The present invention relates to a fluidic device comprising or associated with an operative cavity of the reactor type, allowing, without any mechanical or moving parts, firstly, the isolation of the content of said cavity and, secondly, the isolation with agitation of the content of this cavity.
More particularly, the invention relates to a fluidic device of the microfluidic type, which can be used, by way of example, in systems or devices of the “lab-on-a-chip” type. Today, microfluidics is a technical field that is undergoing development for the purposes of various medical, pharmaceutical, biological and chemical applications. In simple terms, it involves treating liquids, gases and solids, where appropriate, in devices or structures for which the unit volume is between 1 nanoliter and 1 microliter. On this scale, it is consequently necessary or preferred to exclude all mechanical pieces, in particular with a moving part, and, by way of example, thermopneumatics is selected as actuating or motor principle, in particular for the circulation of liquid in such systems.
The main functions required on a much larger scale for treating liquids and gases have been designed and developed so as to be suitable on a microfluidic scale.
As regards, first of all, valves or gates, or more generally means allowing any control of the flow rate of a liquid, various solutions using microbubbles of gas or vapor have been proposed. By way of example, reference will be made to the following publications:
As regards the pumping function of a liquid, and more generally the increase in pressure of a said liquid, mention will be made, by way of example, of the following publications:
As regards also the mixture of two components and, for example, of two liquids, reference will be made to the following work:
In accordance with U.S. Pat. No. 6,193,471, a fluidic device has been described for forming and transporting predetermined volumes of a liquid. For this purpose, according to an embodiment described with reference to
In accordance with U.S. Pat. No. 6,193,471, the formation and the transport of an isolated volume of liquid are obtained by means of the differentiated control, from the outside, of a pressure, respectively in the reserve chamber and in the storage cavities, these control means, which are particularly complex, being represented, for example, with reference to
In accordance with U.S. Pat. No. 4,676,274, a microfluidic device is described, consisting of an arrangement of capillary ducts comprising various capillary valves, with no moving parts, each constructed so as to generate an overpressure at the interface between a control gas and a liquid of interest, or meniscus. Through the outside control of the control gas, into or out of the fluidic device, at the various capillary valves, the liquid of interest can be circulated or “pumped” according to any pre-established process.
In accordance with U.S. Pat. No. 6,117,396, a microfluidic device has been described, for distributing predetermined volumes of a liquid of interest, from one and the same inlet duct, by means of an external source of gas injected into said device so as to displace said predetermined volumes.
In a microfluidic device of the type such as those defined or described above, the present invention relates specifically to the following function, namely the isolation in an operative cavity of a volume of liquid that fills said cavity, optionally with stirring of said volume in said cavity.
The object of the present invention is to effect this function with particularly simple fluidic means.
To this end, a fluidic device according to the present invention, produced from one or more components, for example from a support, comprises:
Consequently, according to the present invention, on either side of the operative cavity, an inlet or outlet duct and a channel for connection with a trapping chamber communicate, directly or indirectly, with the same valve body with no moving parts, of the gate type, placed on the operative cavity. In other words, a said connecting channel is connected up to an inlet or outlet duct, for example by means of an expansion chamber, as described or defined hereinafter.
By way of example, the ducts under consideration in the present invention are capillary ducts, in the sense that, with respect to a predetermined liquid, they are capable of containing the latter at a certain height against gravity. By way of illustration, such ducts have a cross section whose transverse dimension (or diameter) does not exceed 1.5 mm, for example of the order of 500 μm.
When, according to the present invention, a “cavity” or “chamber” is envisioned, the shape and/or the dimensions thereof differentiate it from a duct in the sense that, following one dimension, for example in the direction of circulation of the liquid, the other dimension(s) of the cavity or chamber are greater than that, for example transverse, of a duct.
A device according to the present invention constitutes, by means of the trapping chambers, a thermopneumatic system in the sense that only thermal actuation makes it possible to control the pressure and/or the volume of the gas in the trapping chambers.
