Gravitational Condensation of Atmospheric Water Vapor
Fran De Aquino
Professor Emeritus of Physics, Maranhao State University, UEMA.
Titular Researcher (R) of National Institute for Space Research, INPE
Copyright © 2015 by Fran De Aquino. All Rights Reserved.
Devices that collect water from the atmospheric air using condensation are well-known. They operate in a
manner very similar to that of a dehumidifier: air is passed through a cooled coil, making water to condense. This
is the most common technology in use. Here, we present a device that can collect a large amount of water (more
than 1m3/s) from the atmospheric air using gravitational condensation. Another novelty of this device is that it
consumes little electricity. In addition, the new technology of this device leads to a new concept of pump, the
Gravitational Pump, which can be used to pump water at very low cost from aquifers, rivers, lakes, etc., and also
to supply the high pressure (100atm or more) needed to push seawater through the semipermeable membrane, in
the desalinization process known as reverse osmosis.
Key words: Gravitational Condensation, Atmospheric Water, Reverse Osmosis, Gravity, Water Crisis.
1. Introduction
The percentage of water vapor in the
atmospheric air varies from 0.01% at -42 °C
[1] to 4.24% at 30 °C [2]. Water vapor is only
water in the form of invisible gas. The
atmospheric air contains 0.001% of the
planet’s water, which has a total volume of
1.338×1018m3 [3]. Thus, the Earth’s
atmosphere contains a volume of about
1013m3 of water, which is kept constant by
cycle evaporation /condensation. On the other
hand, the world’s population consumes
currently 9,087 billion cubic meters of water
per year (~1013m3) [4], which is
approximately, the same value maintained
constant in the atmospheric air.
Devices that collect water from the
atmospheric air using condensation are wellknown. They operate in a manner very similar
to that of a dehumidifier: air is passed through
a cooled coil, making water to condense.
A vapor is gas at a temperature lower
than its critical point [5], which means that
the vapor can be condensed to a liquid by
increasing its pressure without reducing the
temperature. The water, for example, has a
critical temperature of 374 °C, which is the
highest temperature at which liquid water can
exist. Therefore, in the atmosphere at ordinary
temperatures, water vapor will condense to
liquid if its pressure is sufficiently increased.
Here we show how a large amount of
atmospheric water vapor (more than 1m3/s)
can be condensed to liquid by means of
gravitational compression produced in a
compression chamber, where gravity is strongly
increased by using gravity control technology
(BR Patent Number: PI0805046-5, July 31,
2008 [6]) based on the discovery of
correlation between gravitational mass and
inertial mass [7]. Also we present a
Gravitational Pump, which works based on
the same principles, and can be used to pump
water at very low cost from aquifers, rivers,
lakes, etc., and also to supply the high
pressure (100atm or more) needed to push
seawater
through
the
semipermeable
membrane, in the desalinization process
known as reverse osmosis.
2. Theory
The gravitational mass mg and inertial
mass mi are not equivalents, but correlated by
means of a factor χ , i.e.,
m g = χ mi0
(1)
where mi 0 is the rest inertial mass of the
particle.
The expression of χ can be put in the
following form [7]:
⎧
2
⎤⎫
⎡
⎞
⎛ B2
mg ⎪
⎪
⎢
⎟
⎜
χ=
n −1⎥⎥⎬
⎨1 − 2⎢ 1 + ⎜
2 r⎟
mi0 ⎪
⎝μ ρ c ⎠
⎥⎦⎪⎭
⎢⎣
⎩
where n r is its index of refraction; B
(2)
is the
intensity of the magnetic field (T ) ; ρ is the
2
light; μ is the magnetic permeability of the mean.
