Allicdata Part #: | LT50J-22-ND |
Manufacturer Part#: |
LTO050F22R00JTE3 |
Price: | $ 3.81 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | RES 22 OHM 50W 5% TO220 |
More Detail: | 22 Ohms ±5% 50W Through Hole Resistor TO-220-2 Non... |
DataSheet: | LTO050F22R00JTE3 Datasheet/PDF |
Quantity: | 1985 |
1 +: | $ 3.46050 |
10 +: | $ 3.24225 |
100 +: | $ 2.30553 |
1000 +: | $ 1.89943 |
Series: | LTO 50 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 22 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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Through Hole Resistors, like the LTO050F22R00JTE3, are a common component in many electronic circuits and play a vital role in providing precise resistance and in protecting devices from short circuits. These resistors are small in size and use a simple yet effective component layout, making them easy to integrate into virtually any circuit. The LTO050F22R00JTE3 is a through hole resistor that behaves similarly to others in its class, but with a few unique features.
First, let\'s take a look at the application field and working principle of this type of resistor. The primary application of a through hole resistor is in DC circuits, which means that they are used to provide a stable voltage in an electrical component in order to control the current. This is done by providing a resistor in series with the component, which works by forcing the current flow to slow down and become steady. This resistance value is determined by the size and resistive accuracy of the resistor in question. The LTO050F22R00JTE3 is rated at 22 Ohms and is capable of providing an excellent level of precise, stable resistance.
The working principle behind the LTO050F22R00JTE3 is essentially identical to that of other through hole resistors. It features a series of connected resistors, which are usually arranged in an in-line pattern. This allows for a single current path that also features multiple resistor values, which helps to ensure a high level of accuracy. Additionally, when the resistors are arranged in this manner, it results in less heat loss and reduces the need for extra forms of heat dissipation.
Aside from the actual resistive element, the LTO050F22R00JTE3 also includes a snap-in design that makes installation and removal a breeze. This design also helps to reduce the amount of time it takes to assemble circuit boards, saving both time and money. Another advantage of this resistor design is that it offers excellent levels of tolerance, meaning that the component can withstand changes in temperature or varying levels of current.
In terms of manufacturing, the LTO050F22R00JTE3 is made from a special form of electrical grade polyester called Nomex. This material is very strong and provides superior levels of tolerance, reliability, and consistency. It is also able to withstand extreme temperatures, which makes it an ideal choice for use in a wide variety of electronic components.
Overall, the LTO050F22R00JTE3 through hole resistor is a powerful and resilient component that is well suited for a variety of applications. It provides a reliable and precise resistance value, which can often be the difference between a successful operation and a costly failure. This resistor\'s snap-in design is also a major plus, making it easy to install and remove, and helping to keep assembly costs and downtime to a minimum. Factor in its excellent level of tolerance and its excellent manufacturing materials, and the LTO050F22R00JTE3 is well worth considering for any through hole applications.
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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