Brookfield DV-E Viscometer Instrukcja Użytkownika Strona 19

  • Pobierz
  • Dodaj do moich podręczników
  • Drukuj
  • Strona
    / 37
  • Spis treści
  • BOOKMARKI
  • Oceniono. / 5. Na podstawie oceny klientów
Przeglądanie stron 18
Brookeld Engineering Labs., Inc. Page 19 Manual No. M98-350-J0912
In taking viscosity measurements with the DV-E Viscometer, there are two considerations which
pertain to the low viscosity limit of effective measurement.
1) Viscosity measurements should be accepted within the equivalent % Torque Range from
10% to 100% for any combination of spindle/speed rotation.
2) Viscosity measurements should be taken under laminar ow conditions, not under turbulent
ow conditions.
The rst consideration has to do with the accuracy of the instrument. All DV-E Viscometers have a
full scale range accuracy of (+/-) 1% of any spindle/speed rotation. We discourage taking readings
below 10% of range because the potential viscosity error of (+/-) 1% is a relatively high number
compared to the instrument reading.
The second consideration involves the mechanics of uid ow. All rheological measurements of
uid ow properties should be made under laminar ow conditions. Laminar ow is ow wherein
all particle movement is in layers directed by the shearing force. For rotational systems, this means
all uid movement must be circumferential. When the inertial forces on the uid become too great,
the uid can break into turbulent ow wherein the movement of uid particles becomes random
and the ow can not be analyzed with standard math models. This turbulence creates a falsely high
viscometer reading with the degree of non-linear increase in reading being directly related to the
degree of turbulence in the uid.
For the following geometries, we have found that an approximate transition point to turbulent ow
occurs:
1) No. 1 LV Spindle: 15 cP at 60 RPM
2) No. 1 RV (optional) Spindle: 100 cP at 50 RPM
3) UL Adapter: 0.85 cP at 60 RPM
Turbulent conditions will exist in these situations whenever the RPM/cP ratio exceeds the values listed
above. The viscosity at which turbulence starts is still at best a guess. Because it is a relationship
between viscous and inertial forces, it can vary dramatically from uid to uid. Turbulence starts
as a small deviation or increase in viscosity for a Newtonian uid. Basically there is no specic
shear that it starts at, only an approximate region of shear depending on the uid.
Przeglądanie stron 18
1 2 ... 14 15 16 17 18 19 20 21 22 23 24 ... 36 37

Komentarze do niniejszej Instrukcji

Brak uwag