This patent application is a U.S. National Phase Application under 35 U.S.C. §371 of International Application No. PCT/SG2009/000493, filed Dec. 23, 2009, entitled MICROFLUIDIC MIXING APPARATUS AND METHOD.
The invention relates to the mixing of different fluids within a microfluidic device. Further the invention relates to the manufacture of such device and its means of operation.
In many microfluidic systems for biological and chemical applications, there is often a need for a fast and complete mixing of various solutions in order to achieve the desired result. However, in micro geometry, the viscosity of the fluid may become significant and dominate the flow characteristics of the fluid resulting in a low Reynold's number and so laminar flow. As a result, mixing depends on diffusion rather than macro scale turbulent flow which is a slow molecular process. Microfluidic mixers are known, with the degree of interference between the mixing fluids sufficient when the fluids are of a similar viscosity. However, due to the limitations of prior art microfluidic mixing devices being able to adequately interfere with the fluids, there are generally inadequate where the respective viscosities of the fluids are substantially different.
It would therefore be advantageous to have a mixing device and method of operation of such a device that introduces greater interference between the fluids in order to better and more quickly achieve the desired degree of mixing.
The following statements provide more specific aspects of the present invention.
In a first aspect the invention provides a microfluidic mixing device for mixing at least two fluids to form a mixed fluid comprising a first mixing chamber for receiving the fluids from at least two fluid paths; a mixing zone upstream from the mixing chamber having a first and second fluid path; said first and second fluid paths overlapping at first and second discreet points so as to provide mutual fluid communication between the first and second paths at said discreet points.
In a second aspect the invention provides a method of mixing at least two fluids to form a mixed fluid comprising the steps of: providing a microfluidic mixing device having a start chamber and a mixing chamber with a mixing zone intermediate said chambers; introducing said fluids to the start chamber; flowing said fluids through a first and second fluid path extending from the start chamber to the mixing chamber, said first and second fluid paths overlapping at a first and second discreet points; bringing fluid in the first fluid path into contact with fluid in the second fluid path at said first discreet point; diametrically swapping the first and second fluid paths; bringing the fluid of the first fluid path into contact with the second fluid path at the second discreet point.
Accordingly by providing interaction between the fluid paths are different positions, the cross sectional flow of both fluid paths are interfered with at multiple points around the peripheral edge of said fluid paths and so leading to a greater interference of flow and so better mixing. Such increased interaction further increases the surface area of interference of the fluid paths and so leading to a better mixing process.
In one embodiment, the internal substrates may provide for microfluidic fluid flow in two levels, said levels being in fluid communication so as to divide and swap flow paths between said layers.
The present invention may provide for a microfluidic mixer for fluids with widely different viscosities. It contains an interconnected multi-channel network through which the bulk fluid volumes may be divided into smaller ones and chaotically reorganized. Then, the multiple fluid streams may be driven into an expansion chamber which triggers viscous flow instabilities.
In one embodiment, the mixing effect may be at least partially attributed to the expansion effect as the first and second path enter the mixing chamber. The sudden pressure loss associated with an expansion may modify the flow from substantially laminar with the first and/or second fluid path to substantially turbulent in the mixing chamber as a result of the expansion.
In one embodiment the chamber may be of a width equal to or grater than the sum of widths of channels of the first and second fluid path immediately upstream of the mixing chamber.
It will be convenient to further describe the present invention with respect to the accompanying drawings that illustrate possible arrangements of the invention. Other arrangements of the invention are possible and consequently, the particularity of the accompanying drawings is not to be understood as superseding the generality of the preceding description of the invention.
For fluids with a large viscosity differential, a stationary phase distribution should be established among the fluids before entering the chamber. Stable shear stress equilibrium exists near the fluid interface. But when the diverse fluid streams enter the mixing chamber, the equilibrium is broken down due to the sudden expansion of the geometry. The fluids must be reorganized to re-establish the equilibrium. The perturbations caused by this expansion instability will intensify the mass exchange between the different fluid species.
