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The Vortex Tube
Separator (VTSä) utilises two elementary physical concepts.
- The Joule Thomson
effect: This is simply the cooling of the gas by adiabatic
expansion across a restriction.
- The Hilsch effect:
This refers to the tangential introduction of a gas stream
through a nozzle creating a forced vortex which leads
to a simultaneous separation of the gas and liquid in
the gravitational field of the vortex and at the same
time causing a temperature gradient to form across the
vortex. (the temperature reduces from the wall to the
tube centre) Due to the temperature gradient the expansion
moves away from a Joule Thomson process (adiabatic expansion)
towards a more efficient isentropic expansion.
The gas is introduced into the Vortex Tube
Separator through a header across tangential inlet nozzles.
In most caese, depending upon the ratio of the inlet to
outlet pressures, the gas will reach near sonic velocity
as it passes into the vortex tube.
Due to the Hilsch effect both a warm
and a cold gas fraction are created. During the near adiabatic
expansion of the gas across the inlet nozzle, condensation
of the gas components occur. The condensate is thrown to
the outer wall of the Vortex Tube Separator and the liquid
passes through drain holes at the bottom of the VTS to a
separator.
Simultaneously, gas moves from
the wall to the centre of the tube where it cools further.
By removing the liquid phase from the tube wall it is possible
to obtain two discrete gas and liquid phases. Special internals
at the opposite end to the inlet enable the cold and warm
gas streams to be separated. The cold gas is diverted back
by the throttle along the tube to the cold gas outlet.
The temperature gradient
and the cold gas stream temperature increase the liquid
separation.
Both the cold and warm
gas streams are thermodynamically superheated. Combing the
warm and cold gas is the normal mode of operation for the
Vortex Tube Separator (VTSä).
(see figure 2)
Dependent upon the gas compositions and process
conditions, a 15 - 20% weight additional condensate recovery
may be expected compared to a typical JT process.
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