Allicdata Part #: | RNMF12FTC6R80-ND |
Manufacturer Part#: |
RNMF12FTC6R80 |
Price: | $ 0.03 |
Product Category: | Resistors |
Manufacturer: | Stackpole Electronics Inc. |
Short Description: | RES 6.8 OHM 1/2W 1% AXIAL |
More Detail: | 6.8 Ohms ±1% 0.5W, 1/2W Through Hole Resistor Axia... |
DataSheet: | RNMF12FTC6R80 Datasheet/PDF |
Quantity: | 1000 |
5000 +: | $ 0.02052 |
Series: | RNMF |
Packaging: | Tape & Reel (TR) |
Part Status: | Active |
Resistance: | 6.8 Ohms |
Tolerance: | ±1% |
Power (Watts): | 0.5W, 1/2W |
Composition: | Metal Film |
Features: | Flame Retardant Coating, Safety |
Temperature Coefficient: | ±50ppm/°C |
Operating Temperature: | -55°C ~ 155°C |
Package / Case: | Axial |
Supplier Device Package: | Axial |
Size / Dimension: | 0.093" Dia x 0.250" L (2.35mm x 6.35mm) |
Height - Seated (Max): | -- |
Number of Terminations: | 2 |
Failure Rate: | -- |
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The RNMF12FTC6R80 Through Hole Resistors (THRs) are commonly used in a variety of electronic applications, from medical equipment to consumer electronics. While they may appear to have little in common, they all require an external component to form a complete circuit. The RNMF12FTC6R80 is a high-power THR used in almost all commercial electronic applications. It consists of two metal electrodes separated by a ceramic resistive film. The film is held onto the titanium substrate using a conductive adhesive. This resistor is designed to handle large currents with minimal heating and has a high resistance range.
RNMF12FTC6R80 Through Hole Resistors have become increasingly popular in the electronics industry due to their low profile, wide resistance range, and high performance. In addition to being used in most commercial applications, through-hole resistors are also commonly used in industrial applications, automotive applications, and laboratory equipment. They are also well suited to applications which require very high operating temperatures.
The working principle behind a THR is relatively simple. Electrical current flowing in one direction is opposed by a dynamic resistance. This resistance is determined by the resistance of the resistor body, the thickness of the resistive film, and the distance between the terminals. The distance between the terminals does not change in this model of THR, but the resistance still varies with the amount of current applied.
RNMF12FTC6R80 Through Hole Resistors are available in a variety of resistive values, from 0.01 ohm to 100 ohm. To calculate the amount of current resistance applied, two variables are used: the ohmic value (Ohm’s law) and the resistance of the resistive film. Ohm’s laws states that current is the ratio of the voltage through a circuit to the resistance of the circuit. The equation for calculating the resistance of a resistor is R=V/I, where R is the resistance, V is the voltage, and I is the current. For a THR, the voltage is the same as the power supply voltage and the current is the amount of current flowing through the device.
RNMF12FTC6R80 Through Hole Resistors are also available in a variety of formats depending on the application. These include the traditional axial, radial, and surface mount forms, as well as chip-type resistors. Surface-mount resistors are suitable for applications where space is limited and mounting a THR would be difficult. Chip-type resistors are ideal for applications that require precision or require a small form factor.
RNMF12FTC6R80 Through Hole Resistors have found widespread use in the electronics industry due to their simple design, wide variety of applications, and robust construction. They have become a reliable and cost-effective solution for applications that require large current handling capacity and high performance. As technology continues to advance, THR technology will become increasingly more important in a variety of applications. It is no wonder that it is quickly becoming an industry standard for commercial device manufacturing.
