| Allicdata Part #: | 92J130E-ND |
| Manufacturer Part#: |
92J130E |
| Price: | $ 1.40 |
| Product Category: | Resistors |
| Manufacturer: | Ohmite |
| Short Description: | RES 130 OHM 2.25W 5% AXIAL |
| More Detail: | 130 Ohms ±5% 2.25W Through Hole Resistor Axial Fla... |
| DataSheet: | 92J130E Datasheet/PDF |
| Quantity: | 1000 |
| 100 +: | $ 1.26787 |
| Series: | 90 |
| Packaging: | Bulk |
| Part Status: | Active |
| Resistance: | 130 Ohms |
| Tolerance: | ±5% |
| Power (Watts): | 2.25W |
| Composition: | Wirewound |
| Features: | Flame Retardant Coating, Safety |
| Temperature Coefficient: | ±30ppm/°C |
| Operating Temperature: | -- |
| Package / Case: | Axial |
| Supplier Device Package: | Axial |
| Size / Dimension: | 0.220" Dia x 0.406" L (5.60mm x 10.30mm) |
| Height - Seated (Max): | -- |
| Number of Terminations: | 2 |
| Failure Rate: | -- |
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Through hole resistors are widely used in various electronic devices for applications involving the control and regulation of electrical signals. The 92J130E is a type of through hole resistor specifically designed for high-current applications, offering a higher maximum current rating than standard through hole resistors.
This type of resistor is capable of handling currents up to 10amps and is made from a combination of copper and ceramic materials for improved thermal performance. It is also designed to withstand higher temperatures than most through hole resistors, making it suitable for applications involving high heat and high current demands. One of the main advantages of this type of resistor is that it is extremely reliable, making it ideal for use in critical circuits.
The 92J130E resistor is typically used in industrial or commercial applications to provide precision voltage or current control. It is often used in power supplies, audio amplifiers, motor control systems, and more. This type of resistor has a low resistance value and is capable of withstanding high temperatures, making it suitable for a wide range of industries and applications.
The working principle of the 92J130E through hole resistor is based on Ohm’s law. According to this law, the resistance of a conductor is proportional to its length divided by its cross-sectional area. Therefore, the longer the resistor, the greater the resistance and vice-versa. To increase or decrease the resistance of the resistor, simply adjust either its length or its cross-sectional area.
The 92J130E resistor is designed for high-current applications so it is constructed with two large copper plates. The copper plates are placed in close proximity to each other and then heated. The heat causes the plates to draw closer together, reducing the overall resistance of the resistor. The current rating of the resistor is determined by the amount of heat applied to the plates and the internal resistance of the resistor.
The 92J130E resistor is an excellent choice for a wide range of applications involving high heat and high current demands. Its large size and high current ratings make it suitable for industrial and commercial applications where precision voltage and current control is needed. The resistor is extremely reliable and can withstand high temperatures, making it an ideal choice for critical circuits. The working principle of the 92J130E through hole resistor is based on Ohm’s law and its resistance can be easily adjusted by changing its length or cross-sectional area.