Preferably, the device comprises, on either side of the operative cavity, two isolating means placed, respectively, on the two ducts, for example inlet and outlet ducts, each constructed to take up two positions, namely a position which establishes communication of one said duct with the outside, and another position which isolates said duct from the outside. By isolating the device with respect to the outside, by means of the two isolating means in the closed position, said device becomes a closed thermodynamic system, in particular with respect to the gas which it contains, trapped in the trapping chambers.
Preferably, a device according to the present invention comprises two expansion chambers, each one placed between said operative cavity and each duct, each chamber communicating on one side with said duct by means of a first capillary valve with no moving parts, that opposes any capillary liquid passage, that opposes any flow of liquid to said chamber and, on the other side, with said cavity by means of a second capillary valve, that opposes any flow of liquid to said chamber.
By way of example, the two connecting channels each connect a trapping chamber with an expansion chamber. In addition, each expansion chamber constitutes the junction between an inlet or outlet duct and a channel for connection with a trapping chamber, on each side of the operative cavity.
The means for controlling the pressure and/or the volume of the gas in one and/or the other trapping chamber are:
The term “hot source” is intended to mean any source capable of providing and/or receiving heat.
Each of these hot sources may be an integrated resistor on the valve of the fluidic device, for example a platinum resistor produced by photolithography, on a valve made of glass, aligned facing one or other trapping chamber during the assembly of the valve with the support. This resistor may have a resistance of around 25 to 50 ohms.
Each of these hot sources may be an emitter of radiation, for example infrared radiation, capable of being absorbed by the gas present in the trapping chambers.
According to another embodiment, it may be advantageous to have only one hot source, alternatively placed facing one and then the other trapping chamber.
The present invention is now described with reference to the attached drawing, in which:
FIGS. 4 to 6 represent, diagrammatically, respectively three embodiments of any capillary valve belonging to a device according to the invention and, by way of example, placed at the junction between a connecting channel and an expansion chamber belonging to the device according to
FIGS. 9 to 11 represent another “threshold” embodiment of an expansion chamber belonging to a device according to
In accordance with
In general, with reference to
The term “capillary valve”, and with reference by way of example to the valve represented as an enlargement under reference (71) in
In practice, the formation and the reproducibility of such a meniscus depend on many factors, among which mention may be made of:
As shown by way of example in
In practice, given the microtechnology used, the operative cavity (3) constitutes, for example, a microreactor having a volume of around 0.1 μl, the expansion chambers (61) and (62) having a volume of around 0.03 μl, and also the trapping chambers (81) and (82) having a volume of around 0.03 μl to 0.15 μl.
In practice, a fluidic device 1 as described above is, moreover, suitable (but in a manner not represented) for working in a technical environment that provides it with:
During the active operating phase of a device according to the invention, i.e. the isolation of the operative cavity filled with the liquid of interest, with or without agitation, said device is isolated from the outside by the means 201 and 202, in the closed position, and constitutes a closed system of heat exchange with the sources 21 and/or 22.
By construction, according to the support (12), the geometry and the size of the fluidic device (1), those skilled in the art will adopt and adjust many parameters, so as to obtain stable and reproducible operation of said device. Among these parameters, mention may be made of:
The form of the operative cavity (3) can be optimized according to the application envisioned. The capillary form, shown in
The device described above is now used for isolating or confining the content of an operative cavity (3), according to the operations, defined hereinafter.
At the start, the device (1) is empty, and the isolating means (201 and 202) are in the open position, as shown in
Preferably, the operative cavity (3) and the expansion chambers (61) and (62) are filled by forced circulation, for example by means of an external pump, of the liquid of interest, from the inlet duct (41) to the other, outlet duct (42), retaining a residual gas and therefore ambient air in the two trapping chambers (81) and (82). The ambient air is therefore trapped in the chambers (81) and (82) at a “filling” temperature, which may be identical to or different from ambient temperature, and at a pressure that is substantially equal to the outlet pressure, i.e. that available in the duct (42).
