Allicdata Part #: | RT50J-330-ND |
Manufacturer Part#: |
RTO050F330R0JTE1 |
Price: | $ 4.75 |
Product Category: | Resistors |
Manufacturer: | Vishay Sfernice |
Short Description: | RES 330 OHM 50W 5% TO220 |
More Detail: | 330 Ohms ±5% 50W Through Hole Resistor TO-220-2 No... |
DataSheet: | RTO050F330R0JTE1 Datasheet/PDF |
Quantity: | 1000 |
1 +: | $ 4.32000 |
10 +: | $ 4.04955 |
100 +: | $ 2.87973 |
1000 +: | $ 2.37249 |
Series: | RTO 50 |
Packaging: | Tube |
Part Status: | Active |
Resistance: | 330 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: | 0.398" L x 0.177" W (10.10mm x 4.50mm) |
Height - Seated (Max): | 0.591" (15.00mm) |
Number of Terminations: | 2 |
Failure Rate: | -- |
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Through hole resistors are essential components in electrical and electronic circuits, used to introduce a known resistance into a circuit. As such, they are widely used in industries ranging from aerospace to automotive and from medical to military. The RTO050F330R0JTE1 is an example of a through hole resistor that offers a high tolerance, non-inductive option with very low temperature coefficients and long-term stability.
RTO050F330R0JTE1 Application Field
The RTO050F330R0JTE1 resistor is a non-inductive through hole resistor, designed for use in applications that require higher power or current handling than conventional chips. Examples of these applications include switched-mode power supplies, power converters, high-current power amplifiers, medical equipment, and automotive systems. The RTO050F330R0JTE1 resistor is also used in both consumer and professional audio systems, as it is designed to withstand high voltage transients and power surges.
In addition to its use in high-power circuits, the RTO050F330R0JTE1 is also used in precision applications. As a non-inductive resistor, it is not affected by external interfering fields, making it ideal for instrumentation, measurement circuits, professional audio gear, and critical operational areas of computers and networks.
RTO050F330R0JTE1 Working Principle
The RTO050F330R0JTE1 is constructed from a high-purity ceramic substrate, onto which a metal-alloy film is deposited. This alloy film is patterned to create the desired resistance value, and a protective coating is then applied to cover the film. The combination of the metal-alloy film and the ceramic substrate results in a very stable resistor with high power and current handling capability.
The RTO050F330R0JTE1 offers excellent electrical performance, with a low temperature coefficient and very long-term stability. It also offers very low inductance values, which helps to reduce the noise generated in high-current circuits. In addition, its high power rating makes it suitable for use in high-power applications such as power supplies and amplifiers.
The RTO050F330R0JTE1 also offers a very high tolerance, with a maximum deviation of ±2%. This means the resistance can remain within 2% of the specified value, making it ideal for use in precision applications. Finally, the RTO050F330R0JTE1 has a wider operating temperature range than most other resistors, covering -55°C to +150°C.
Conclusion
