This invention pertains generally to magnetic separation systems. More specifically, this invention pertains to the design and mechanism of a magnetic separation system with pre and post processing modules.
Sorting small amounts of biological and non-biological material is an important capability in biology and medicine. The target and/or non-target species may comprise small or large chemical entities of natural or synthetic origin such as chemical compounds, supermolecular assemblies, proteins, cells, viruses, bacteria, organelles, other intracellular materials, fragments, analytes, glasses, ceramics, etc. Magnetic Activated Cell Sorting (MACS) is sometimes used as a cell sorting technique because it allows the rapid selection of a large number of target cells. The applications of MACS span a broad spectrum, ranging from protein purification to cell based therapies. Typically, target materials are labeled with one or more superparamagnetic particles that are conjugated to a molecular recognition element (e.g. a monoclonal antibody) which recognizes a particular surface marker of the target.
In order to achieve high throughput and high recovery of the rare target materials (or other target components), improvements on existing MACS systems are needed.
A system for sorting and trapping magnetic target species includes a microfluidic sorting chamber designed to receive and then temporarily hold magnetic particles in place within the module. A pre-processing and/or post-processing module is in fluidic communication with the sorting chamber. A pre-processing module may mix a sample and magnetic particles to cause certain species in the sample to be labeled. The microfluidic chamber may include a mechanism to move magnetic particles within the chamber. A post-processing module or the microfluidic chamber may be used to separate the labeled species from the magnetic particles by adding a release reagent. The magnetic particles and/or their payloads may be released and separately collected at an outlet of the chamber or the post-processing module.
In various embodiments, a fluidic sorting and trapping system is designed or adapted to receive, label one or more species in a sample, and then temporarily hold magnetic particles in place within a sorting chamber or module. The captured species are then released, collected, and/or further processed. In such embodiments, the magnetic particles flowing into the sorting chamber are trapped there while the other sample components (non-magnetic) continuously flow through and out of the chamber, thereby separating and concentrating the species captured on the magnetic particles. Only after the non-magnetic sample components have flowed out of the sorting chamber are the magnetic particles and/or their payloads released and separately collected at an outlet of the sorting chamber.
According to various embodiments, magnetic particles are subjected to hydrodynamic forces within a region of fluidics system such as a chamber on a unitary fluidics device in order to facilitate labeling magnetic particles, releasing captured species from magnetic particles or otherwise processing a fluid medium containing magnetic particles. In a pre-processing module, one or more reservoirs on the fluidic device may receive a fluid medium containing a sample, magnetic particles, and/or a selection entity such as an antibody marker. These components may be delivered separately to different reservoirs, e.g., a sample reservoir and a magnetic particle reservoir. These reservoirs may be in fluid communication with each other and with the sorting chamber. Valves between reservoirs and the sorting chamber control pre-processing flow and processing flow.
In certain embodiments, contents of the reservoirs may be mixed by moving the fluid medium from one reservoir to another. For example, the fluid medium may be from different reservoirs may be mixed via pneumatic pressure, magnetic field, ultrasonic agitation, stirring, and the like. The pre-processing may incubate or label a sample with magnetic particles and selection entities. In some embodiments, pre-processing may include washing raw magnetic particles, for example, magnetic particles containing preservatives, with a wash buffer prior to labeling.
While the magnetic particles and the bound species are temporarily trapped in the sorting chamber, buffer flow may remove unlabeled and other material from the chamber. Further, the buffer flow may be stopped to allow agitation of the magnetic particles and bound species trapped in the sorting chamber. According to various embodiments, this agitation and movement may further release unlabeled and unwanted material from being physically immobilized among the magnetic particles. This agitation and movement may be caused by magnetic forces induced by alternating magnets, ultrasonic waves, mechanical stirring, pneumatic pressure, and other forces. The magnetic particles and bound species may be then immobilized again while more buffer flows through the sorting chamber to further remove the unlabeled and unwanted material.
In still other embodiments, post processing operations may be performed on the trapped and concentrated magnetic particles with bound species in the sorting chamber or in a post-processing module. Reagents may be added to lyse cells, further react with the trapped material, or release the bound species from the magnetic particles. In certain embodiments, the magnetic particles and/or the released species may be separately collected at an outlet of the chamber or the post-processing module.
These and other features and embodiments of the invention will be described in more detail below with reference to the associated drawings.
Introduction and Context
Magnetic Activated Cell Sorting (MACS) systems are capable of high-purity selection of the labeled sample components. In certain embodiments these systems operate in a “trapping mode” where the non-target and target species are sequentially eluted after the application of the external magnetic field. In other words, the species attached to magnetic particles are held in place while the unattached species are eluted. Then, after this first elution step is completed, the species that are attached magnetic field and were prevented from being eluted are freed in some manner such that they can be eluted and recovered. In other embodiments, the systems operate in a “deflection mode” in which labeled and unlabeled species from a sample flow through a sorting region exposed to a magnetic field, and those species labeled with magnetic particles are deflected into an outlet chamber where they can be collected in purified form.
