
Allicdata Part #: | RN65E2320BBSL-ND |
Manufacturer Part#: |
RN65E2320BBSL |
Price: | $ 1.03 |
Product Category: | Resistors |
Manufacturer: | Vishay Dale |
Short Description: | RES 232 OHM 1/2W .1% AXIAL |
More Detail: | 232 Ohms ±0.1% 0.5W, 1/2W Through Hole Resistor Ax... |
DataSheet: | ![]() |
Quantity: | 1000 |
100 +: | $ 0.93744 |
300 +: | $ 0.80352 |
500 +: | $ 0.66960 |
1000 +: | $ 0.58032 |
5000 +: | $ 0.56247 |
Series: | Military, MIL-R-10509/2, RN65 |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 232 Ohms |
Tolerance: | ±0.1% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Metal Film |
Features: | Flame Retardant Coating, Military, Moisture Resistant, Safety |
Temperature Coefficient: | ±25ppm/°C |
Operating Temperature: | -65°C ~ 175°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.180" Dia x 0.562" L (4.57mm x 14.27mm) |
Height - Seated (Max): | -- |
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, or THRs, are a type of electrical resistor designed to provide long-term reliability and durability in electrical systems. The RN65E2320BBSL is a THR available from Panasonic Corporation, designed for use in industrial, automotive, and consumer electronics applications. This article will provide a discussion of the RN65E2320BBSL’s intended applications field, as well as a brief overview of its internal working principle.
Applications
The RN65E2320BBSL is manufactured to JEDEC standards for use in industrial, automotive, and consumer electronics applications. It is also designed for use under operating temperatures of –55°C to +150°C, making it suitable for various types of communications applications. Devices utilizing this THR can be found in a variety of applications, including mobile phones, automotive electronic circuits, control systems, and power supplies.
The RN65E2320BBSL is available in a variety of sizes and shapes, including full size SMT and Through Hole. It also features a tolerance of ±5% as well as low temperature coefficient of resistance (TCR). This makes it well-suited for use in precision circuits where high accuracy is required.
Working Principle
Like other THRs, the RN65E2320BBSL utilizes a fixed resistor which has an insulated case and leads that make it easy to mount. The resistor’s body is typically made from ceramic, and the leads are usually made of metal. A small wooden bridge is added to the resistor in order to ensure an electrical connection between the resistor case and the leads.
The RN65E2320BBSL is designed to resist the flow of electricity by creating resistance when a current is applied. This is done by increasing the amount of energy required for electricity to travel through the resistor. The result is that the current is weakened, thus protecting sensitive components and electronics that are connected to the circuit.
The RN65E2320BBSL’s resistance can be adjusted through the use of a potentiometer. This device has three terminals: one for the voltage source, one for the resistor, and one for the load. By adjusting the potentiometer, the desired resistance can be set and the current can be limited as needed.
Conclusion
