[0001] The present application relates to a method and an apparatus for transporting fluid
in a conduit, for example a pipe, as disclosed respectively in the preamble of independent
claims 1 and 6.
[0002] Pump technology has evolved very little since Archimedes' time. Indeed, all known
pumps are based on the same main principle and, put simply, they work by either pushing
or pulling (i.e. sucking) the fluid. The previously known pumps thus generate a static
pressure which, when the fluid is pushed, diminishes downstream in the pumping direction
and, if the transport distance is sufficiently long, will ultimately reach zero at
one point, which means that the fluid cannot be transported past this point without,
for example, another pump being connected before this point is reached.
[0003] In about 1594, Galileo Galilei invented a pump which basically can be termed a syringe.
In this connection, he noticed that it was impossible to draw water up from a depth
of more than about 10 metres. Galileo could not explain the reason for this limitation,
but this phenomenon has since been explained and in hydraulic engineering today it
is acknowledged that the theoretical 10-metre boundary line cannot be crossed. In
practice, due to various effects (for example, friction), the suction lift limit is
less than about seven metres.
[0004] The previously known pumps therefore have clear limitations. The suction lift limit
means that in the case of vertical transport of a fluid over large distances towards
the surface, for example, in the offshore industry, a pump must be installed on the
bottom and additional pumps must be installed in series in the direction of transport.
This makes installation and maintenance difficult, and since the entire weight of
the fluid column is lifted during pumping, an enormous amount of energy is required
to pump the fluid when the transport distances involved are long. The drawbacks of
the previously known pumps are therefore the aforementioned suction lift limit, low
efficiency and high energy consumption.
[0005] To avoid the aforementioned drawbacks of the prior art, there is according to the
invention provided a method and an apparatus as disclosed respectively in the characterising
clause of claims 1 and 6.
[0006] Advantageous embodiments of the invention are set forth in the dependent claims.
[0007] Unlike previously known pumps, the fluid is not pushed or sucked in the conventional
manner when using the apparatus or method according to the invention. Instead, in
a preferred embodiment, mechanical impulses or pressure waves are introduced into
the fluid in a pipe. In a sense, the apparatus, or the pump, acts as a hammer, generating
acoustic waves (or pressure waves) in the system. The waves travel through the fluid
in the pipe at the speed of sound and with very little dissipation.
[0008] Acoustic waves are large pressure oscillations, and when a wave encounters a valve,
the valve remains closed while the pressure difference across the valve is positive
(i.e. pressure above atmospheric), and opens when the pressure difference becomes
negative (i.e., pressure below atmospheric) in response to the wave being reflected
by the valve, thus creating a flow through the valve in the direction of the negative
pressure in order to equalise the pressure across the valve. The valve generates the
suction effect, and energy is supplied to the valve through the fluid. In other words,
the fluid carries potential energy in the form of acoustic waves, and a main function
of the valve is to transform this energy into kinetic energy, after which the fluid
volume that has flowed through the valve in response to the wave's activation thereof
is transported in the form of a compression wave which travels through the fluid.
The fluid transport, or pumping, thus takes place according to the invention in that
each small or incremental fluid volume that flows through the valve is transported
downstream through the rest of the fluid in the form of a pressure wave of increased
volume density.
[0009] With the apparatus and method according to the invention there is probably no suction
lift limit. A successful test with a vertical suction height of 24 metres (which is
more than three times the previously known conventional, practical suction lift limit)
has been conducted, the suction height being chosen on the basis of the maximum vertical
pipe length the test facility allowed. The experiment shows that the invention is
a major breakthrough in the domain of fluid transport, and the new technology according
to the invention will be even more efficient when the pipe is placed in water, due
to the hydrostatic balance between the inside and the outside of the pipe. Such conditions
are usual in oil extraction where deep sea pumping is required.
[0010] The parts of the apparatus, or the pump, according to the invention which constitute
the wave generator may advantageously be positioned on top of a fluid source, for
example, an oil well, and thus positioned will contribute to a dramatic reduction
in installation and maintenance costs in addition to a substantial reduction in energy
consumption.
[0011] Only the part of the device which constitutes the fluid dividing means, preferably
a check valve, will be arranged at the fluid transport starting point, which often
means at the bottom of the fluid source. A check valve of this kind will be relatively
easy to put in place, and does not require any external energy supply apart from the
energy supplied through the fluid in the form of waves. The wave generator will thus
be the part of the apparatus that requires external energy supply via power cables,
hydraulic lines, mechanical transmissions or the like.
[0012] During time-consuming maintenance and repair work, the wave generator can be temporarily
replaced by a new one, thereby allowing continuous operation. The apparatus and the
method according to the invention will thus result in reduced total costs, which will
always be a major objective in oil production.