In accordance with embodiments of this invention, magnetic particles are subjected to hydrodynamic forces in order to mix them with a reagent and/or in some cases expose them to shear forces to remove attached species. In certain embodiments, the magnetic particles are exposed such forces while the particles are constrained to a region of a fluidics device such as a chamber or channel; e.g., a sorting region or a pair of reservoirs used for labeling. Typically, though not necessarily, the magnetic particles are suspended within a fluid during the processing; i.e., they are not confined to a particular wall of the device. Examples of systems and methods that provide fluidic mixing of magnetic particles and allow for labeling and/or release of sample species are depicted in
Typically a single fluidics device (sometimes referred to herein as a “chip”) contains both a sorting station and a one or more mixing stations as described herein. The sorting station separates magnetic from non-magnetic species from a sample. As explained, the functionalized magnetic particles specifically bind with some species (but not all species) of a sample. Thus, the two classes of species may be separated (sorted) based on their affinity for the functionalized magnetic particles. As explained below, two examples of on chip sorting mechanisms are trapping and deflection. The on chip mixing station may be employed to mix magnetic particles with sample, reagent, or other component. The fluidics device is typically, though not necessarily, a unitary device which may be easily moved about as a single portable unit. In some embodiments it is formed from a single solid substrate (e.g., glass or polymer), which may be monolithic and contain multiple stations, channels, ports, and/or other fluidics components. The device may be designed for a single use and therefore be disposable.
For context an example of a trapping-type magnetic separation system will now be described.
In the depicted embodiment, a pressure system (including a syringe pump and a pressure controller) provides the principal driving force for flowing sample through the trapping module. Of course, other designs may be employed using alternative driving forces such as a continuous pump. Buffer from buffer reservoirs is also provided to the cartridge under the controlled by a buffer pump and a flow control module. Further, as described in more detail herein, various forces may be employed to facilitate mixing of magnetic particles with other components such as samples, release reagents, labeling regents, and other reagents used to process the magnetic particles. Examples of such forces include forces applied by varying external magnetic fields, delivering pneumatic pressure, etc.
In
As shown, target species 145 are captured on the trapping region. The remaining uncaptured material 149 (or other species) and debris provided with the sample are washed clear of the trapping region because they are not affixed to magnetic particles.
It should be noted that positive or negative trapping schemes may be employed. In a positive trapping scheme as shown in
A side view of the trapping region in action is depicted in
In certain embodiments, the magnetic field is controlled using an electromagnet. In other embodiments, permanent magnets may be used, which are mechanically movable into and out of proximity with the sorting station such that the magnetic field gradient in the sorting region can be locally increased and decreased to facilitate sequential capture and release of the magnetic particles. In some cases using an electromagnet, the magnetic field is controlled so that a strong field gradient is produced early in the process (during capture of the magnetic particles) and then reduced or removed later in the process (during release of the particles).
As shown in the example of
In some embodiments, the trapping region is relatively thin but may be quite wide to provide relatively high throughput. In other words, the cross-sectional area of the channel itself is relatively large while the height or depth of the channel is quite thin. The thinness of the channel may be defined by the effective reach of the magnetic field which is used to attract the magnetic particles flowing through the trapping region in the fluid medium.
Various details of fluidics systems suitable for use with this invention are discussed in other contexts in the description of flow modules in U.S. patent application Ser. No. 11/583,989 filed Oct. 18, 2006 and U.S. Provisional Patent Application No. 61/037,994 filed Mar. 19, 2008, both of which are incorporated herein by reference in their entireties and for all purposes. Examples of such details include buffer composition, magnetic particle features, external magnet features, ferromagnetic materials for MFGs, flow conditions, sample types, integration with other modules, control systems for fluidics and magnetic elements, binding mechanisms between target species and magnetic particles, etc. Generally, in a magnetic trapping module the applied external magnetic field will be relatively higher (considering the overall design of the module) than that employed in a continuous flow magnetic flow sorter of the type described in U.S. patent application Ser. No. 11/583,989. In either case, the magnetic force exerted on target species should be sufficiently greater than the hydrodynamic drag force in order to ensure that the target species (coupled to magnetic particles) are deflected or captured and held in place against the flowing fluid.
