Curve Corrections for Different Fluids

In practice this will however become not applicable for fluids of kinematic viscosities above 20mm²/s ( 20 cst ) due to the influence of a higher Reynolds Number with increasing viscosity. Empirical conversion methods have been developed for curve corrections for medium- and high-viscous fluids, which in practical application in older versions meant the time-consuming evaluation of diagrams, but in the current versions were prepared by corresponding formula sets. The most widespread method worldwide is the method from the Hydraulic Institute (USA), which has been standardised as ANSI/HI 9.6.7 and ISO/TR 17766. In practice, the conversion is usually carried out by computer programmes such as the Spaix PumpSelector. The computer implementation of this method enables the conversion of performance curves, whereby the user only has to define the desired delivery data and the pumped medium. The best efficiency point of the pump is of vital importance with all the known curve correction methods. The following conditions can be stated for the validity of this method:
  • Centrifugal pumps with closed or semi-open impellers
  • Kinematic viscosity in the range between 1 and 3000 mm²/s
  • Flow rate at best efficiency point between 3 and 410 m³/h
  • Head per stage between 6 and 130 m
  • Fluid displacement by means of a centrifugal pump under normal operating conditions
  • Handling of Newtonian Fluids

Centrifugal Pump

A centrifugal pump is a hydraulic flow machine in which the transport of the pumped medium is realized by utilizing the centrifugal forces (centrifugal forces) caused by the rotation of the impeller. Energy is transferred by deflecting the flow within the impeller blades. Centrifugal pumps are typically applied for pulse free, continuous or intermittent operation, but they are not suitable for dosing or metering applications. The strengths of this process are in the continuous, pulsation-free operation. Another advantage is the relatively simple design and good adaptability, which avoids high maintenance costs. The application is limited with regard to the viscosity of the pumped medium. With increasing fluid viscosity the efficiency is decreasing. Therefore the application is practically limited to fluids with a kinematic viscosity up to 100 .. 150 mm²/s. For higher viscosities positive displacement pumps are preferred. Important parameters are head, flow rate, power requirement, efficiency and NPSH value. The parameters are generally shown as performance curves depending on the volume flow (flow rate).

Viscosity

Newtonian fluids, at laminar flow, create shear tension and pressure super-imposed normal tensions which are proportional to the deformation velocity, the proportionality factor being the absolute viscosity. The kinematic viscosity is defined as: The viscosity depends on temperature and pressure, whereby pressure dependency of fluids is of negligibly small characteristics. Viscosity of non-Newtonian fluids can moreover be time-related (thixotropic or rheopexic flow characteristics); its characteristics then becoming undefined. The viscosity of a medium has an influence on both the system curve and the pump performance curve. For centrifugal pumps, the pump curves are converted in practice at a kinematic viscosity of more than 10 mm²/s.

Non-Newtonian Fluids

This is thus indicated that there is no line coherence between deformation and shear tensors and that the viscosity rate is time-related. Non-Newtonian flow characteristics can be observed with the following fluids:
  • gaseous soot in oil varnish
  • cereal corn suspensions in water
  • waste water sludgesewage
  • toothpaste
  • mortar
  • soap solutions
Examples: Thixotropic characteristics can be observed on numerous kinds of varnishes and lacquers, that means the viscosity is time-related. On stirring with constant angular velocity a rather great resistance is being experienced at first, whilst after a time the viscosity becomes noticeable less, tending towards its lower limits. Plastic and pseudoplastic characteristics can be observed on many industrial sludge’s e.g. suspensions of lime (mortar) and chalk (toothpaste). Below the shear rate (flow limit)they behave like solid bodies and above as fluids. Colloidal fluids, such as caoutchouc or solution of soap in water, behave like thixotropic fluids but will not recover their original viscosity when agitation is stopped. The viscosity of such fluids decreases as agitation or shear rate is increased. The reverse (dilettante) characteristic scan be observed on some high-concentrated suspensions., their viscosity increases with increasing agitation or shear velocity rate. Both the pump curves and the classical methods for calculation of the pipe friction loss assume a constant viscosity and are not valid for non-Newtonian fluids. Depending on the flow behaviour of the pumped medium, they can at best be used as an approximation. For many non-Newtonian media, there are therefore special calculation or approximation methods for sizing and selection.

Task of Pumps

In a narrower sense, in contrast to blowers and compressors for gases and compressible media, pumps for incompressible media are referred to as liquid pumps. This means that the volume of the fluid remains approximately constant as the pressure increases. In practice, this also includes liquid mixtures with a low solid or gas content. In the case of liquid transport, the pressure of the pump is required to overcome the flow resistance that arises in the pipe system, e.g. for the circulation in a heating system. In addition, in cases of different liquid levels, overcoming the difference in height (Hgeo) is required, e.g. fluid displacement to a higher level ie. to fill and maintain a near constant level in an overhead tank.