RN65D3481FBSL Allicdata Electronics
Allicdata Part #:

RN65D3481FBSL-ND

Manufacturer Part#:

RN65D3481FBSL

Price: $ 0.75
Product Category:

Resistors

Manufacturer: Vishay Dale
Short Description: RES 3.48K OHM 1/2W 1% AXIAL
More Detail: 3.48 kOhms ±1% 0.5W, 1/2W Through Hole Resistor Ax...
DataSheet: RN65D3481FBSL datasheetRN65D3481FBSL Datasheet/PDF
Quantity: 1000
100 +: $ 0.68040
300 +: $ 0.58320
500 +: $ 0.48600
1000 +: $ 0.42120
5000 +: $ 0.40824
Stock 1000Can Ship Immediately
$ 0.75
Specifications
Series: Military, MIL-R-10509/2, RN65
Packaging: Bulk 
Part Status: Active
Resistance: 3.48 kOhms
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: --
Description

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

RN65D3481FBSL Application Field and Working Principle

Through hole resistors, ranging from low power to high power, are widely used in a variety of applications. The RN65D3481FBSL, a typical through hole resistor, is a vitreous enamel coated 5W resistor which is suitable for use in applications such as telecoms, motors, instruments, power supplies and more.

The Construction of RN65D3481FBSL

The RN65D3481FBSL resistor is composed of two parts: a ceramic core and a metal lead. The core is made of a ceramic-based material filled with carbon or metallic powder coat. This powder coating creates a stable and uniform resistive path for electrical current passing through it. The metal lead is made of a non-magnetic material, such as copper, which reduces the eddy current effect caused by the high current passing through the resistor. This combination of core materials and lead materials makes the RN65D3481FBSL resistor highly suitable for use in high frequency and high power applications.

Application Fields of RN65D3481FBSL

Due to its low temperature coefficient, the RN65D3481FBSL is well suited for applications which require high accuracy and stability. The low temperature coefficient (0.02%) provides excellent temperature compensation and temperature stability when operating over wide temperature ranges. Furthermore, the RN65D3481FBSL is rated at 5W and can withstand high power loads. This makes it suitable for use in applications such as telecoms, motors, instruments, power supplies and more.

Working Principle of RN65D3481FBSL

The working principle of a through hole resistor is the same as that of any other resistor. It functions as a voltage divider, dividing the applied voltage across its terminals according to its resistive value. The terminals of a through hole resistor are designed to be able to withstand high power, and thus are insulated with a vitreous enamel coating. This protects the metal lead from heat dissipation and oxidation which may occur during its operation. When a voltage is applied to the terminals, the ceramic core and the surrounding metal lead resist the flow of current according to the resistance value of the resistor. The current through the resistor is proportional to the voltage applied across the terminals, known as Ohm\'s Law. The Ohm\'s Law states that the voltage across the terminals is proportional to the current passing through the resistor, as expressed in this formula: V = I*R, where V is the voltage, I is the current and R is the resistance of the resistor.

Conclusion

The RN65D3481FBSL is a 5W through hole resistor which is suitable for use in applications such as telecoms, motors, instruments, power supplies and more. Its low temperature coefficient (0.02%), combined with its high power rating, makes it an ideal choice for many applications. Furthermore, the principle of operation of the RN65D3481FBSL is the same as for any other resistor, using Ohm\'s Law to determine the voltage across its terminals according to the current passing through it.

The specific data is subject to PDF, and the above content is for reference

Related Products
Search Part number : "RN65" Included word is 40
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...
Latest Products
SQM700JB-68K

RES WW 7W 5% TH68 kOhms 5% 7W Through Ho...

SQM700JB-68K Allicdata Electronics
SQM700JB-1R3

RES WW 7W 5% TH1.3 Ohms 5% 7W Through Ho...

SQM700JB-1R3 Allicdata Electronics
RNC60J24R9FSB14

RES 24.9 OHM 1/4W 1% AXIAL24.9 Ohms 1% 0...

RNC60J24R9FSB14 Allicdata Electronics
RWR89S2R80DRS70

RES 2.8 OHM 3W 0.5% WW AXIAL2.8 Ohms 0.5...

RWR89S2R80DRS70 Allicdata Electronics
RNC60J7503FSB14

RES 750K OHM 1/4W 1% AXIAL750 kOhms 1% 0...

RNC60J7503FSB14 Allicdata Electronics
RWR81S3400FSB12

RES 340 OHM 1W 1% WW AXIAL340 Ohms 1% 1W...

RWR81S3400FSB12 Allicdata Electronics