PRODUCTS
  • KLINGER Termiske masseflowmår BL 1
  • Termiske masseflowmår component by Klinger 2
  • Termiske masseflowmår connected with rod 3
  • KLINGER Termiske masseflowmår BL 0
  • Termiske masseflowmår component by Klinger 1
  • Termiske masseflowmår connected with rod 2

Thermall Massflowmeter

Klinger STG is a Thermal mass flow meter, based on the thermal dispersion principle, which can be used for measuring on clean dry gases.

STG is delivered in different versions, but common to them all is that the two temperature sensors (bodies) are located at the tip of an insertion sensor, which must be placed where the flow is desired to be monitored. This means that the sensor part itself constitutes only a slight restriction in the pipe system, and therefore it will be suitable for working at very low operating pressures.

  • Wide measuring Span, typical 100:1
  • Independent of variations in pressure and temperature 
  • Direct reading in Mass- or Compensated Volmeflow

 

Generel data

 

Type: 

Klinger STG-I (Insertion) Klinger STG-F (Flanged)

Dimensions: DN10 to DN4.000mm
Process Connections: Flanged or Weld in stud (Hot tap are available)
Wetted parts: Stainless Steel (304 eller 316)
Ranges: 0,1 ... 100 Nm/s
Accuracy: ± 1% .... 2,5% of Measured value
Power Supply: 24VDC (± 15%) or 220VAC
Output: 4 til 20mA max load 500 Ohm
  Pulse
  2 x relay  NO, 10A/220V/AC eller 5A/30V/DC
Communication (Option) RS485 / HART

 

NOTE - Thermal masseflowmeters are only for clean and dry gasses (Not Acethylene) 

 

 


 

 

Type: STG

  • Datablad (DK)
  • Datablad (UK)
  • Manual (UK)
  • Kontakt osContact us

Thermal Massflowmeters

Thermal flow meters / switches are based on the thermal dispersion principle, a principle that describes how a heated body cools when a medium passes.


If the principle is to be used for flow measurement, it is done by controlling the heating of a body in the medium, as the heating is controlled so that there is always a constant difference temperature with an identically designed reference outside the medium, then the power to be used for heating will be proportional to the mass flow of the medium.

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