In a typical example, the magnetic trapping process proceeds as follows. First, a sample such as a biological specimen potentially containing the target material, which may be cells, parts of cells, protein, or smaller material, are labeled with small magnetic particles coated with a capture moiety (e.g., an antibody) specific for the surface marker of the target material. This labeling process may take place on or off the microfluidic sorting device. In accordance with certain embodiments, the labeling is performed on the same device in a pre-processing module. After this labeling, the sample is flowed into the sorting station (comprising a trapping or deflection region) with or without concurrently flowing buffer solution. Buffer may be delivered through one or more inlets and sample through one or more others. The sorting station is energized with an external magnetic field to deflect or hold the magnetically labeled target cells or other species against the hydrodynamic drag force exerted by the flowing fluid. This occurs while continuously eluting the un-labeled non-target species. As explained above, the magnetic field is typically applied by an external magnet positioned proximate the sorting station. In the trapping embodiments, after most or all of the sample solution has flowed clear of the sorting station, the magnetic components are released. This may be accomplished by any of a number of different mechanisms including some that involve modifying the magnetic field gradient and/or increasing the hydrodynamic force. For example, the magnetic field in the chamber may be reduced, removed, or reoriented and concurrently the sample inlet flow is replaced with release agent (for releasing the captured species) and/or buffer flow. Ultimately the previously immobilized magnetic components, or just their captured species (now purified), flow out of the chamber in a buffer solution. The purified sample component comprising the target species may then be collected at an outlet of the sorting chamber, which, in some configurations may be located directly downstream from the trapping chamber.
It should be understood that embodiments of the invention are not limited to analysis of biological or even organic materials, but extend to non-biological and inorganic materials. Thus, the apparatus and methods described herein can be used to screen, analyze or otherwise process a wide range of biological and non-biological substances in liquids. The target and/or non-target species may comprise small or large chemical entities of natural or synthetic origin such as chemical compounds, supermolecular assemblies, proteins, organelles, fragments, glasses, ceramics, etc. In certain embodiments, they are monomers, oligomers, and/or polymers having any degree of branching. They may be expressed on a cell or virus or they may be independent entities. They may also be complete cells or viruses themselves.
The magnetic capture particles employed in separations of this invention may take many different forms. In certain embodiments, they are superparamagnetic particles or nanoparticles, although in some cases they may be ferromagnetic or paramagnetic. As a general proposition, the magnetic particles should be chosen to have a size, mass, and susceptibility that allow them to be easily diverted from the direction of fluid flow when exposed to a magnetic field in microfluidic device (balancing hydrodynamic and magnetic effects). In certain embodiments, the particles do not retain magnetism when the field is removed. In a typical example, the magnetic particles comprise iron oxide (Fe2O3 and/or Fe3O4) with diameters ranging from about 10 nanometers to about 100 micrometers. However, embodiments are contemplated in which even larger magnetic particles are used.
The magnetic particles may be coated with a material rendering them compatible with the fluidics environment and allowing coupling to particular target components. Examples of coatings include polymer shells, glasses, ceramics, gels, etc. In certain embodiments, the coatings are themselves coated with a material that facilitates coupling or physical association with targets. For example, a polymer coating on a micromagnetic particle may be coated with an antibody, nucleic acid sequence, avidin, or biotin.
One class of magnetic particles is the nanoparticles such as those available from Miltenyi Biotec Corporation of Bergisch Gladbach, Germany. These are relatively small particles made from coated single-domain iron oxide particles, typically in the range of about 10 to 100 nanometers diameter. They are coupled to specific antibodies, nucleic acids, proteins, etc. Magnetic particles of another type are made from magnetic nanoparticles embedded in a polymer matrix such as polystyrene. These are typically smooth and generally spherical having diameters of about 1 to 5 micrometers. Suitable beads are available from Invitrogen Corporation, Carlsbad, Calif. These beads are also coupled to specific antibodies, nucleic acids, proteins, etc.
As indicated, aspects of this invention pertain to on chip mixing of magnetic particles which may be suspended in a fluidics medium. The mixing involves exposing the magnetic particles to hydrodynamic forces which may originate from various sources. Examples of such sources include pneumatic or hydraulic sources, varying external magnetic and/or electric fields, mechanical stirring, and gravitational fields (e.g., caused artificially by rotational forces). Regardless of the origin of the hydrodynamic force, the magnetic particles are typically confined to a particular region of a fluidics device during the processing. Thus, the particles are typically not subjected to a sorting process in which a magnetically bound portion of a sample is separated from the remainder of the sample. The two following sections present specific examples of pre-separation labeling of sample species and post-separation release of such species.
Pre-Separation Processing
This aspect of the invention pertains to ways to insure that the target or non-target components of a sample become “labeled” with magnetic beads as appropriate. This labeling operation is performed upstream (prior to) the trapping/separating stage in which the magnetic particles are captured and held stationary in a flowing fluid medium.