In the current embodiment
Considering the first mixing cycle, the mixing zone 20 includes two fluid paths 25, 30 which are arranged to divide the fluid within start chamber 10. The first fluid path 25 projects from the start chamber 10 centrally before entering a re-directed channel 50 so as to divert the flow out of a plane defined by the start chamber to a different parallel plane.
The second fluid path 30 is divided into two channels 44, 45 and project from the start chamber on either side of the first fluid path 25.
It will be noted that in the present embodiment, the size of one channel 45 is greater than that of the second channel 44 and so providing an asymmetrical flow characteristic between the channels 44, 45. As the magnitude of the velocity and direction of the fluid streams are different in the first fluid path and each of the channels 44, 45 of the second fluid path upon contacting, there will be strong shearing and stretching of the fluids such that the distribution pattern of the fluids will be altered through this increased interference of said flows. It will be appreciated that whilst this may have a beneficial effect, a differential channel width represents merely one embodiment, with an equal channel width also falling with the effective application of the present invention.
The first fluid path 25 is then divided into two separate channels 33, 34. Here again, the channels are of different sizes giving asymmetrical flow characteristics. The first and second fluid paths 25, 30 are positioned at different levels, and so as the fluid paths cross at a discreet point 35, the overlap provides fluid communication between the first and second fluid paths.
The divided channels 33, 34 of the first fluid path are then redirected through channels 60, 61 so as to return to the first level. The channels 44,45 of the second fluid path having engaged with the first fluid path, then recombine before being redirected through a channel 55 so as to bring the second fluid path to the second level. Consequently the fluid paths 25, 30 have now swapped relative positions between the levels.
In this swap of relative positions, the two fluid paths again overlap so as to meet at a further discreet point 40 providing further fluid communication between the fluid paths. In this instance, however, the relative positions of the fluid paths have changed and therefore interact at different points around the periphery of the cross section of the flow. Thus in this swapping of relative positions, an interaction between the fluid paths has been affected at different locations and so providing different interaction between the flows, increasing the surface area of the interference. In this instance, swapping of the relative positions of the fluid paths has been achieved at diametrically opposed positions through the arrangement of the two layers.
The channels 33, 34 of the first fluid path now recombine and progress into the mixing chamber 15 with the second fluid path being redirected back to the first level and also projecting into the mixing chamber 15. Thus in the first cycle of the microfluidic mixing device, the mixing zone 20 has provided for a number of different and substantial interferences with the flow so as to promote mixing of the two fluids. Each of these interferences arrangement is significantly greater than that of the prior art devices leading to substantial increases in the speed and completeness of mixing of the fluids.
Accordingly the device 150 shown in 3A is sufficient to mix the two fluids of substantially different viscosities within three mixing zones.
The three dimensional effect of the fluid paths achieves the desired swapping of relative positions of the fluid paths so as to achieve interaction and interference of the flow. Further, providing substrates having the required shapes cut into the substrates leads to a low cost solution for the manufacture of such devices. Thus the three dimensional structure may be manufactured inexpensively whilst still providing a complex chaotic mixing effect to the introduced fluids.
The four substrates 180, 185, 200, 205 are assembled to form the device 210 with the outer substrates 200, 205 sealing the fluid paths so as to retain fluid within the device. Apertures 191 are provided in one of the external substrates 200 which correspond to apertures 187 in one internal substrate 185 which in turn correspond to the inlet channels 188 for introducing the fluids to the device. Similarly an aperture 194 of the external substrate 200 correspond to an aperture 193 in the aforementioned substrate 185 which corresponds to an outlet channel 192 for removal of the mixed fluid.
Thus the chaotic microfluidic mixing device in its various embodiment provides several distinct strategies for mixing two fluids which may be used separately or together subject to their degree of mixing that is required or the degree of dissimilarity of the fluids to be mixed. Further such a three dimensional chaotic mixer also offers an opportunity for a very low cost means of construction in a still further embodiment through the use of stamped, punched or cut substrates providing the microfluidic channels which are subsequently sealed by external substrates to form a simple assembly as shown in
The device includes entry points 230, 235 into which fluids are introduced, with lead-in channels 240, 245 directing the fluids into the mixing zone.