The specific data is subject to PDF, and the above content is for reference
Part Number | Manufacturer | Price | Quantity | Description |
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RNMF14FTD1K40 | Stackpole El... | 0.01 $ | 1000 | RES 1.4K OHM 1/4W 1% AXIA... |
RNMF14FTD2K74 | Stackpole El... | 0.01 $ | 1000 | RES 2.74K OHM 1/4W 1% AXI... |
RNMF14FAD3K30 | Stackpole El... | 0.01 $ | 1000 | RES 3.3K OHM 1/4W 1% AXIA... |
RNMF14FTD56R2 | Stackpole El... | 0.01 $ | 1000 | RES 56.2 OHM 1/4W 1% AXIA... |
RNMF14FTD180K | Stackpole El... | 0.01 $ | 1000 | RES 180K OHM 1/4W 1% AXIA... |
RNMF14FTC681K | Stackpole El... | 0.01 $ | 1000 | RES 681K OHM 1/4W 1% AXIA... |
RNMF12FTD100R | Stackpole El... | 0.01 $ | 1000 | RES 100 OHM 1/2W 1% AXIAL... |
RNMF12FTD5K11 | Stackpole El... | 0.01 $ | 1000 | RES 5.11K OHM 1/2W 1% AXI... |
RNMF12FTC130R | Stackpole El... | 0.01 $ | 1000 | RES 130 OHM 1/2W 1% AXIAL... |
RNMF12DTC69K8 | Stackpole El... | 0.03 $ | 1000 | RES 69.8K OHM 1/2W .5% AX... |
RNMF12DTC750K | Stackpole El... | 0.03 $ | 1000 | RES 750K OHM 1/2W .5% AXI... |
RNMF12DTC10R0 | Stackpole El... | 0.03 $ | 1000 | RES 10 OHM 1/2W .5% AXIAL... |
RNMF12DTC1M00 | Stackpole El... | 0.03 $ | 1000 | RES 1M OHM 1/2W .5% AXIAL... |
RNMF12DAC1M00 | Stackpole El... | 0.03 $ | 1000 | RES 1M OHM 1/2W 0.5% AXIA... |
RNMF14DTC180K | Stackpole El... | 0.03 $ | 1000 | RES 180K OHM 1/4W 0.5% AX... |
RNMF12FTC2R20 | Stackpole El... | 0.03 $ | 1000 | RES 2.2 OHM 1/2W 1% AXIAL... |
RNMF12FAD2R20 | Stackpole El... | 0.03 $ | 1000 | RES 2.2 OHM 1/2W 1% AXIAL... |
RNMF12FAC3R30 | Stackpole El... | 0.03 $ | 1000 | RES 3.3 OHM 1/2W 1% AXIAL... |
RNMF12FTC3R90 | Stackpole El... | 0.03 $ | 1000 | RES 3.9 OHM 1/2W 1% AXIAL... |
RNMF12FTC4R70 | Stackpole El... | 0.03 $ | 1000 | RES 4.7 OHM 1/2W 1% AXIAL... |
RNMF12FTC6R80 | Stackpole El... | 0.03 $ | 1000 | RES 6.8 OHM 1/2W 1% AXIAL... |
RNMF12FAC6R80 | Stackpole El... | 0.03 $ | 1000 | RES 6.8 OHM 1/2W 1% AXIAL... |
RNMF12FTC1R62 | Stackpole El... | 0.03 $ | 1000 | RES 1.62 OHM 1/2W 1% AXIA... |
RNMF12FAC2R20 | Stackpole El... | 0.03 $ | 1000 | RES 2.2 OHM 1/2W 1% AXIAL... |
RNMF12FTC2R61 | Stackpole El... | 0.03 $ | 1000 | RES 2.61 OHM 1/2W 1% AXIA... |
RNMF12FTC3R32 | Stackpole El... | 0.03 $ | 1000 | RES 3.32 OHM 1/2W 1% AXIA... |
RNMF12FAC3R90 | Stackpole El... | 0.03 $ | 1000 | RES 3.9 OHM 1/2W 1% AXIAL... |
RNMF12FTC4R64 | Stackpole El... | 0.03 $ | 1000 | RES 4.64 OHM 1/2W 1% AXIA... |
RNMF12FAC4R70 | Stackpole El... | 0.03 $ | 1000 | RES 4.7 OHM 1/2W 1% AXIAL... |
RNMF12FTC6R81 | Stackpole El... | 0.03 $ | 1000 | RES 6.81 OHM 1/2W 1% AXIA... |
RNMF12CTD33K2 | Stackpole El... | 0.04 $ | 1000 | RES 33.2K OHM 1/2W .25% A... |
RNMF12CTD100R | Stackpole El... | 0.04 $ | 1000 | RES 100 OHM 1/2W .25% AXI... |
RNMF14BTC100K | Stackpole El... | 0.09 $ | 1000 | RES 100K OHM 1/4W 0.1% AX... |
RNMF12CTD1K10 | Stackpole El... | 0.05 $ | 1000 | RES 1.1K OHM 1/2W .25% AX... |
RNMF12CTC33K2 | Stackpole El... | 0.05 $ | 1000 | RES 33.2K OHM 1/2W .25% A... |
RNMF12CTC100K | Stackpole El... | 0.05 $ | 1000 | RES 100K OHM 1/2W .25% AX... |
RNMF14BTE68K0 | Stackpole El... | 0.11 $ | 1000 | RES 68K OHM 1/4W .1% AXIA... |
RNMF14BTE100K | Stackpole El... | 0.11 $ | 1000 | RES 100K OHM 1/4W 0.1% AX... |
RNMF12BTE10K2 | Stackpole El... | 0.12 $ | 1000 | RES 10.2K OHM 1/2W 0.1% A... |
RNMF12BTE7K50 | Stackpole El... | 0.12 $ | 1000 | RES 7.5K OHM 1/2W 0.1% AX... |
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...