As explained, the magnetic particles will have a surface functional group that has a specific affinity for either the target or non-target species. Thus, when the magnetic particles come in contact with the relevant species, they bind with those species to form conjugates. An inventive operation pertains to a mechanism for facilitating the binding or conjunction of the magnetic particles with the appropriate species or component from the sample.
Typically, though not necessarily, this pre-sorting treatment is performed in one or more separate chambers or reservoirs located in fluid communication with the trapping region. Such chambers or reservoirs may be located on the same device (chip) as the trapping region or in a separate device or chip. They may have micro fluidic dimensions or even slightly larger dimensions if appropriate. In one example, each of one or more pre-treatment reservoirs has a volume of approximately five milliliters. Typically, the reservoirs may be between 0.5 ml to 10 ml.
The magnetic beads, as well as the sample, and other reagents to facilitate binding are each provided to the reservoir or reservoirs. Note that the magnetic particles may be provided in a functionalized form, in which case it will be unnecessary to provide the other reagents. There, the magnetic particles are moved with respect to the other components in the reservoir(s) to facilitate labeling. This movement is induced by successive application of pneumatic pressure two separate chambers in accordance with certain embodiments. In some embodiments, this movement is induced by a magnetic mixing mechanism of the type described for magnetic particle release as described in a later section. The same mechanisms for facilitating mixing may be employed; e.g., a moving a magnetic field as by, for example, oscillating the field. Other examples of mixing mechanisms include ultrasonic agitation or stirring.
A specific example of a sequence of operations involving a pneumatic labeling operation is presented in
Next as illustrated in block 203, magnetic particles (coated with a capture agent such an antibody specific for a target or non-target species in a sample) are added to a second on chip reservoir, which is fluidically connected to the first on-chip reservoir, although it may be temporarily isolated by a closed valve located between the two reservoirs. The magnetic particles may be delivered to the second reservoir manually or automatically as described above for delivery of the sample to the first reservoir.
After filling the reservoirs, each is capped or otherwise sealed in order to prevent the fluids from escaping during on chip mixing. See block 205. This operation is completed after all of the reservoirs have completed the filling process. The capping mechanism may be achieved using a double edge seal, which is integrated into the design of the caps over each well (see
Next as illustrated in a block 207, a valve between the first and second reservoirs is opened to allow the fluids in the two reservoirs to mix. In an alternative embodiment, the two reservoirs are not fluidically isolated during the sample and magnetic particle filling operations. In such embodiments, operation 207 is unnecessary.
At this point, the contents of the reservoirs is mixed by pneumatically pushing the contents back and forth between the two reservoirs. See block 209. This mixing may facilitate labeling of particular sample species with the magnetic particles. Alternatively it may facilitate some other pre-sorting process such as contacting a sample with a buffer. In any case, the pneumatic pressure and/or vacuum is sequentially applied to the two reservoirs so that the contents are driven toward one or the other of the reservoirs at any given time.
Finally, as illustrated in block 211 of
In the depicted embodiment, the pneumatic system connected to wells on the chip includes four components per well: a pump, a proportional valve, a switching valve, and a pressure transducer. This arrangement is duplicated for each well, although the pump may be common for all wells. The two valves (proportional and switching) respectively serve the purpose of metering the air pressure at the wells, and venting the wells to atmosphere. By venting the wells to atmosphere, residual air pressure in the reservoirs is released immediately, stopping fluid flow in the chip instantly. The pressure transducer and proportional valves are, in some embodiments, linked in a closed-feedback loop to maintain a set pressure and flowrate, determined by the current stage of the mixing/separation process.
In
A buffer subsystem is depicted in dashed lines and includes in addition to the on-chip buffer reservoir a proportionate valve PV1 (220), a switching valve SV1 (221) and a pressure transducer T1 (222). The proportionate valve PV1 (220) opens and closes by degrees dictated by the magnitude of an applied control signal (e.g., electrical voltage) and applies precisely controlled pressure levels to the buffer reservoir 216. The switching valve SV1 (221) has two settings, one allowing direct application of pressure from valve PV1 (220) to the buffer reservoir 216 and another allowing venting from the buffer chamber to atmosphere 223. Pressure transducer T1 (222) measures the pressure applied to the buffer reservoir 216. The measured pressure is provided as feedback to proportionate valve PV1 to maintain a desired pressure in the buffer reservoir. Note that the pressure is directly proportional to the flow rate, which is the parameter of most importance in the fluidics system.
In some embodiments, buffer is metered into sample reservoirs S1 217 and S2 218 through an on chip valve V1224 in an open position. After a sufficient amount of buffer is delivered to the sample chambers, valve V1224 is closed and the sample is mixed in a manner as set forth below. This approach may be particularly appropriate in designs where the chip is supplied with pre-packaged reagents.
