| Allicdata Part #: | LT50J-10K-ND |
| Manufacturer Part#: |
LTO050F10001JTE3 |
| Price: | $ 3.81 |
| Product Category: | Resistors |
| Manufacturer: | Vishay Sfernice |
| Short Description: | RES 10K OHM 50W 5% TO220 |
| More Detail: | 10 kOhms ±5% 50W Through Hole Resistor TO-220-2 No... |
| DataSheet: |  LTO050F10001JTE3 Datasheet/PDF |
| Quantity: | 520 |
| 1 +: | $ 3.46050 |
| 10 +: | $ 3.24225 |
| 100 +: | $ 2.30553 |
| 1000 +: | $ 1.89943 |
| Series: | LTO 50 |
| Packaging: | Tube |
| Part Status: | Active |
| Resistance: | 10 kOhms |
| 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 are one of the most commonly used components in electrical engineering. The LTO050F10001JTE3 is a Through Hole Resistor specially designed for high-performance applications. It has a voltage rating of up to 24 V and a power rating of up to 25 W.
The LTO050F10001JTE3 is a high-precision, high-stability resistor with low noise, good stability and low temperature drift. It is manufactured using advanced S-type annealed wire wound element technology. The unique S-type annealed wire winding element ensures that the resistor has excellent performance in high frequency applications.
The LTO050F10001JTE3 is used in a wide variety of applications. It is often used in automotive, industrial, and consumer electronics products. It is also used in many high accuracy, precision voltage and current measurement devices and power conditioning equipment.
The main advantage of the LTO050F10001JTE3 is its excellent temperature characteristics. The resistor has excellent stability over a wide temperature range, from -55°C to +125°C. It also has an impressive +/- 0.5% maximum resistance tolerance, ensuring a very high degree of accuracy and precision.
The working principle of the LTO050F10001JTE3 is relatively simple. The resistor is a four-layer component, comprised of a base layer, a winding layer, a thermal insulation layer, and a top layer. The winding layer is made of annealed wire and is wound in a serpentine shape. This arrangement gives the resistor its excellent stability and precision.
The LTO050F10001JTE3 resistor is a reliable, high-performance Through Hole Resistor that is well suited for a wide range of high-precision applications. Its high temperature stability, low noise, and good stability make it a great choice for many different applications. In addition, its unique S-type annealed wire winding element ensures excellent performance in high frequency 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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