
Allicdata Part #: | RN65D24R9FBSL-ND |
Manufacturer Part#: |
RN65D24R9FBSL |
Price: | $ 0.75 |
Product Category: | Resistors |
Manufacturer: | Vishay Dale |
Short Description: | RES 24.9 OHM 1/2W 1% AXIAL |
More Detail: | 24.9 Ohms ±1% 0.5W, 1/2W Through Hole Resistor Axi... |
DataSheet: | ![]() |
Quantity: | 1000 |
100 +: | $ 0.68040 |
300 +: | $ 0.58320 |
500 +: | $ 0.48600 |
1000 +: | $ 0.42120 |
5000 +: | $ 0.40824 |
Series: | Military, MIL-R-10509/2, RN65 |
Packaging: | Bulk |
Part Status: | Active |
Resistance: | 24.9 Ohms |
Tolerance: | ±1% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Metal Film |
Features: | Flame Retardant Coating, Military, Moisture Resistant, Safety |
Temperature Coefficient: | ±100ppm/°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
Introduction
RN65D24R9FBSL is a type of through hole resistors that has a wide variety of applications in the industry. It has a low temperature coefficient, wide range of resistance, low noise performance, and a wide temperature range. This makes it one of the most versatile resistors in the market.
Application Field
RN65D24R9FBSL is mainly used in high frequency applications due to its low temperature coefficient, wide range of resistance, and low noise performance. It is typically used in signal processing, filtering, and precision circuits. It is also used in power systems, RF and microwave systems, audio applications, and many other applications. It is also well suited for automotive and industrial systems.
Some of the most common applications of RN65D24R9FBSL are found in audio systems. It can be used to control the power supply for audio amplifiers, power converters, and other audio systems. Additionally, it is used to provide active filtering for audio signals in order to reduce unwanted noise and distortion. It is also used in motor control systems, automotive circuits, and medical and communications systems.
Working Principle
When operating at high frequency, RN65D24R9FBSL works primarily by producing a resistance to current flow. This resistance is produced by a phenomenon called “adjustable temperature coefficient”. The adjustable temperature coefficient is a result of the changing resistive material inside the resistor, the resistor’s exact construction, and how the resistor was designed. It is the combination of these things that allows RN65D24R9FBSL to have a well regulated resistive value over a wide temperature range.
Due to its low temperature coefficient, RN65D24R9FBSL is used in many super high frequency applications because of its ability to regulate its resistive value effectively. This feature is especially beneficial for signal processing, filtering, and precision circuits because these applications often require precise resistive values.
Additionally, the wide range of resistive values makes it suitable for many types of projects. It can be used in both low-resistance and high-resistance circuits, making it suitable for a wide range of circuit types. This is important for applications like RF and microwave systems, which require precise resistive values over a wide range of frequencies.
Conclusion
In conclusion, RN65D24R9FBSL is a type of through hole resistors that has a wide variety of applications in the industry. It has a low temperature coefficient, wide range of resistance, low noise performance, and a wide temperature range. This makes it one of the most versatile resistors in the market and is well suited for applications in signal processing, filtering, and precision circuits, as well as power systems, RF and microwave systems, audio applications, automotive circuits, and medical and communications systems.
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...