In certain embodiments, buffer is not added to the sample reservoir prior to mixing. In such cases, buffer may still be metered into sample reservoirs, but only to rinse the sample once the mixing is performed and the sample is flowed into the trapping region.
Buffer may also be delivered to the edges of the trapping region via lines 225 shown along the edge of the separation chip. During a sorting process, this is performed in conjunction with delivering the sample from reservoirs S1 and S2 to the trapping region.
Pressure to sample reservoirs S1 and S2 is provided from the pump via various fluidic components depicted on the dotted lines. Sample reservoir S1 (217) has associated proportionate valve PV3, switching valve SV3 and pressure transducer T3. Sample reservoir S2 (218) has associated proportionate valve PV2, switching valve SV2 and pressure transducer T2. These act on reservoirs S1 and S2 in the same manner as elements PV1, SV1, and T1 act on the Buffer reservoir 216.
Mixing of the sample may be accomplished by passing the sample (and associated fluidic components) back and forth between reservoirs S1 and S2 through the hatched path 226 joining them. This is performed by alternately applying pressure to each reservoir while a valve V2 remains shut. After a sufficient number of cycles (e.g., about 10-500), the sample is sufficiently mixed and can be supplied to the trapping region to effect sorting.
Note that the components applied sample reservoirs include, in addition to sample, magnetic particles and optionally an affinity binding reagent (e.g., an antibody). After mixing, the beads are coupled to target species via the binding reagent, which is coupled to the bead surface. As indicated buffer is supplied to the sample reservoirs from the buffer reservoir. Prior to mixing, a user may apply the sample, the magnetic particles and the optional binding reagent to the sample reservoirs. The user may also deliver buffer to the Buffer reservoir 216 and a bead release agent to a bead release reservoir (“R”) 219. Each of these components may be provided by, e.g., pipetting. Thereafter, a cap is applied to seal each reservoir and provide a port for delivering pneumatic pressure. An example of a reservoir and cap design is presented in
After the sample is mixed sufficiently, valve V2 is opened and the sample flows into the trapping region concurrently with buffer. Different collection chambers may be used depending on whether the selection method is positive or negative. In a positive selection, target particles are labeled, trapped, and collected. In a negative selection, target particles are not labeled or trapped and are collected at the outlet after the non-target species are trapped. A negative selection may be useful to isolate unknown substances in a sample by eliminating known substances. If positive selection is employed (i.e., selection for target species on the magnetic particles), valve V4 is closed and valve V3 is opened to allow non-target sample components to be collected in a chamber C−. If, on the other hand, negative selection is employed (i.e., non-target species bind to the magnetic particles), valve V4 is opened and valve V3 is closed to allow the target components from the sample to be collected in a chamber C+.
In certain embodiments, multiple trapping chambers may be connected in series to effectively concentrate a target species. In these embodiments, a first trapping chamber may trap magnetic particles with labeled species along with other undesired species. The trapped material may be released to a second trapping chamber where the target species is further concentrated by removing more of the undesired species. Through the use of two or more trapping chambers in series, very high purity collection is achieved.
A bead release sub-system 214 of the pneumatic system includes a proportionate valve PV4, a switching valve SV4, and a pressure transducer T4, in addition to the on-chip release reagent reservoir, “R.” In one embodiment, the bead release sub-system accomplishes its function on trapped beads in the trapping region as follows. Initially valve V3 is closed while valve V4 is opened (assuming a positive selection approach is employed). Valve V5 is also opened to allow bead release reagent to flow into the trapping region. After a sufficient amount of reagent flows into the trapping chamber, switching valve SV4 is turned to the vent position and no further reagent flows into the trapping region (temporarily). Then, mixing may be performed within the trapping region. In one embodiment this is accomplished by moving magnets (or arrays of magnets) located above and below the trapping region to alternately attract the magnetic particles to the top and then the bottom of the trapping region. As indicated elsewhere herein, this serves to free some trapped non-specifically bound non-target material from the magnetic particles.
After the magnetic mixing (if performed), buffer or additional release reagent may be flowed through the trapping region in order to flush the unbound target into chamber C+. In other embodiments, one or more additional cycles of reagent contact and optional mixing are performed. In such embodiments, switching valve SV4 is turned to the flow position and additional bead release reagent flows into the trapping region from the release reagent reservoir. After a sufficient amount of reagent is flowed into the region, valve SV4 is again turned to the vent position and further magnetic mixing may be performed. In some embodiments, multiple cycles (e.g., 4 cycles) of reagent contact and mixing are performed. After each cycle, additional target material is captured in chamber C+.
In certain embodiments, all components of shown within the dashed line rectangle labeled “Separation Chip” reside on a single unitary substrate such as an injection molded polymeric material (e.g., a polypropylene). A cap covers all or some portion of the substrate including at least one (and usually all) of the reservoirs.
