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Rapid Viscosity Process Analyzer

  • NG # 003934-HW-WIN-O34

Manufactured by:

This seller generally responds in under 48 hours

To remain competitive, today’s refiners must employ all optimization and product control techniques available. The use of online physical property analyzers is one of the key features to reach those objectives because they measure important quality properties in the process directly.

Specification

Technologycontinuously analyzing kinematic viscosity, capillary-type
Methodcompliant with: ASTM D445, DIN EN ISO 3104, IP 71
Sample at inletfiltered 10 μm or 50 μm (depending on the viscosity measuring range), bubble-free max. viscosity = end of measuring range (technical clarification required) (sample as coolant ≤ 10 cSt)
3.8 to 10 l/h (depends on variant)
3 to 14 bar (43.5 to 203 psi)
for L + M Versions: TM *-35 K<tinlet tm k for h versions: depends on td> </tinlet>
Sample at outletcan handle back pressure (on request)
Electrical datamax. 8 (4 to 20 mA; 1000 Ω); active isolated on request
4 to 20 mA; 160 Ω
24 V DC; max. 0.5 A
high: 15 to 28 V DC/low: 0 to 4 V DC
24 V DC; max. 0.8 A
CommunicationMODBUS/RTU via RS485 or RS422 or FOC is
MODBUS/TCP via FOC is
ethernet available
kinematic viscosity (others on request)
Alarm, Ready/Valid; Stream Selection, Validation Request, Reset
Ambient conditionsoperation 5 to 40 °C (41 to 104 °F) storage -20 to 60 °C (-4 to 140 °F)
operation 5 to 80 % relative humidity, non-corrosive; storage 5 to 80 % relative humidity, non-corrosive
IP 54 (comparable with NEMA 13)
HMItouch display 19"
remote access on request
cyber security
operating system Windows10 enterprise LTSB
Bartec Benke control software PACS
Process connectionstube fittings: typically Swagelok 6mm/12mm/18mm; others on request
sample inlet up to 2 sample streams and 1 validation stream
sample outlet
vent line (if required)
coolant (if required)
Weight and dimensionsapprox. 250 kg
(W x H x D) approx. 1190 x 1930 x 710 mm
free space right: 150 mm/left: 100 mm

Description

All fluids that fulfil the conditions of Newton’s friction law are referred to as Newtonian fluids. Their viscosity is a material constant, which is only dependent on pressure and temperature. The viscosity for incompressible and Newtonian fluids can be derived from the so called Hagen-Poiseuille law. The fluid is assumed to flow under laminar conditions.