[0013] The apparatus, or the pump, according to the invention is highly efficient, and its
efficiency has been measured to be up to 95%. The transport material may be liquids,
gases, multiphase fluids or highly viscous fluids. Successful tests have also been
conducted with a non-Newtonian fluid.
[0014] With the apparatus and method according to the invention, it is anticipated that
it will be possible to extract oil from oil fields which cannot be extracted today
using conventional pumps due to high costs or quite simply because it is technically
impossible.
[0015] The method and apparatus according to the invention will be described in more detail
below on the basis of advantageous, non-limiting exemplary embodiments, and with reference
to the accompanying drawings and appended claims, wherein:
Figure 1 is a simplified diagram of a first embodiment of the apparatus according
to the invention used for vertical transport of a fluid from a lower to an upper fluid
reservoir;
Figure 2 is a simplified diagram of a second embodiment of the apparatus according
to the invention, and includes an enlarged detailed view of a part of the apparatus;
Figure 3 is a sectional view of the apparatus shown in Figure 1 along the line B -
B;
Figure 4 is a graph of the oscillatory motion of the apparatus shown in Figures 1,
2 and 3;
Figure 5 is a graph of pressure measurements made during a test of the apparatus according
to the invention; and
Figure 6 is a graph of pressure measurements made during another test of an apparatus
according to the invention.
[0016] In the description and the claims, the terms "upstream" and "downstream" are related
to the direction of fluid transport or pumping direction, as should be implicitly
apparent.
[0017] Figure 1 shows a first embodiment of the apparatus according to the invention, where
fluid is transported from a lower 1 to an upper 2 fluid reservoir through a pipe 3,
and comprising a wave generator 4 and a fluid dividing means in the form of a check
valve 5 located at a lower end of the pipe 3 submerged in the reservoir 1. Another
check valve 6 is shown located downstream of the wave generator 4. This check valve
6 may have a stabiliser function, serve as a regulator of several parameters depending
on the structure of the fluid transport system, or alternatively be omitted. In the
figure, the direction of fluid transport is indicated by solid arrows, whilst the
direction of travel of a wave generated by the wave generator 4 is indicated by a
stippled arrow. The check valves 5, 6 are basically constructed in that spring-loaded
balls lie sealingly against respective valve seats, as will readily be apparent to
a person of skill in the art. When a wave from the wave generator hits the one-way
valve 5 and is reflected upwards (concurrently), the check valve will open in order
to then be closed again because of the pressure difference that occurs across the
valve as a result of the wave, as explained above. An incremental fluid volume ΔV
will then flow concurrently through the valve 5, and travel in the form of a pressure
wave through the fluid in the pipe 3 on the downstream side of the valve 5 to the
upper fluid reservoir 2.
[0018] With regard to the initial conditions for the fluid transport system comprising the
apparatus according to the invention, there may initially be air on the whole or part
of the downstream side of the check valve 5 and liquid on the upstream side of the
check valve. A wave formed by the wave generator 4 will travel first through the air
and then through the liquid on the downstream side of the check valve 5 before the
valve is activated by the wave to admit an incremental liquid volume ΔV. Thus, for
each generated wave, the pipe 3 will be successively filled with liquid, and after
sufficiently many generated waves liquid will flow out of the pipe 3 and to the upper
fluid reservoir 2. Therefore, the wave generator 4 does not initially need to generate
a wave directly in liquid in order to cause liquid to be transported from the lower
1 to the upper 2 fluid reservoir, as the wave can be transmitted between different
fluids in gas and liquid state.
[0019] The wave generator 4 consists of the following main components: a membrane 7, an
oscillator 8 and a vibrator or power source 9. The basic mode of operation of the
wave generator 4 will be explained in more detail below with reference to Figures
2 and 3, which show a second embodiment of the invention in which the wave generator
and fluid dividing means - unlike in the first embodiment shown in Figure 1 - constitute
an integral unit in that a plurality of check valves 5 are arranged in a piston 7'.
[0020] In Figure 2, the power supplying motion of the power source 9 is indicated by a double
arrow, whilst the direction of fluid transport through the pipe 3 is indicated by
regular arrows. The oscillator 8 includes an oscillating weight 10 disposed between
a first end of two coil springs I 1 and 12, and connected to the piston 7' via a shaft
13. A second end of the coil spring 12 is rigidly supported, and a second end of the
coil spring 11 is connected to the vibrator or power source 9 which via the coil spring
11 and at a given frequency imparts to the oscillating weight 10 a translational oscillating
motion of an amplitude of A about a neutral point N. Thus, the oscillating weight
10 will, together with the coil springs 11 and 12, form a part of an oscillating system
having a given resonant frequency, and the motion of the oscillating weight 10 will
be transmitted to the piston 7' via the shaft 13.