Note that the depicted chip includes a bubble trap (“BT”) 227 on the release reagent and sample inlet lines to the trapping region. In some embodiments, the bubble trap comprises a single membrane that spans two separate channels to capture bubbles on both the reagent and sample lines as shown.
In a typical embodiment, the fluidics system applies a relatively low pressure to drive sample, buffer, and/or other fluid through the fluidics chip. For many applications and designs, a pressure in the range of 0.05 psi to 10 psi is appropriate. For example, sample mixing may be accomplished using a pressure of about 0.1 to 1 psi applied (alternately) to the two sample reservoirs. For buffer flushing, however, a higher pressure may be appropriate, e.g., about 5 psi.
In many designs, the components of the pneumatic system (pump, valves and transducers) are all commercially-available, off-the-shelf components that can be acquired at relatively low cost from vendors such as Hargraves Technology Corporation (Mooresville, N.C.), and Clippard Instrument Laboratory (Cincinnati, Ohio). In various embodiments, the entire pneumatic system may be replaced with an equivalent system delivering a set amount of flow utilizing a different force, such as hydraulic, magnetic or electrical force.
The downward sloping bottom surface facilitates draining liquid including magnetic particles (and possibly other components) through the outlet port 230. It may be generally conically shaped allow other downward sloping shapes may be used as well (e.g., various pyramidal shapes). The main holding portion 231 may be of any suitable shape such as cylindrical, oval, polygonal, etc.
In a specific embodiment, the sample reservoirs are designed with a capacity of 5 mL each, to allow complete transfer of a 5 mL from well to well. In the depicted example, the wells are cylindrical in shape, with an inverted-cone bottom surface. This shape is similar to that of a standard centrifugation tube.
As depicted in
In some cases, the cap and the upper surface of the reservoir may have mating surfaces to facilitate sealing. For example, in the depicted embodiment, the upper surface of the reservoir includes a circumferential lip 233 extending upward from a principal plane of the chip substrate. A complementary groove 234 is provided in the cap to engage the lip and provide a seal for preventing ingress and egress of liquid.
Coupling of the flow delivery system to the chip is achieved using a simple gasket 235 (e.g., an elastomeric o-ring) that creates an airtight seal with a rigid manifold 236 in the system apparatus. See
Another pre-separation processing may include washing raw magnetic particles, for example, magnetic particles containing preservatives, with a wash buffer prior to labeling. According to various embodiments, raw magnetic particles may be introduced to a sample well before any sample containing target species is added. The raw magnetic particles may contain preservatives, which is preferably removed before the particles are used to label a target species. A wash buffer may be introduced to a different sample well or the same sample well containing the magnetic particles. Mixing techniques described herein for mixing and labeling samples and for agitating magnetic particles in the sorting chamber may be used to wash the preservatives from the magnetic particles. An external magnet may be used to retain the magnetic particles in the sample well while the wash buffer drains. In other embodiments, the magnetic particles may be allowed to drain into the sorting chamber where they will become trapped by the magnetic field. From the sorting chamber, the magnetic particles may be released into an outlet where it can be collected and re-introduced in a sample well for the labeling process. In still other embodiments, the washed magnetic particles may be returned directly into the sample well.
Post-Separation Processing
The post separation operations described here involve primarily methods for releasing target species from magnetic particles that have been trapped in a trapping station or otherwise separated in a sorting station. In a typical scenario, at the end of a trapping operation, the only sample species that remain in the trapping region are bound to magnetic particles. For many applications, it is important to separate the captured species from the magnetic particles prior to further processing.
In the post separation operations described here, some mechanism for releasing the bound species from the magnetic particle is employed. Various binding and release systems are available. These include, for example, release reagents that (1) digest a linkage chemically coupling the magnetic bead to the captured species, (2) compete with chemical or biochemical linkage mechanisms for binding with the captured species, and (3) cleaving the linkage with a secondary antibody.
The advantages of magnetic mixing include (1) exposing the magnetic bound particle pair to more release agent in the solution and (2) exposing the magnetic bound particle pair to increased fluidic drag to provide stress on the linkage between the magnetic particle and its non-magnetic payload. This increases the probability of dissociation.
In accordance with some embodiments, a bead release reagent will be introduced into the trapping region, and then mixed with the magnetic particles to facilitate releasing the bound species. A flow chart shown in
The magnetic mixing operation may be characterized in terms of various parameters such as the direction of motion, the frequency of the oscillations, the duration of the process, etc. In one example, the beads were moved back and forth at a frequency of 0.15 Hertz for 15 minutes. This frequency and mixing duration are representative of an approximately minimum frequency and maximum mixing period respectively—depending on the size, magnetic field saturation strength of the beads, and other factors such as the fluid viscosity, the frequency can be varied across a wide range. In the case of relatively large magnetic beads (e.g. 4.5 μm diameter), the frequency may be increased to ˜1 Hertz, and the mixing period reduced proportionally to about 2 minutes.
