Hydrocyclone Physics

Researchers cannot measure or fully explain the complex interaction between fluid and particles in a vortex


                                                                                      A functional overview:  The principal of operation of a hydrocyclone is based on the concept of the terminal settling velocity of a solid particle in a centrifugal field. The rock slurry feed enters tangentially into the cylindrical section and follows a circular path with a net inward flow of fluid from the outside to the vortex finder on the axis. The high circulating field is usually high enough to create an air core on the axis that extends from the spigot opening at the bottom of the conical section through the vortex finder to the overflow at the top. The centrifigal force field is many times larger than the gravitational field.
TParticles that experience this centrifugal field will tend to move outwards relative to the carrier fluid because of a greater relative density. The larger heavier particles migrate rapidly to the outside walls and will then be forced to move downward on the inside of the conical wall. Small, light particles will be dragged inwards by the fluid as it moves toward the vortex finder. It is this drag force that creates much of the complexity of particle behavior and is a function of the hydrodynamic conditions inside and the shape and size of the particle.
  

cyclone

The classification action of the hydrocyclone is determined by the net effect of the two competing forces that act on each particle - the outward centrifugal force and inward drag force. A particle that experience equilibrium between these two forces will have an equal chance of exiting the overflow or underflow.  This size particle tends to orbit and get moved towards either exit by random collisions with other particles and random eddy motion of the highly turbulent flow field.

Condition that define the equilibrium orbit:
Drag force = Centrifigal force
.5 Cd(Vr - Ur)^2 pA = Vo^2/r *Vp(ps-pf)    Cd=drag coefficient, Vr=radial velocity of fluid, Ur=radial velocity of particle, p=fluid density
A=particle cross sectional area, Vo=tangential component of particle velocity vector, r=radius of tangent motion, Vp=particle volume, ps=density of the particle.


This theoretical model of particle behavior when solved for particle size would be impossible to use in an online computer model of the particle leaving the overflow. However, the description indicates which external grinding circuit parameters would be useful as secondary measurements to infer particle size =  = = = = slurry flow




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