The specific data is subject to PDF, and the above content is for reference
| Part Number | Manufacturer | Price | Quantity | Description |
|---|
| 92J1R0 | Ohmite | 1.83 $ | 1000 | RES 1 OHM 2.25W 5% AXIAL1... |
| 92J1K5 | Ohmite | 2.01 $ | 1000 | RES 1.5K OHM 2.25W 5% AXI... |
| 92J1R5 | Ohmite | 1.83 $ | 1000 | RES 1.5 OHM 2.25W 5% AXIA... |
| 92J1K0E | Ohmite | 2.02 $ | 1000 | RES 1K OHM 2.25W 5% AXIAL... |
| 92J10R | Ohmite | 2.26 $ | 133 | RES 10 OHM 2.25W 5% AXIAL... |
| 92J18RE | Ohmite | 1.4 $ | 1000 | RES 18 OHM 2.25W 5% AXIAL... |
| 92J1R3E | Ohmite | 1.67 $ | 1000 | RES 1.3 OHM 2.25W 5% AXIA... |
| 92J160E | Ohmite | 1.4 $ | 1000 | RES 160 OHM 2.25W 5% AXIA... |
| 92J120E | Ohmite | 1.4 $ | 1000 | RES 120 OHM 2.25W 5% AXIA... |
| 92J130E | Ohmite | 1.4 $ | 1000 | RES 130 OHM 2.25W 5% AXIA... |
| 92J1K0 | Ohmite | 2.01 $ | 1000 | RES 1K OHM 2.25W 5% AXIAL... |
| 92J1K3E | Ohmite | 2.02 $ | 1000 | RES 1.3K OHM 2.25W 5% AXI... |
| 92J1R8E | Ohmite | 1.67 $ | 1000 | RES 1.8 OHM 2.25W 5% AXIA... |
| 92J1R2E | Ohmite | 1.67 $ | 1000 | RES 1.2 OHM 2.25W 5% AXIA... |
| 92J1R6E | Ohmite | 1.67 $ | 1000 | RES 1.6 OHM 2.25W 5% AXIA... |
| 92J100 | Ohmite | 1.52 $ | 1000 | RES 100 OHM 2.25W 5% AXIA... |
| 92J1R0E | Ohmite | 1.67 $ | 1000 | RES 1 OHM 2.25W 5% AXIAL1... |
| 92J100E | Ohmite | 1.4 $ | 1000 | RES 100 OHM 2.25W 5% AXIA... |
| 92J1K8E | Ohmite | 2.02 $ | 1000 | RES 1.8K OHM 2.25W 5% AXI... |
| 92J180E | Ohmite | 1.4 $ | 1000 | RES 180 OHM 2.25W 5% AXIA... |
| 92J1K4E | Ohmite | 2.02 $ | 1000 | RES 1.4K OHM 2.25W 5% AXI... |
| 92J10RE | Ohmite | 1.4 $ | 1000 | RES 10 OHM 2.25W 5% AXIAL... |
| 92J1R5E | Ohmite | 1.67 $ | 1000 | RES 1.5 OHM 2.25W 5% AXIA... |
| 92J15R | Ohmite | 1.52 $ | 1000 | RES 15 OHM 2.25W 5% AXIAL... |
| 92J1K6E | Ohmite | 2.02 $ | 1000 | RES 1.6K OHM 2.25W 5% AXI... |
| 92J13RE | Ohmite | 1.4 $ | 1000 | RES 13 OHM 2.25W 5% AXIAL... |
| 92J1K5E | Ohmite | 2.02 $ | 1000 | RES 1.5K OHM 2.25W 5% AXI... |
| 92J1K2E | Ohmite | 2.02 $ | 1000 | RES 1.2K OHM 2.25W 5% AXI... |
| 92J150E | Ohmite | 1.4 $ | 1000 | RES 150 OHM 2.25W 5% AXIA... |
| 92J1R2 | Ohmite | 1.83 $ | 1000 | RES 1.2 OHM 2.25W 5% AXIA... |
| 92J1K2 | Ohmite | 2.01 $ | 1000 | RES 1.2K OHM 2.25W 5% AXI... |
| 92J110E | Ohmite | 1.4 $ | 1000 | RES 110 OHM 2.25W 5% AXIA... |
| 92J150 | Ohmite | 1.52 $ | 1000 | RES 150 OHM 2.25W 5% AXIA... |
| 92J12RE | Ohmite | 1.4 $ | 1000 | RES 12 OHM 2.25W 5% AXIAL... |
| 92J15RE | Ohmite | 1.4 $ | 1000 | RES 15 OHM 2.25W 5% AXIAL... |
| 92J16RE | Ohmite | 1.4 $ | 1000 | RES 16 OHM 2.25W 5% AXIAL... |
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92J130E Datasheet/PDF