The next operation of the process involves terminating the magnetic mixing operation in block 264 by, e.g., putting the strong magnetic field back into position at the bottom of the trapping region channel to thereby attract and capture the magnetic particles again. Presumably, at this point the particles are now largely unbound, i.e., separated from their target (or non-target) species.
A subsequent operation 265 involves flushing out the unbound target (or non-target) from the trapping region. This may involve flowing fresh bead release agent or other fluid through the trapping region while the magnetic particles remain affixed to the bottom of the trapping region. This causes elution of the separated species.
While the sequence of five operations depicted above may be sufficient to effectively release and elute all or substantially all the trapped target species in many applications, other applications may require multiple repetitions of operations 262 to 265 to effectively remove all the target species from the trapping region. Regardless of how many repetitions are employed, the very last elution step may involve flowing either a buffer or bead release agent into the trapping region. In all prior operations, the delivery of fresh fluid into the trapping region will typically entail delivery of a bead release agent to facilitate further release of bound target species.
The depicted apparatus includes an on chip fluidic trapping station which receives a buffer solution 280 and a mixture of labeled and unlabeled sample species. The non-target species 281 are depicted as dark circles while the target species 282 are depicted as light circles. The target species are coupled to magnetic particles 283 which are shown as small dots. The fluidics trapping station includes upstream and downstream valves that can isolate the station so that no fluid enters or leaves the station during certain operations.
The depicted apparatus also includes two groups of external magnets (284 and 285), upper and lower arrays of alternating polarity permanent magnets. These arrays can move with respect to the trapping station with at least two degrees of freedom. First, they can move laterally along the direction of flow of the sample and buffer and second, they can move in an orthogonal direction, toward and away from upper and lower surfaces of the trapping station of the fluidics device. The two arrays of magnets may move independently of one another or coupled together dependently.
The specific sequence of operations shown in
Next, as shown in panel 292, the magnet assemblies are fully in position over the capture surface of the trapping station. At this point, all magnetically-labeled species are trapped on the lower surface of the station, which may include a soft magnetic structure 286 (e.g., a ferromagnetic trapping grid). Incidentally, a few non-magnetically-tagged species 281 are also trapped due to non-specific physical entrapment. At the conclusion of this process, valves 287 (shown as “X”s) are closed at the upstream and downstream sides of the station.
Next, as shown in the panel 293, the upper/lower magnet assemblies are translated vertically to bring the upper magnet assembly 284 in contact with the top of the channel. Concurrently, the lower magnet assembly 285 is moved sufficiently far away from the device to release the magnetic beads from the lower surface, e.g., the trapping grid. The magnetically-labeled species move toward the top wall of the channel, leaving the non-magnetically-tagged species free in solution. This is down while the valves remain closed so that little or no fluid enters of leaves the trapping station.
Next as shown in panel 294, the magnet assembly position is reversed to bring the lower magnet assembly back to its original position after trapping. This operation and the previous operation can be repeated one or more times (e.g., multiple times) to ensure that all non-magnetically-labeled species are free in solution within the trapping station. In the depicted embodiment, the valves remain closed during this entire operation. Thereafter, the valves are opened and a buffer solution is pumped through the channel to elute the non-magnetically-tagged species. See panel 295 on the left side of
The bead release operations are depicted on the right set of panels in
Next, as shown in panel 298 on the right side, the magnet assembly position is reversed to bring the lower magnet assembly 285 back to its original position. The valves 287 remain closed. This operation and the previous one can be repeated one or more times to ensure that all the beads are released from their attached targets. Now, with the lower magnet assembly back at the lower position and the beads trapped on the trapping grid, the valves 287 are opened and buffer solution is flowed through the channel, eluting the now free target species. See panel 299 on the right side. Finally, in the depicted embodiment shown in panel 2100, the magnet assembly is moved halfway up to remove the interaction of both external magnetic assemblies, allowing the beads to be eluted from the channel with buffer solution.
In an alternative embodiment, the permanent magnet assemblies are replaced with electromagnets as the external magnets. The magnetic mixing may be implemented by alternating energizing electro magnets on the top and bottom of the trapping region.
In other magnetic mixing embodiments, the magnetic field moves in a direction other than bottom to top and vice or versa. As an example, mixing could be facilitated by moving the beads left and right or front to back within the trapping region so long as there is little or no flow of fluid within the trapping region during this mixing.
Dynamically Varying External Magnetic Fields
In accordance with embodiments of this invention, a dynamically varying magnetic field may be applied to the trapping region during flow of the magnetic particles. This may involve, for example, progressive insertion of a magnetic field over the trapping region during the trapping operation.
