Allicdata Part #: | 716-1215-ND |
Manufacturer Part#: |
LTO150F22000JTE3 |
Price: | $ 6.33 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | LTO150 F 2K2 5% TU30 E3 |
More Detail: | 2.2 kOhms ±5% 150W Through Hole Resistor TO-247-2 ... |
DataSheet: | LTO150F22000JTE3 Datasheet/PDF |
Quantity: | 60 |
1 +: | $ 5.74650 |
10 +: | $ 5.22540 |
100 +: | $ 3.72299 |
1000 +: | $ 3.44390 |
Series: | LTO 150 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 2.2 kOhms |
Tolerance: | ±5% |
Power (Watts): | 150W |
Composition: | Thick Film |
Features: | Automotive AEC-Q200, Non-Inductive |
Temperature Coefficient: | ±200ppm/°C |
Operating Temperature: | -55°C ~ 175°C |
Package / Case: | TO-247-2 |
Supplier Device Package: | TO-247-2 |
Size / Dimension: | 0.620" L x 0.197" W (15.76mm x 5.00mm) |
Height - Seated (Max): | 0.953" (24.20mm) |
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 used in a variety of electronic applications, and they offer a range of resistance values and withstand a wide range of temperatures. The LTO150F22000JTE3 is a Through Hole resistor designed to provide a resistance value of 22,000 ohms (22k ohms) with a tolerance of 10%. It is a wirewound resistor, which means that thin metal wire is constantly wound onto a ceramic former, thus providing a consistent and reliable resistance.
The LTO150F22000JTE3 Through Hole resistor can be used for a wide variety of applications. It is suitable for use in high-frequency signals, band-pass or low-noise filters, or in power circuits where a reliable, low-noise resistor is required. It is also suitable for signal isolation, signal filtering, and communication circuits. In addition, it can be used in automotive systems, where it acts as a thermal cut-off protector.
The working principle of the LTO150F22000JTE3 is based on a simple concept. When electrical current flows through the resistor, an amount of energy is dissipated as heat. The amount of energy, and thus the amount of heat generated, is proportional to the resistance, hence the higher the resistance value, the more heat is generated. In order to limit the amount of heat, the resistor must dissipate the energy in the form of heat. The ceramic former provides a large surface area, allowing the heat to be quickly and safely dissipated.
In conclusion, the LTO150F22000JTE3 is a Through Hole resistor that offers a reliable, low-noise resistance of 22,000 ohms with a tolerance of 10%. It is suitable for use in a variety of applications including high-frequency signals, band-pass or low-noise filters, power circuits, signal isolation, and thermal cut-off protection. Its working principle is based on the fact that electrical current flows through the resistor, generating an amount of heat proportional to the resistance. The heat is then dissipated through the large surface area provided by the ceramic former.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
LTO100F100R0JTE3 | Vishay Sfern... | 6.45 $ | 2337 | RES 100 OHM 100W 5% TO247... |
LTO100F15R00JTE3 | Vishay Sfern... | 6.45 $ | 345 | RES 15 OHM 100W 5% TO2471... |
LTO100F4R700JTE3 | Vishay Sfern... | 6.45 $ | 270 | RES 4.7 OHM 100W 5% TO247... |
LTO100F1R000JTE3 | Vishay Sfern... | 6.45 $ | 773 | RES 1 OHM 100W 5% TO2471 ... |
LTO100F10000JTE3 | Vishay Sfern... | 6.45 $ | 282 | RES 1K OHM 100W 5% TO2471... |
LTO100F10R00JTE3 | Vishay Sfern... | 6.45 $ | 261 | RES 10 OHM 100W 5% TO2471... |
LTO100F10R00FTE3 | Vishay Sfern... | 8.79 $ | 410 | RES 10 OHM 100W 1% TO2471... |
LTO100F100R0FTE3 | Vishay Sfern... | 8.79 $ | 240 | RES 100 OHM 100W 1% TO247... |
LTO100FR0150JTE3 | Vishay Sfern... | 8.79 $ | 207 | RES 0.015 OHM 100W 5% TO2... |
LTO150F100R0JTE3 | Vishay Sfern... | 6.33 $ | 17 | LTO150 F 100R 5% TU30 E31... |
LTO150F47R00JTE3 | Vishay Sfern... | 6.33 $ | 16 | LTO150 F 47R 5% TU30 E347... |
LTO150F10000JTE3 | Vishay Sfern... | 6.33 $ | 12 | LTO150 F 1K 5% TU30 E31 k... |
LTO150F220R0JTE3 | Vishay Sfern... | 6.33 $ | 20 | LTO150 F 220R 5% TU30 E32... |
LTO150F4R700JTE3 | Vishay Sfern... | 6.33 $ | 1000 | LTO150 F 4R7 5% TU30 E34.... |
LTO150FR1000JTE3 | Vishay Sfern... | 7.59 $ | 19 | LTO150 F R1 5% TU30 E3100... |
LTO100FR1000FTE3 | Vishay Sfern... | 10.55 $ | 22 | RES 0.1 OHM 100W 1% TO247... |
LTO100FR0470JTE3 | Vishay Sfern... | 7.73 $ | 5 | RES 0.047 OHM 100W 5% TO2... |
LTO100F10001JTE3 | Vishay Sfern... | 6.45 $ | 49 | RES 10K OHM 100W 5% TO247... |
LTO100FR0500JTE3 | Vishay Sfern... | 8.51 $ | 36 | RES 0.05 OHM 100W 5% TO24... |
LTO100F4R700FTE3 | Vishay Sfern... | 8.79 $ | 33 | RES 4.7 OHM 100W 1% TO247... |
LTO100FR0220JTE3 | Vishay Sfern... | 8.79 $ | 41 | RES 0.022 OHM 100W 5% TO2... |
LTO150F1R000JTE3 | Vishay Sfern... | 6.33 $ | 45 | LTO150 F 1R 5% TU30 E31 O... |
LTO150F22000JTE3 | Vishay Sfern... | 6.33 $ | 60 | LTO150 F 2K2 5% TU30 E32.... |
LTO150FR4700JTE3 | Vishay Sfern... | 6.33 $ | 30 | LTO150 F R47 5% TU30 E347... |
LTO150F2R200JTE3 | Vishay Sfern... | 6.33 $ | 1000 | LTO150 F 2R2 5% TU30 E32.... |
LTO150F22R00JTE3 | Vishay Sfern... | 6.33 $ | 30 | LTO150 F 22R 5% TU30 E322... |
LTO150F10R00JTE3 | Vishay Sfern... | 6.33 $ | 25 | LTO150 F 10R 5% TU30 E310... |
LTO150F470R0JTE3 | Vishay Sfern... | 6.33 $ | 27 | LTO150 F 470R 5% TU30 E34... |
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...