The basis is volumetric.
Temperature rise at low flows results from low hydraulic efficiencies (effy in decimals) as energy is lost in friction. Sulzer's formula for the temperature rise in
oC:
(0.00981/c)(Head, m)[(1/effy)-1]
where c is the specific heat of the incompressible fluid expressed in kJ/(kg.K); for organics this value is about half of that for water usually taken at 4.18; while 0.00981 is the acceleration of gravity 9.81 m/s
2 divided by 1,000 to convert kJ into J.
As you may see, the "heat up" formula already includes the liquid density in the Head factor (=pressure divided by density).
BTW, I've checked it, and the formula is dimensionally consistent:
(m/s
2)(m)(kg.K)/(J)=(m/s
2)(m)(kg.K)/(kg.m
2/s
2)=K
There is more heat up from throttling the liquid in the clearance of the axial thrust balancing device taken as
(0.00981/c)(Head, m)(1/effy.)
Both results are taken together when determining minimum flow.
Sulzer lists the
criteria for minimum flow without sustaining any damage, as follows, I quote:
-temperature rise due to internal energy loss,
-internal recirculation in the impeller (whit large
impeller inlet dia. compared with the outside dia., NPSH
rises in the part-load range),
-increased vibration due to greater flow separation,
-increased pressure fluctuation at part load,
-increased axial thrust at low flow rates,
-increased radial thrust (especially with single volute
pumps).
Sulzer continues saying -among other statements for high head and high kW pumps- that for small pumps running at temperatures sufficiently far from that corresponding to the VP, it will suffice to determine the minimum flow Q
min, m
3/h by:
(P, kW)*3600(s/h)
/[(density, kg/m
3)(c, kJ/kgK)(20
oC)]
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