For
analysis of the accelerator models efficiency, in the absence of any
flow contraints, several graphs were plotted:
-
Characteristic
of the ratio Vt/Vc between flow velocity Vt in the
channel
narrowerzone and
the stream velocity Vc, as a function of the stream velocity Vc.
-
Characteristic
of the introduced net head +DH
by using such a stream accelerator, as a function of the stream velocity
Vc,
calculated on free conditions by +DH
= (Vt2/2g) - (Vc2/2g).
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The
ratio Vt/Vc is in the absence of any flow constraints, almost
steady for typical stream velocities. The following table states
characteristic values of the ratio Vt/Vc in the absence of any flow
constraints, for the several accelerator models tested.
Model |
A1 |
A2 |
B1 |
C1 |
B2 |
C2 |
B3 |
B4 |
Vt/Vc
% |
140
% |
130
% |
110
% |
105
% |
115
% |
115
% |
120
%
|
115
% |
Comparing
the models efficiency values, we may conclude that:
-
The
divergent zone should not be too short nor too long having an optimum
length to guarantee an auxiliary rotation between inside and outside
stream vortexes.
-
The
channel narrower zone should not be too short, avoiding that
turbulences at diverging zone affect turbine to work, nor too long
that depression at outlet compensates concentration at the inlet.
-
Funneling
of the inlet concentration zone should be adequate to have all
incoming flow through the channel narrower zone.
-
The
conduit external surface should be slightly inclined and not offering
obstacles to the outside stream in order to facilitate creation of
depression nearby the outlet section.
-
The
accelerator model to be used on a industrial scale should have an
optimized shape, being similar to Model A1 that is the more efficient model
among all tested stream accelerator models. For this model, the flow
velocity Vt through the channel narrower zone is in the absence
of any flow constraints about 40% higher than the velocity Vc
of the outside free stream, meaning that the flow loading in the
channel narrower zone is about 2 times higher than the outside stream
loading and the power density about 2,75 times higher than the power
density of the outside stream. This corresponds to the introduction of a
net head +DH
of about 200 mm for a stream velocity Vc of 2 m/s (4 knots),
of about 300 mm for a stream velocity Vc of 2,5 m/s (5 knots)
and of
of about 400 mm for a stream velocity Vc of 3 m/s (6 knots).
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