[0021] The oscillating weight 10 and the piston 7' will thus oscillate at an amplitude A
at a given frequency, and it will be apparent to those skilled in the art that a small
amplitude, for example in the range of 5 mm, and high frequency, for example in the
range of 100 Hz, will cause a high acceleration which in turn will cause the fluid
on the downstream side of the piston 7' to be supplied with a high power impulse from
the piston 7'. Furthermore, the potential energy and kinetic energy of the oscillating
system, minus the energy losses in the system, will always be constant, the losses
here consisting mainly of the power impulse supplied to the fluid via the piston 7'.
[0022] The enlarged detailed view in Figure 2 shows the structure of the check valves 5
more clearly. Each valve is arranged as a through opening in the piston 7' perpendicular
to the piston 7' surface 14. A membrane 15 with a central orifice 16 is provided in
the through opening. A central abutment element 17 for the membrane 15 is also provided,
so that a part of the membrane 15 will be moved into sealing contact with the abutment
element by the positive pressure formed on the downstream side of the valve 5 when
the piston moves in the downstream direction. Fluid flow through the valve 5 will
thus be prevented. Conversely, when the piston 7' moves in the upstream direction,
it will be apparent to those skilled in the art that fluid flow through the valve
5 can take place unimpeded. When the piston 7' moves in the upstream direction, an
incremental fluid volume ΔV will thus flow through the open valves 5 in the piston
7' to the downstream side. When the piston then changes direction of travel, the valves
5 will close and the incremental fluid volume ΔV is transported in the form of a pressure
wave formed by the motion of the piston 7' and which travels in the fluid on the downstream
side of the piston 7'. Because the valves 5 are open when the piston 7' moves counter-flow,
the motion resistance of the piston in this direction will be small, and it may therefore
be more descriptive to say that the incremental fluid volume ΔV is "captured" on the
downstream side of the piston during the counter-flow motion of the piston 7' than
that the incremental fluid volume ΔV flows through the valve, as the pressure difference
across the piston 7' will be small during the counter-flow motion of the piston 7'.
[0023] In Figure 4, the translational oscillating motion of the oscillating system or oscillator
8 is graphically presented in the form of a sine curve as a function of time, and
where the aforementioned losses consist of an amplitude decrement D between two successive
oscillations. The work required to create oscillations of the same amplitude is supplied
to the oscillator 8 from the power source 9.
[0024] As mentioned above, various tests of the apparatus and method according to the invention
have been conducted in which the theoretical suction lift limit for the conventional
pumps known to date has been exceeded.
[0025] Figure 5 shows a graph of pressure measurements as a function of time made at two
different points in a pipe during a suction lift test of one embodiment of the apparatus
according to the invention which is essentially identical to the embodiment shown
in Fig. 1, and where, as previously mentioned, a suction lift height of 24 metres
was obtained. From the figure it can be seen that, as expected, there is a phase displacement
between the pressure waves (represented by the peaks in the figure) by the apparatus
(i.e., at a reference height equal to zero metres) and the pressure waves 16 metres
upstream in the pipe from the said reference height (i.e., lower than the apparatus),
as the pressure waves moves through the fluid at a given wave velocity. More surprisingly,
it can be seen from the figure that the pressure waves are in fact also intensified
as the pressure 16 metres upstream in the pipe is considerably higher than at the
said reference height. From wave physics, it is generally known that waves travel
more easily in a denser or more compressed medium, and the explanation of the aforementioned
phenomenon is believed to reside in the fact that the static pressure, and thus also
the density, of a fluid generally increases with increasing depth in the fluid, and
that the wave is intensified because it travels though a medium having steadily increasing
pressure and density.
[0026] Figure 6 is a graph of pressure measurements made during a test of another, small-scale
embodiment of an apparatus according to the invention, essentially like the embodiment
shown in Figures 2 and 3, and where the pressure was measured at three different points.
The different points were immediately upstream of the apparatus (indicated by a circular
symbol), immediately downstream of the apparatus (indicated by a cruciform symbol)
and at a greater downstream distance from the apparatus (indicated by square symbol).
The figure shows respectively the mean pressure, the maximum pressure and the RMS
pressure as a function of frequency, and as can be seen from the figure, the mean
pressure, the maximum pressure and the RMS pressure all increase in the downstream
direction. Furthermore, the test readings indicate that in particular the maximum
pressure and the RMS pressure difference between the measuring points increases with
increasing frequency, which is believed to be due to wave superposition.
