Inductive Free Precision Metal Foil Sampling Resistor
In high-precision electronic circuits, the accuracy of resistance values is critical. Traditional resistors with inductance can cause unwanted effects on circuit performance. The use of inductance-free resistors, such as metal foil sample resistors, eliminates these effects and improves circuit performance.
Description
Inductance-Free Precision Metal Foil Sample Resistors
In high-precision electronic circuits, the accuracy of resistance values is critical. Traditional resistors with inductance can cause unwanted effects on circuit performance. The use of inductance-free resistors, such as metal foil sample resistors, eliminates these effects and improves circuit performance.
Metal foil resistors the thickness of the foil determines the resistor's value, which is typically very low, from fractions of an ohm to a few hundred ohms. These resistors are manufactured to extremely tight tolerances, ensuring high precision and reliability.
In addition to their inductance-free properties, metal foil sample resistors exhibit very low thermal EMF and low noise. This makes them ideal for use in precision circuits, such as amplifiers, filtering circuits, and measuring instruments.
One of the most significant advantages of metal foil sample resistors is their stability over time. They are not susceptible to drift or aging, ensuring that they maintain their accuracy and reliability over extended periods of time.
The use of metal foil sample resistors is not limited to precision circuits. They can also be used in high-frequency circuits, as their small size and low inductance make them suitable for high-speed applications.
In conclusion, metal foil sample resistors are an excellent choice for high-precision electronic circuits that require high accuracy, stability, and reliability. Their inductance-free properties, low noise, and thermal EMF make them ideal for use in amplifiers, measuring instruments, and high-speed circuits.
Metal foil sampling resistor RNG6040

Product features:
● Resistance ranges from 0.005Ω to 1000Ω
● Rated power up to 50W
● Resistance accuracy is ±0.01%
● Temperature coefficient is ±2ppm/K
● Non-inductive design
● Load stability up to 0.02%
● Load life stability: 0.02%
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Table 1-Parameters |
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mode |
RNG6040 |
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Stopped value interval |
From 0.005 to 1000Ω |
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power rating |
The heat sink is not installed70℃ |
20w |
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Add radiator |
60w |
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accuracy |
0.01%/ 0.025%/ 0.05%/ 0.1% |
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Thermal resistance |
1.6KW |
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stability (2000h) |
0.02%(Maximum variation) |
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temperature coefficient |
±10ppm/K (20 to 60℃) ±5ppm/K (20 to 60℃) ±2ppm/K (20 to 60℃) |
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Pressure resistance value |
500VDC |
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Maximum current |
50A |
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Thermoelectric potential |
<1μV/K |
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Operating temperature interval |
-40 to 130℃ |
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Resistance material |
Manganese copper, nichrome foil |
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placode |
Aluminium oxide |
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Protective layer |
Epoxy resin |
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Electrode material |
Tinned copper |
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Pin count |
4 |
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Maximum torque |
1Nm |
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| Table 1- Temperature coefficients |
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Product Temperature coefficient curve △R/RPPM |
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Figure2-The reduced power curve |
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Rated Power Note- RNG6040 Series resistance connected to a suitable radiator for use. The maximum internal temperature is 130°C. Using the following formula: Where: RθH= thermal resistance of the radiator (K / W) RθR = electric resistance of thermal resistance (K / W) TMAx = maximum resistance maximum working temperature TA = Ambient temperature of radiator (℃) P = power of resistor (W) |
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Table 3 Line connection |
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For low resistance resistance (less than 10 Ω), the increase in the resistance and temperature coefficient of the copper pin exceeds the resistance itself. A four-legged Kelvin connection is recommended, as shown in the figure below. The load current on the V-pin will cause a measurement error.
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| Figure 4-Resistsurface temperature rise curve |
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| Figure 5-Product size drawing |
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