Inductive Free Precision Metal Foil Sampling Resistor
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Inductive Free Precision Metal Foil Sampling Resistor

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

1

 

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%

 

Table 1-Parameters

mode

RNG6040

Stopped value interval

From 0.005 to 1000Ω

power rating

The heat sink is not installed70℃

20w

Add radiator

60w

accuracy

0.01%/ 0.025%/ 0.05%/ 0.1%

Thermal resistance

1.6KW

stability (2000h)

0.02%(Maximum variation)

temperature coefficient

±10ppm/K (20 to 60℃)

±5ppm/K (20 to 60℃)

±2ppm/K (20 to 60℃)

Pressure resistance value

500VDC

Maximum current

50A

Thermoelectric potential

<1μV/K

Operating temperature interval

-40 to 130℃

Resistance material

Manganese copper, nichrome foil

placode

Aluminium oxide

Protective layer

Epoxy resin

Electrode material

Tinned copper

Pin count

4

Maximum torque

1Nm

 

Table 1- Temperature coefficients

2

Product Temperature coefficient curve R/RPPM

 

Figure2-The reduced power curve

product-391-280

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)

 

Table 3 Line connection

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.

4

 

Figure 4-Resistsurface temperature rise curve

product-750-431

 

Figure 5-Product size drawing

6

 

Support Customization

 

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