New Energy Technologies Magazine nr 3 2005.pdf - Index of

weight of the left ones by the weight of the
water filling the useful capacities, an
additional force will influence the right side
of the belt and create a rotary moment of the
systems:
Z=mgNR (1),
where m is the mass of the water in the useful
capacity; g is the acceleration of free fall; N
is the number of the cylinders filled with
water in the vertical sector of the belt; R is
the wheel's radius.
Thus, the belt will rotate clockwise. When the
cylinder filled with water will pass the lowest
point and occupy a vertical position, the
piston will press the water out of the cylinder
under the influence of gravity force. At the
same time, in the upper cylinder, which is
connected with it, the piston will go down
under the influence of the weight and draw
the water from the lower cylinder into its
useful capacity. Both weights will operate in
the same direction under the influence of
gravity force overcoming a pressure of a
liquid spout with height H (where h is an
upright distance from the bottom of the left
lower cylinder to the bottom of the right
upper one). A condition of the water raise will
be determined by the excess of the sum of
pressures created by two weights over a
pressure created by water spout H:
2Mg/s ρgH (2),
where M is the mass of the weight; s is the
sectional area of the cylinder's useful
capacity; ρ is the specific density of the liquid.
it follows that an optimal height of water
rises:
H = 2M/sρ (3).
Due to the fact that, if the lower cylinder is
located vertically, the water from it raises up
to height H in the upper cylinder, which is
connected with it, the system increases its
potential energy by a value of
E 0
= mgH (4)
under the influence of gravity force inside the
cylinders. The water mass corresponds with
the cylinder's useful capacity:
m = ρsL (5),
where L is a length of the useful capacity.
Using (4) and taking into account (3) and (5),
the potential energy increase can be
expressed as
E 0
= 2MgL (6),
which is equivalent to the work produced
during motion of the weights under the
influence of gravity force in both cylinders.
Thus, the described system is a gravity
engine of perpetual mobile type able to
produce yield using only gravity force.
Thus, the gravity engine's power will be
determined by a quantity of the cylinders
passing through a permanent point of the
system (n) per second and efficiency (η)
taking into account friction losses:
W=nE 0
η (7)
Under permanent speed of the belt's motion
(V):
n=V/(L+d) (8),
where d is the interval between adjoining
capacities of the cylinders. Putting (7) into
expressions (6) and (8), we obtain an
expression of the power as:
W=2MgVηL/(L+d) (9)
It can be seen that a maximal power can be
obtained by a possible increase of the belt's
motion and placing the cylinders on the belt
with minimal allowable intervals.
However, it is early to talk about efficiency
and future possibilities of the gravity engine
without making an experimental test.
The author would be thankful for critics and
discussion the model proposed.
24 New Energy Technologies #3(22) 2005