Given the capillary valves (101) and (102) described above, resulting from the construction of the device according to
FIGS. 4 to 6 describe various possible forms of capillary valve.
The overpressure thus obtained at a capillary valve as described above means that the requirement as to the pressure to be applied to the residual gas is not as great.
The capillary valve (101) or (102) can be produced according to one of the embodiments represented diagrammatically in
After circulation of the liquid of interest, the state of the device represented in
The device is then isolated by placing the isolating means (201 and 202) in the closed position, as represented in
Next, the residual gas is brought into the two trapping chambers (81) and (82) at an “isolating” temperature, that is greater than the temperature previously referred to as filling temperature, so as to bring the pressure in the trapping chambers (81) and (82) to a value that is sufficient to evacuate all the liquid of interest from the two expansion chambers (61) and (62), by means of the two ducts (41) and (42), respectively. As a result, the expansion chambers (61) and (62) are filled with two bubbles of residual gas, isolating the operative cavity (3) with respect to any leakage of the liquid of interest and/or to any diffusion of the particles contained in said liquid of interest, to the ducts (41) and (42), or from said ducts (41) and (42) to said cavity (3).
Throughout the description, the term “particle” is intended to mean any discrete element, for example an element carrying biological information, such as an electrically charged, magnetic or nonmagnetic particle carrying a biological molecule.
The state of the device represented in
This isolating step can be carried out according to different modes:
As regards the trapping chambers (81) and (82), they are of a size such that they initially contain a volume of the residual gas which, when heated to the “isolating” temperature, completely or partially occupies the expansion chambers (61) and (62) respectively. Moreover, these same chambers (81) and (82) have a compensating role, when liquid naturally returns toward them at the time the device is cooled to a temperature that is optionally lower than the filling temperature. As soon as the temperature increases again, the liquid returns, without being captured in the chambers (81) and (82), to the expansion chambers (61) and (62) respectively.
It is clearly understood that the use of the fluidic device (1), for the purposes of isolating or confining an operative cavity (3) described above, can be carried out without the expansion chambers (61) and (62).
According to the description above, it is therefore possible to isolate a reaction mixture against the diffusion to the outside of any particles or species that it contains, in a particularly simple manner, and in particular by means of a purely thermopneumatic, in particular thermodynamic, actuation of the device. By virtue of this confinement, the concentration of the reaction mixture is not modified, which may be essential for the yield and for the integrity of the reaction carried out.
The use of the same fluidic device (1) for agitating the content of the operative cavity (3) will now be described. For such a use:
As already described with reference to
The device (1) is isolated with the means (201 and 202) in the closed position.
The temperature of the residual gas in both the trapping chambers (81) and (82) is increased from the filling temperature to a reference temperature; this increase in the temperature in the chambers (81) and (82) is preferably simultaneous. However, the reference temperature in the trapping chamber (82) has a high value that is greater than the “low” value in the other trapping chamber (81). Because of this difference in reference temperatures, respectively in the chambers (81) and (82), the expansion chamber (62) is completely filled with a bubble of the residual gas, while the expansion chamber (61) is partially filled with the same residual gas. Consequently, firstly, a discrete quota (20) of the liquid of interest remains in the expansion chamber (61) and, secondly, the residual gas is compressed on the side of the expansion (61) and trapping (81) chambers. The state of the device represented in
Between the states of the device (1) represented, respectively, in
Next, the temperature of the residual gas in the other trapping chamber (81) is increased, by an increment Δt, from the reference temperature previously attained, while the reference temperature in the trapping chamber (82) is not modified. It is of course possible to simply reverse the heat exchanges of the heat sources (21, 22) in order to achieve the same result. Consequently, firstly, the quota (20) of the liquid of interest is displaced from the operative cavity (3) to the expansion chamber (62) associated with the trapping chamber (81), and is thus evacuated from the expansion chamber (61) and, secondly, the residual gas is compressed in the expansion chamber (62).
