrical circuit works correctly. The resistance value can be adjusted using a potentiometer. The resistance is generated by the metal film resistor element which is sandwiched between two polyester substrates.
The LTO030FR4700JTE3 is a reliable, high temperature resistant, through hole resistor that is used in many electronic applications. Its resistance value can be adjusted using a potentiometer, and it has a wide operating temperature range. It is often used in automotive, military, power supply, and circuit protection applications. It is reliable, has a fast and predictable response, and its high power dissipation ensures that it can withstand electrical surges.
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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