The device 220 further includes mixing chambers 255 separating each mixing zone 250. The mixing process ends through the fluid flowing through the final outlet channel 260 to be extracted through exit point 265.
The periodic nature of the mixing device according to the present invention maybe alternatively described as a plurality of modules which have been combined with entry and exit points from the basis of the mixing process.
The second fluid path 280 is defined by a single inlet 290 which separates at a division point 315 to eventually flow through outlets 300, 310.
As with previous embodiments, the module 270 is constructed on two separate planes with the second fluid path being substantially in the upper plane. Fluid received through the inlet 290 flows through a cross plane channel 292 from the first plane into the second plane with the highlighted portion of the second fluid path 280 representing the path in the second plane. Downstream from the division point 315 are further cross plane channels 316, 317 which return the flow to the first plane.
Having the fluid paths in respective parallel planes allows for the fluid paths to come into contact at the straight points 325, 330 which include apparatus between the paths to commit fluid communication. As discussed in previous embodiment, the fluid communication promotes mixing the fluid paths and so assisting with the mixing of the fluids. Thus the construction of a microfluidic mixing device accordingly to various embodiments may be defined in terms of modules used in the construction with each module determining a degree of mixing that occurs within the device.
For example referring again to
Here a mixing zone 380 comprises a first and second fluid path as previously described. Combined with the mixing zone 380 is a mixing chamber 420. The intent is for the fluids to undergo a degree of mixing within the first and second fluid paths, with a chaotic element added to the mixture as the fluids enter the larger mixing chamber. In a further embodiment the mixing chamber may be significantly larger than that of the channels 385, 400, 410 of the first and second fluid paths. Thus the sudden pressure loss experienced by the fluid may lead from laminar flow to turbulent flow as a result of the expansion into the mixing chamber.
In a further embodiment, in order to achieve the expansion effect, the width 415 of the mixing chamber adjacent to the inlet from the first and second paths may be equal to or greater than the sum of the widths 390, 395, 405 of the channels of the first and second fluid path.
Experimental Results
A prototype of a device according to the present invention was fabricated with 2.5 mm-thick PMMA plate and using CNC micro-milling. A DIXI end mill 7256 Ø0.35 was used for machining of the microstructures. The channel widths are: w0=600, w1=450, w2=750 (μm). The diameter of the chamber is 3.45 mm. The structure depth for both the layers is 400 μm.
The device was examined using glycerol (with 2 vol % phenolphthalein pH indicator) and 1 wt % NaOH aqueous solution. Their flow rates are indicated with Q1 and Q2. At Q1=Q2=0.2 ml/min, the average Re is around
The first stage is from the inlet to chamber C2. In this stage, the less viscous liquid is confined by the more viscous liquid to form thin fluid streams. The flow is stable and the mixing mainly relies on diffusion. Starting from C2, the flow automatically transits to an unstable state. Slight instability first appears at the bottom of C2 (left side when facing the incoming flow), and it grows stronger downstream. In C3 the flow turns to fully developed turbulence. After that, the flow slowly calms down in the 4th and 5th mixer unit. In this stage, the mixing is significantly improved by the turbulent fluid motion. Through efficient mixing, the homogeneity of the fluids has been much improved. After C5, the flow restores to the steady state.
The mixer is further tested using more viscous complex polymer samples. The samples are shear-thinning fluids, for which the viscosities decrease with the increasing rate of shear stress. Three samples were tested. The changes in their viscosities with the shear rate were measured using an Anton Paar rheometer (Physica MCR 301). At shear rate 1 l/s, their viscosities are: SBS1, 5440; SBS2, 17300; SBS3, 54600 cP. The samples are to be mixed with water inclusive 1% food dye (around 1 cP).
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/SG2009/000493 | 12/23/2009 | WO | 00 | 6/22/2012 |
Publishing Document | Publishing Date | Country | Kind |
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WO2011/078790 | 6/30/2011 | WO | A |
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Number | Date | Country | |
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20120269027 A1 | Oct 2012 | US |