The state of the device represented in
This cooling may be advantageously obtained naturally, by simple convection and dissipation of the heat, since the fluidic device according to the invention has very small dimensions.
The temperature of the residual gas in the other (81) of the trapping chambers is then returned to the “reference” temperature, at its low value, in return for which the same quota (20) is displaced to the expansion chamber (61) associated with said trapping chamber (81), so as to again achieve the state represented diagrammatically in
The operations described above can be brought about a whole number of times, so as to generate oscillations in the discrete quota (20) on either side of the operative cavity (3). These oscillations may be obtained at frequencies of 0.5 Hz to 25 Hz. They may be brought about over a period of the order of one hour, corresponding to the duration of the chemical (or other) reaction in the operative cavity (3).
Consequently, the fluidic device (1) according to
The pressure obtained in step (d) is the equilibrium pressure.
Preferably, steps (c) and (d) are repeated.
The operations described above can be brought about a whole number of times, so as to generate oscillations in the discrete quota (20) on either side of the operative cavity (3), through the latter, the residual gas being compressed in each direction, or in the expansion chamber (62) or in the expansion chamber (61), and each time exerting a return action in the opposite direction.
As described above with reference to FIGS. 1 to 3, it is observed that not only is an agitating function obtained, but also an isolating function, since the volume of the liquid of interest, present in the operative cavity (3) is isolated, with the discrete quota (20) of the same liquid, representing in general a few % of the volume of the operative cavity (3). In particular, the capillary valves (71, 72, 51, 52, 101 and 102) play exactly the same role in the agitating function as in the purely isolating function.
By means of the same capillary valves, the residual gas is compressed, without being able to flow either toward the inlet duct (41) or toward the outlet duct (42). Thus, the residual gas can play a shock-absorbing role in the agitating function described above.
The quota (20) of the liquid of interest is determined via the combination of the geometry of the expansion chambers (61) and (62), and the choice of the “agitation” temperatures disclosed above.
As shown in FIGS. 9 to 11, the expansion chambers (61) or (62) may have a predetermined geometry so as to obtain a “threshold” structure.
According to these figures, each expansion chamber (61) or (62) comprises, in the direction of the operative cavity (3), two successive narrowings A and B, toward diameters or cross sections that are respectively less with respect to one another. Consequently, starting with complete filling of the expansion chamber (61) according to
Of course, the agitation described above with reference to
Overall, by means of the fluidic device according to the invention, it is possible, particularly simply and merely with a thermal or other control, to obtain both an isolation in the operative cavity (3) against any leakage of said liquid and/or diffusion of particles to the outside, or the same isolation but with agitation.
A fluidic device as described or defined above is particularly suitable for carrying out a method, such as ELISA or ELOSA, for determining a target species, or analyte, described schematically hereinafter with reference to
According to this method, it involves determining, i.e. qualitatively and/or quantitatively detecting, a target species or analyte (C), comprising two sites (C1, C2) for binding, respectively, with a first ligand (L1) and with a second ligand (L2) linked directly or indirectly to a label E.
To this ends the method comprises the following steps:
This method, defined in general, of the immunoassay type, may be the subject of various adjustments or additions, in particular according to the analyte (C), or to the device for implementing it. Thus:
In a manner well known to those skilled in the art in the immunoassay field:
In order to carry out a method of determination as defined above, a device in accordance with
In this way, the conjugate 301 can circulate to the operative cavity (3) and bind, in the latter, with the particles of the functionalized (M2, L3) support 303.
Number | Date | Country | Kind |
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02/08038 | Jun 2002 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/FR03/01946 | 6/24/2003 | WO | 1/5/2005 |