The RTO050F330R0JTE1 is an example of a through hole resistor that offers excellent performance and reliability with high power, low inductance, and high tolerance. It is used in a wide range of applications, from high-power switching circuits to precision instrumentation. Its wide operating temperature range and long-term stability make it an ideal choice for a variety of applications.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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RTO020F10R00JTE3 | Vishay Sfern... | 4.07 $ | 159 | RES 10 OHM 20W 5% TO22010... |
RTO050F3R900JTE1 | Vishay Sfern... | 4.75 $ | 1083 | RES 3.9 OHM 50W 5% TO2203... |
RTO020F100R0JTE3 | Vishay Sfern... | 4.07 $ | 616 | RES 100 OHM 20W 5% TO2201... |
RTO020F470R0JTE3 | Vishay Sfern... | 4.07 $ | 588 | RES 470 OHM 20W 5% TO2204... |
RTO020F47R00JTE3 | Vishay Sfern... | 4.07 $ | 63 | RES 47 OHM 20W 5% TO22047... |
RTO020F10001JTE3 | Vishay Sfern... | 4.07 $ | 391 | RES 10K OHM 20W 5% TO2201... |
RTO020F47000JTE3 | Vishay Sfern... | 4.07 $ | 220 | RES 4.7K OHM 20W 5% TO220... |
RTO020F1R000JTE3 | Vishay Sfern... | 4.07 $ | 151 | RES 1 OHM 20W 5% TO2201 O... |
RTO020F22000JTE3 | Vishay Sfern... | 4.07 $ | 124 | RES 2.2K OHM 20W 5% TO220... |
RTO020F3R900JTE3 | Vishay Sfern... | 4.07 $ | 116 | RES 3.9 OHM 20W 5% TO2203... |
RTO050F15R00JTE1 | Vishay Sfern... | -- | 1528 | RES 15 OHM 50W 5% TO22015... |
RTO050F12R00JTE1 | Vishay Sfern... | 4.75 $ | 1314 | RES 12 OHM 50W 5% TO22012... |
RTO050F2R000JTE1 | Vishay Sfern... | 4.75 $ | 880 | RES 2 OHM 50W 5% TO2202 O... |
RTO050F100R0JTE1 | Vishay Sfern... | 4.75 $ | 211 | RES 100 OHM 50W 5% TO2201... |
RTO050F4R700JTE1 | Vishay Sfern... | 4.75 $ | 140 | RES 4.7 OHM 50W 5% TO2204... |
RTO050F15000JTE1 | Vishay Sfern... | 4.75 $ | 104 | RES 1.5K OHM 50W 5% TO220... |
RTO020FR1000JTE3 | Vishay Sfern... | -- | 1005 | RES 0.1 OHM 20W 5% TO2201... |
RTO020FR0680JTE3 | Vishay Sfern... | 4.87 $ | 163 | RES 0.068 OHM 20W 5% TO22... |
RTO020F4R700JTE3 | Vishay Sfern... | 4.07 $ | 1000 | RES 4.7 OHM 20W 5% TO2204... |
RTO020F22R00JTE3 | Vishay Sfern... | 4.07 $ | 1000 | RES 22 OHM 20W 5% TO22022... |
RTO050F10R00JTE1 | Vishay Sfern... | 4.75 $ | 1000 | RES 10 OHM 50W 5% TO22010... |
RTO020F2R200JTE3 | Vishay Sfern... | 4.07 $ | 11 | RES 2.2 OHM 20W 5% TO2202... |
RTO020F56R00JTE3 | Vishay Sfern... | 4.07 $ | 1000 | RES 56 OHM 20W 5% TO22056... |
RTO050F330R0JTE1 | Vishay Sfern... | 4.75 $ | 1000 | RES 330 OHM 50W 5% TO2203... |
RTO050F47R00JTE1 | Vishay Sfern... | 4.75 $ | 1000 | RES 47 OHM 50W 5% TO22047... |
RTO050FR2000JTE1 | Vishay Sfern... | 4.75 $ | 26 | RES 0.2 OHM 50W 5% TO2202... |
RTO020F220R0JTE3 | Vishay Sfern... | 4.07 $ | 100 | RES 220 OHM 20W 5% TO2202... |
RTO020F12R00JTE3 | Vishay Sfern... | 4.07 $ | 1000 | RES 12 OHM 20W 5% TO22012... |
RTO020F10002JTE3 | Vishay Sfern... | 4.07 $ | 45 | RES 100K OHM 20W 5% TO220... |
RTO050F22R00JTE1 | Vishay Sfern... | 4.75 $ | 78 | RES 22 OHM 50W 5% TO22022... |
RTO050F56R00JTE1 | Vishay Sfern... | 4.75 $ | 46 | RES 56 OHM 50W 5% TO22056... |
RTO050F10000JTE1 | Vishay Sfern... | 4.75 $ | 40 | RES 1K OHM 50W 5% TO2201 ... |
RTO050F47000JTE1 | Vishay Sfern... | 4.75 $ | 34 | RES 4.7K OHM 50W 5% TO220... |
RTO050FR1000JTE1 | Vishay Sfern... | 5.7 $ | 54 | RES 0.1 OHM 50W 5% TO2201... |
RTO020F15R00JTE3 | Vishay Sfern... | 4.07 $ | 78 | RES 15 OHM 20W 5% TO22015... |
RTO020F680R0JTE3 | Vishay Sfern... | 4.07 $ | 35 | RES 680 OHM 20W 5% TO2206... |
RTO050F2R200JTE1 | Vishay Sfern... | 4.75 $ | 40 | RES 2.2 OHM 50W 5% TO2202... |
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