[0027] Instead of the piston 7' with valves 5 shown in Figures 2 and 3, a semi-permeable
membrane may alternatively be provided, where fluid can simply flow through the membrane
in the downstream direction, and instead of springs 11, 12, other types of energy
storing elements may alternatively be provided, for example, closed devices filled
with a compressible medium, magnets of the same polarity, resilient materials such
a rubber or the like, which have small losses due to inner frictional resistance.
Similarly, the power source 9 need not be an electric vibrator as shown in Figure
1, but may be any form of motor or power-generating device which either directly or
indirectly produces a translational oscillating motion of a desired frequency and
amplitude. In addition, it will be apparent to those of skill in the art that the
check valves 5, 6 may be made in many different ways, and that the designs shown in
Figures 1-3 are therefore only two of many possible embodiments known
per se. Finally, although in the exemplary embodiments shown and described in connection
with Figures 1-3 a pipe 3 is used, the pipe 3 may be replaced by any conduit in which
at least one wave can travel and an incremental fluid ΔV volume can be transported.
Consequently, the method and the apparatus according to the invention are not limited
by the appended claims.
[0028] This application is a divisional application of European patent application no.
05 814 040.1 (the "parent application"), also published under no.
EP-A-1 859 167. The original claims of the parent application are repeated below in the present
specification and form part of the content of this divisional application as filed.
- 1. A method for transporting fluid in a conduit (3), for example, a pipe, comprising
a fluid dividing means (5) in the conduit which divides the conduit (3) into an upstream
side and a downstream side, and which fluid dividing means (5) in a first state prevents
fluid communication between the upstream side and the downstream side and in a second
state allows fluid communication between the upstream side and the downstream side,
characterised by the steps of:
- generating at least one wave in the fluid on the downstream side of the fluid dividing
means (5), which wave causes the fluid dividing means (5) to be brought into the second
state so that an incremental fluid volume ΔV from the upstream side of the fluid dividing
means (5) can flow to the downstream side of the fluid dividing means (5); and
- causing a change in pressure on the downstream side of the fluid dividing means (5)
when the fluid dividing means (5) is brought back to the first state,
whereby the incremental fluid volume ΔV is transported in the form of a pressure wave
which travels in the fluid on the downstream side of the fluid dividing means (5).
- 2. A method according to claim 1, characterised in that the step of generating the at least one wave in the fluid on the downstream side
comprises moving the fluid dividing means (5) in the fluid.
- 3. A method according to claim 1, characterised in that the step of generating the at least one wave comprises generating the wave at a distance
downstream from the fluid dividing means (5).
- 4. A method according to claim 1, characterised in that the step of generating the at least one wave comprises generating a pressure wave.
- 5. A method according to any one of the preceding claims, characterised in that the step of generating the at least one wave in the fluid on the downstream side
of the fluid dividing means (5) comprises generating a plurality of waves using an
oscillator (8) and a power source (9).
- 6. An apparatus for transporting fluid in a conduit (3), for example a pipe, comprising
a fluid dividing means (5) in the conduit (3) which divides the conduit (3) into an
upstream side and a downstream side, and which fluid dividing means (5) in a first
state prevents fluid communication between the upstream side and the downstream side
and in a second state allows fluid communication between the upstream side and the
downstream side, characterised in that
a wave generator (4) is provided for generating at least one wave in the fluid on
the downstream side of the fluid dividing means (5), which wave causes the fluid dividing
means (5) to be brought into the second state so that an incremental fluid volume
ΔV from the upstream side of the fluid dividing means (5) can flow to the downstream
side of the fluid dividing means (5) and cause a change in pressure on the downstream
side of the fluid dividing means (5) when the fluid dividing means (5) is brought
back to its first state;
whereby the incremental fluid volume ΔV is transported in the form of a pressure wave
which travels in the fluid on the downstream side of the fluid dividing means (5).
- 7. An apparatus according to claim 6, characterised in that the wave generator (4) comprises an oscillator (8) and a power source (9) for generating
a plurality of waves.
- 8. An apparatus according to claim 6 or 7, characterised in that the fluid dividing means (5) is a check valve.
- 9. An apparatus according to claim 6 or 7, characterised in that the fluid dividing means (5) is a semi-permeable membrane.
- 10. An apparatus according to claim 8, characterised in that a plurality of check valves (5) are arranged in a piston (7') or a membrane (7).
- 11. An apparatus according to one or more of claims 6 to 10, characterised in that the wave generator (4) and the fluid dividing means (5) constitute an integral unit.
- 12. An apparatus according to one or more of claims 6 to 10, characterised in that the wave generator (4) is located at a distance downstream of the fluid dividing
means (5).
- 13. An apparatus according to any one of claims 6 to 12, characterised in that a check valve (6) is provided downstream of the wave generator (4).
- 14. An apparatus according to any one of claims 6 to 13, characterised in that the at least one wave generated by the wave generator (4) is a pressure wave.