It was shown that there is an additional
effect - Gravitational Shielding effect - produced
by a substance whose gravitational mass was
reduced or made negative [8]. It was shown that,
if the weight of a particle in a side of a lamina is
matter density of the particle; c is the speed of
r
r r
P = m g g ( g perpendicular to the lamina) then
r
r
of the lamina is P ′ = χm g g , where χ = m g mi 0
the weight of the same particle, in the other side
( m g and mi 0 are respectively, the gravitational
mass and the inertial mass of the lamina). Only
when χ = 1 , the weight is equal in both sides of
the lamina. The lamina works as a Gravitational
Shielding. This is the
Gravitational Shielding
effect. Since P′ = χP = χmg g = mg (χg) , we can
( )
consider that m ′g = χm g or that g ′ = χg .
Valve
Liquid Water
373.946°C and 217.7atm
Water drops
Compressed Air
Repulsive
gravity
χg
Air
ρ
Gravitational Shielding
Air
χ
B
g
Coil
Fig. 1 – Gravitational Condenser. Condensation of
the atmospheric water vapor by means of
gravitational compression. (Developed starting
from a process patented in July, 31 2008,
PI0805046-5 [6]).
Now consider the system shown in Fig.1.
At the base of the compression chamber there is a
gravitational shielding. In this case, this device is
basically a hollow cylinder, where a magnetic
field B passes through its air core. The air density
inside the cylinder was reduced down to
ρ = 8.017 ×10 −14 kg.m −3 * , in order to produce a
strong value (negative) of χ , using a practicable
value of B . Thus, according to Eq. (2), the value
of χ inside the air core is given by
χ = ⎧⎨1 − 2⎡ 1 + 12176.20B4 − 1⎤⎫⎬
⎩
⎢⎣
⎥⎦⎭
(3)
Consequently, for B = 1.0T , we obtain
(4)
χ ≅ −217.7
This means that the air inside the compression
chamber can be subjected up to a pressure
217.7 times greater than the atmospheric pressure
at the Earth’s surface, i.e., 217.7atm.
The pressure required to liquefy (to
condense) water vapor at its critical temperature
(373.946°C, 647.096K) is 217.7atm [9]. When
this occurs in the Gravitational Condenser, water
drops are driven to the top of the chamber (See
Fig.1), because they are subjected to repulsive
gravity † χg . Thus, this “reverse rain” fills with
water the top of the compression chamber. Then,
the regulator valve (placed at the top of the
chamber) opens, releasing the water to be stored
and distributed. After the exit of the water, occurs
the exit of the dehumidified air, which was inside
the compression chamber. When the pressure
inside the chamber becomes equal to the
atmospheric pressure, the regulator valve is
closed, and a new cycle of compression begins, in
order to produce more water.
If the atmospheric air inside the
Gravitational Condenser is at temperature of
30 °C, then the percentage of water vapor
contained it is 4.24% [2]. Assuming that the
Gravitational Condenser can withdraw of the air
just 30% of this value, then the total volume of
water withdrawal from the atmospheric air inside
the chamber will be 1.27%(ρ wvapor ρ water ) of the
volume of atmospheric air compressed inside the
compression chamber. Since the state equation,
gives ρ wvapor = 2.2 ×10−3 ( pwvapor T ) [10], then for
pwvapor ≅ 217.7atm= 2.2 ×107 N / m2 and T = 647.096 K ,
we get ρ wvapor ≅ 74.8kg .m −3 . Thus, if the volume
of the compression chamber of the Gravitational
Condenser is 1,000 m3 , (10m×10m ×10m) and the
volume of the compressed air inside the chamber
*
This density is equivalent to Earth’s atmospheric
density at about 600km height.
†
In respect to Earth’s gravity which is attractive.
3
is 217.7×(the volume of the chamber)=217,700
m3, then the total volume of water withdrawal
from the atmospheric air will be given by
(1.27% 100)(ρ wvapor ρ water ) × 217,700 ≅ 207m3 of water.
