WRN-420、 430 fixed flange assembled thermocouple
High temperature temperature sensor | Stable performance, accurate measurement | Good pressure resistance | Good interchangeability
Overview and use
Industrial assembled thermocouples are commonly used as temperature sensors in conjunction with display instruments, recording instruments, and electronic regulators. It can directly measure the surface temperature of liquids, vapors, gases, and solids in the range of 0 ℃ to 1800 ℃ during various production processes.
Working principle
Two conductors with different compositions are welded at both ends to form a circuit. The temperature measuring end is called the measuring end, and the wiring terminal is called the reference end. When there is a temperature difference between the measurement and reference ends, a thermal current will be generated in the circuit. When connected to a display instrument, the instrument will indicate the temperature value corresponding to the thermoelectric potential generated by the thermocouple. |
Working principle diagram of thermocouple |
Nominal pressure of thermocouple
Generally refers to the static external pressure that the protective tube can withstand at working temperature without breaking. In fact, the allowable working pressure is not only related to the material, diameter, and wall thickness of the protective tube, but also to its structural form, installation method, insertion depth, as well as the flow rate and type of the measured medium.
Minimum insertion depth of thermocouple
It should not be less than 8-10 times the outer diameter of its protective tube (except for special products).
Structure of Thermocouples Product Structure
From the temperature measurement principle of thermocouples, it can be known that in addition to the two thermoelectric electrode materials, the most basic thermocouple must also be made into measuring and reference ends at both ends of the thermoelectric electrode according to requirements, commonly known as the "hot end" and "cold end", which are the so-called "two ends". |
Selection of Temperature Measuring Elements for Thermocouples
Thermocouple category | Graduation | Measurement range ℃ | Allowable deviation △ t ℃ | Performance characteristics | |
advantage | disadvantage | ||||
Nickel chromium nickel silicon | K | 0~1200 | ± 2.5 ℃ or ± 0.75% t | Good thermoelectric potential, stability, and oxidation resistance, making it the most widely used temperature measuring element | Not suitable for reducing atmosphere, affected by aging changes and short-range ordered structural changes |
Nickel chromium copper nickel | E | 0~800 | ± 2.5 ℃ or ± 0.75% t | Among the existing thermocouples, the thermoelectric potential rate is the highest, the sensitivity is high, the two-stage non-magnetic thermoelectric potential has good linearity, good stability, and good oxidation resistance, making it the most widely used temperature measuring element | Not suitable for reducing atmosphere, low thermal conductivity, with slight hysteresis phenomenon. Not suitable for reducing atmosphere, affected by aging changes and short-range ordered structure changes |
Copper Copper Nickel | T | —40~350 | ± 1 ℃ or ± 0.75% t | Can be used in reducing atmospheres, with good linearity of hot spot potential, good low-temperature characteristics, and good stability | Low operating temperature, easy oxidation of positive copper, large thermal conductivity error |
Iron copper nickel | J | 0~800 | ± 2.5 ℃ or ± 0.75% t | Can be used in reducing atmospheres, with a higher thermoelectric potential than K | Iron is prone to rusting and has a large drift in thermoelectric properties |
Nickel chromium silicon nickel silicon | N | 0~1200 | ± 2.5 ℃ or ± 0.75% t | Having all the advantages of K-type thermocouples, the short-range ordered structural changes have little impact | Not suitable for reducing atmosphere, affected by aging changes |
Product selection
Model representation
Model representation Type specification
Thermocouple category | Product model | Graduation | Protective tube material | Temperature measurement range ℃ | Output | |
Single nickel chromium nickel silicon | WRN-430 | K | 304 | 0-800 | DIRECT | |
Double branch nickel chromium nickel silicon | WRN2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRNB-430 | 304 | 0-800 | 4~20mA output | ||
Double branch nickel chromium nickel silicon | WRNB2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRE-430 | E | 304 | 0-800 | DIRECT | |
Double branch nickel chromium nickel silicon | WRE2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WREB-430 | 304 | 0-800 | 4~20mA output | ||
Double branch nickel chromium nickel silicon | WREB2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRC-430 | T | 304 | 0-800 | DIRECT | |
Double branch nickel chromium nickel silicon | WRC2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRCB-430 | 304 | 0-800 | 4~20mA output | ||
Double branch nickel chromium nickel silicon | WRCB2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRF-430 | J | 304 | 0-800 | DIRECT | |
Double branch nickel chromium nickel silicon | WRF2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRFB-430 | 304 | 0-800 | 4~20mA output | ||
Double branch nickel chromium nickel silicon | WRFB2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRM-430 | T | 304 | 0-800 | DIRECT | |
Double branch nickel chromium nickel silicon | WRM2-430 | GH2520 | 0-1000 | |||
Single nickel chromium nickel silicon | WRMB-430 | 304 | 0-800 | 4~20mA output | ||
Double branch nickel chromium nickel silicon | WRMB2-430 | GH2520 | 0-1000 |
installation diagram
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