In conclusion, the RN65E2320BBSL is a THR manufactured by Panasonic Corporation that is designed for a variety of industrial, automotive, and consumer electronics applications. It is designed to resist the flow of electricity and provide long-term reliability and durability. Additionally, this THR is available in a variety of sizes and shapes, and it features a tolerance of ±5% and a low temperature coefficient of resistance.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
---|
RN65D40R2FR36 | Vishay Dale | 0.14 $ | 1000 | RES 40.2 OHM 1/2W 1% AXIA... |
RN65D56R2FR36 | Vishay Dale | 0.14 $ | 1000 | RES 56.2 OHM 1/2W 1% AXIA... |
RN65D1362FRE6 | Vishay Dale | 0.15 $ | 1000 | RES 13.6K OHM 1/2W 1% AXI... |
RN65D12R5FB14 | Vishay Dale | 0.15 $ | 1000 | RES 12.5 OHM 1/2W 1% AXIA... |
RN65D4120FRE6 | Vishay Dale | 0.15 $ | 1000 | RES 412 OHM 1/2W 1% AXIAL... |
RN65D1651FRE6 | Vishay Dale | 0.15 $ | 1000 | RES 1.65K OHM 1/2W 1% AXI... |
RN65D1070FRE6 | Vishay Dale | 0.15 $ | 1000 | RES 107 OHM 1/2W 1% AXIAL... |
RN65D8002FRE6 | Vishay Dale | 0.15 $ | 1000 | RES 80K OHM 1/2W 1% AXIAL... |
RN65C6810FR36 | Vishay Dale | 0.16 $ | 1000 | RES 681 OHM 1/2W 1% AXIAL... |
RN65C6341FRE6 | Vishay Dale | 0.16 $ | 1000 | RES 6.34K OHM 1/2W 1% AXI... |
RN65C2552FRE6 | Vishay Dale | 0.16 $ | 1000 | RES 25.5K OHM 1/2W 1% AXI... |
RN65C4021FRE6 | Vishay Dale | 0.16 $ | 1000 | RES 4.02K OHM 1/2W 1% AXI... |
RN65C2502DB14 | Vishay Dale | 0.2 $ | 1000 | RES 25K OHM 1/2W .5% AXIA... |
RN65E3302FRE6 | Vishay Dale | 0.21 $ | 1000 | RES 33K OHM 1/2W 1% AXIAL... |
RN65E3300FRE6 | Vishay Dale | 0.21 $ | 1000 | RES 330 OHM 1/2W 1% AXIAL... |
RN65D13R3FRSL | Vishay Dale | 0.23 $ | 1000 | RES 13.3 OHM 1/2W 1% AXIA... |
RN65D4123FRSL | Vishay Dale | 0.23 $ | 1000 | RES 412K OHM 1/2W 1% AXIA... |
RN65D1960FRSL | Vishay Dale | 0.23 $ | 1000 | RES 196 OHM 1/2W 1% AXIAL... |
RN65D48R7FRSL | Vishay Dale | 0.23 $ | 1000 | RES 48.7 OHM 1/2W 1% AXIA... |
RN65D2802FRSL | Vishay Dale | 0.23 $ | 1000 | RES 28K OHM 1/2W 1% AXIAL... |
RN65D7501FRSL | Vishay Dale | 0.23 $ | 1000 | RES 7.5K OHM 1/2W 1% AXIA... |
RN65D7502FRSL | Vishay Dale | 0.23 $ | 1000 | RES 75K OHM 1/2W 1% AXIAL... |
RN65C4990BR36 | Vishay Dale | 0.25 $ | 1000 | RES 499 OHM 1/2W .1% AXIA... |
RN65D1254FRE6 | Vishay Dale | 0.26 $ | 1000 | RES 1.25M OHM 1/2W 1% AXI... |
RN65E4001BB14 | Vishay Dale | 0.3 $ | 1000 | RES 4K OHM 1/2W .1% AXIAL... |
RN65E1501BRSL | Vishay Dale | 0.45 $ | 1000 | RES 1.5K OHM 1/2W .1% AXI... |
RN65C4321FB14 | Vishay Dale | 0.63 $ | 1000 | RES 4.32K OHM 1/2W 1% AXI... |
RN65C3010FB14 | Vishay Dale | 0.63 $ | 1000 | RES 301 OHM 1/2W 1% AXIAL... |
RN65C3402FB14 | Vishay Dale | 0.63 $ | 1000 | RES 34K OHM 1/2W 1% AXIAL... |
RN65D2102FB14 | Vishay Dale | 0.63 $ | 1000 | RES 21K OHM 1/2W 1% AXIAL... |
RN65E6341FB14 | Vishay Dale | 0.68 $ | 1000 | RES 6.34K OHM 1/2W 1% AXI... |
RN65C4423FBSL | Vishay Dale | 0.75 $ | 1000 | RES 442K OHM 1/2W 1% AXIA... |
RN65C5111FBSL | Vishay Dale | 0.75 $ | 1000 | RES 5.11K OHM 1/2W 1% AXI... |
RN65C2843DBSL | Vishay Dale | 0.75 $ | 1000 | RES 284K OHM 1/2W .5% AXI... |
RN65C2432FBSL | Vishay Dale | 0.75 $ | 1000 | RES 24.3K OHM 1/2W 1% AXI... |
RN65C2611FBSL | Vishay Dale | 0.75 $ | 1000 | RES 2.61K OHM 1/2W 1% AXI... |
RN65D1372FBSL | Vishay Dale | 0.75 $ | 1000 | RES 13.7K OHM 1/2W 1% AXI... |
RN65D5620FBSL | Vishay Dale | 0.75 $ | 1000 | RES 562 OHM 1/2W 1% AXIAL... |
RN65D2490FBSL | Vishay Dale | 0.75 $ | 1000 | RES 249 OHM 1/2W 1% AXIAL... |
RN65D6813FBSL | Vishay Dale | 0.75 $ | 1000 | RES 681K OHM 1/2W 1% AXIA... |
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...