Assuming that the time interval required to
condense this volume of water is approximately
60s, then just one Gravitational Condenser with
the mentioned characteristics can supply about 3.5
m3/s of water. This means that a set of 10 or 15
Gravitational Condenser of this type can supply
sufficient water for the total consumption of a
large city as New York or S. Paulo.
etc., and also to supply the high pressure (100 atm
or more (See Eq. (4)) needed to push seawater
through the semipermeable membrane, in the
desalinization process known as Reverse
Osmosis ‡ (See Fig.3). Thus, these devices can
strongly contribute to solve the current water
crisis.
semipermeable
membrane
desalinated
water
χg
Liquid
Gravitational
Shielding
χg
Gravitational Shielding
g
Gravitational Pump
Seawater
χ
B
salt solution
100 atm
(or more)
Repulsive
gravity
ρ
concentrated
Fig. 3 – Reverse Osmosis using a Gravitational
Pump.
Coil
Liquid
g
Fig. 2 – Gravitational Pump – Liquids (Water, Oil,
etc) can be propelled by using the gravitational
pump shown above (a process patented in July, 31
2008, PI0805046-5 [6]).
‡
Figure 2 shows a Gravitational Pump
based on the same principles described in Fig.1. A
Gravitational Shielding placed at the bottom of
the pump, reverses and intensifies the gravity in
the region above the gravitational shielding (it
becomes equal to χg ). Thus, any liquid can be
propelled through this type of pump (See Fig.2).
Obviously, the operational costs of the
Gravitational Condenser and of the Gravitational
Pump are very low. In addition, the Gravitational
Condenser can be constructed at the own cities,
where the water will be consumed.
The Gravitational Pump, in turn, can pump
water at very low cost from aquifers, rivers, lakes,
Reverse Osmosis is the process of forcing a solvent
from a region of high solute concentration through a
semipermeable membrane to a region of low solute
concentration by applying a pressure in excess of the
osmotic pressure. The most important application of
reverse osmosis is the separation of pure water from
seawater and brackish waters. However, the
conventional process of reverse osmosis has a great
obstacle: it requires high amount of electricity to
produce the high pressure (60 to 80atm), needed to
push seawater through the semipermeable membrane
[11,12]. This process is best known for its use in
desalination (removing the salt and other minerals from
sea water to get fresh water), but since the early 1970s,
it has also been used to purify fresh water for medical,
industrial, and domestic applications.
4
References
[1] Michael B. McElroy "The Atmospheric Environment"
2002 Princeton University Press p. 34 figure 4.3a
[2] Michael B. McElroy "The Atmospheric Environment"
2002 Princeton University Press p. 36 example 4.1
[3] Gleick, P.H., ed. (1993). Water in Crisis: A Guide to the
World's Freshwater Resources. Oxford University Press.
p. 13, Table 2.1 "Water reserves on the earth".
[4] Hoekstra, A. Y and Mekonnen, M.M. (2012) PNAS 109
(9) 3232-3237; published ahead of print February 13,
2012, doi:10.1073/pnas.1109936109.
[5] R. H. Petrucci, W. S. Harwood, and F. G. Herring,
General Chemistry, Prentice-Hall, 8th ed. 2002, p. 483–
86.
[6] De Aquino, F. (2008) Process and Device for Controlling
the Locally the Gravitational Mass and the Gravity
Acceleration, BR Patent Number: PI0805046-5,
July 31, 2008.
[7] De Aquino, F. (2010) Mathematical Foundations
of the Relativistic Theory of Quantum Gravity,
Pacific Journal of Science and Technology, 11 (1),
pp. 173-232.
[8] De Aquino, F. (2011) Ultrafast Conversion of Graphite
to Diamond in Gravitational Pressure Apparatus,
http://vixra.org/abs/1208.0007, p. 4.
[9] International Association for the Properties of Water and
Steam, 2007, available at: http://www.iapws.org ;
http://www.chem.purdue.edu/gchelp/liquids/critical.html
[10] http://www.engineeringtoolbox.com/density-air-d_680.html
[11] Shannon, M. A. et al., (2008) Nature 452, 301-310.
[12] Humplik, T. et al., (2011) Nanotechnology, 22, 292001.