This approach has the advantage of reducing or preventing build up of magnetic particles at the leading edge or elsewhere in the trapping region. Generally, a build up has been observed to occur where the magnetic field is strongest, typically at the edge of a permanent magnet used to apply the external magnetic field. As should be clear, such build up can result in under utilization of the trapping region (portions of the trapping region where the magnetic field strength is not great might not capture many or any of the magnetic particles). Further, the clump or pile up of magnetic particles may actually block passage of further magnetic particles to the down stream portions of the trapping region. It may also capture unbound species from the sample and thereby reduce purity of the captured components of the sample.
By using a dynamically varying magnetic field in accordance with this invention, one can produce a relatively evenly dispersed layer of the magnetic particles captured over the trapping region. In some cases, this layer is effectively a monolayer of magnetic particles on the trapping region, although bilayers and the like may be produced depending upon the area of the trapping region and the quantity of sample to be processed. In some cases, the design and application may result in sub-monolayer coverage; i.e., less than the full capacity of the capture surface is utilized.
A relatively uniform distribution of magnetic particles in the trapping region may be useful during post-separation operations such as bead release. The release agent will fill the entire the channel and the uniform spreading of magnetic bound target particles will allow greater access to the magnetic bead bound target particles by the release agent.
The external magnet (or a system of magnets) that is variably positioned during capture of the magnetic particles may be driven by any of a number of different means, some of which will be described below. Further, the external magnet may be a permanent magnet or electromagnet, or multiples of either of these or combinations of permanent and electromagnets.
In accordance with some embodiments of this invention, the position of greatest magnetic field strength is gradually moved over the trapping region during the period of time when particles are flowing into the channel. The direction of movement of the magnetic field during trapping may be, in one embodiment, from a down stream position to an up stream position within the trapping region. In other words, the direction of movement of the magnetic field is opposite that of the direction of the fluid flow in the trapping region. Such embodiments may involve, for example, moving a permanent magnet in a direction from a downstream position to an upstream position underneath the base of a flow channel, particularly the region of the channel comprising the trapping region. Thus, as magnetic particles first enter the trapping region, the leading edge of the permanent magnet is positioned just beyond the downstream edge of the trapping region. Thereafter, as the magnetic particles begin to flow into the trapping region, the leading edge of the permanent magnet is gradually moved upstream and ultimately comes to rest at or near the upstream boundary of the trapping region. In certain embodiments, it reaches its position at about the time when the magnetic particles cease flowing into the trapping region.
In an alternative embodiment, the external magnet moves from the upstream to the downstream positions of the trapping region during capture of the magnetic particles. In other words, the external magnet moves in the same direction as the fluid flow. In this embodiment, as in the previously described embodiment, the duration of the movement of the external magnet should correspond, at least roughly, to the period of time during which magnetic particles are flowing through the trapping region. One specific embodiment employs a downstream movement of a magnet to sequentially capture and release and capture and release . . . the same particles in order to remove non-specifically bound sample species from the magnetic particles.
As indicated, control of the repositioning of the magnetic field within the trapping region can be accomplished by various mechanisms. In a first embodiment, this is accomplished by moving a magnetic field producer (e.g., a permanent magnet) over one surface of the trapping region (typically outside the channel) during the passage of magnetic particles through the trapping region. In another embodiment, the external magnet is an electromagnet which moves along the trapping region (same as the permanent magnet) during the flow of magnetic particles into the trapping region. Optionally, the position of the magnetic field produced by the electromagnet can be controlled by other means such as mechanically moving some or all of the electromagnet's coils during the trapping period.
In another embodiment, the dynamic repositioning of the magnetic field during trapping is accomplished by sequential insertion of a series of external magnets, each of relatively small size with respect of the size of the trapping region. In one embodiment, the magnets are permanent magnets. In a specific embodiment, these permanent magnets are arranged in alternating polarities (e.g., a first magnet has its south pole oriented toward the trapping region, a second magnet has its north pole oriented toward the trapping region, a third magnet has its south pole oriented toward the trapping region, a fourth magnet has its north pole oriented toward the trapping region, etc.).
Typically, in embodiments involving sequential insertion of the plurality of magnets, the magnets are arranged along the axial flow direction. In one example, the number of magnets is about 5 to 50. In a specific embodiment, about 20 separate permanent magnets are employed and arranged in alternating polarities, each having a width (dimension along the axial flow direction) of approximately 0.5 to 10 millimeters (e.g., 1.5 millimeters). More generally, the width of the individual permanent magnets is determined, at least in part, by the axial length of the trapping region and the number of magnets to be inserted.
In a typical embodiment, the first inserted magnet is the most downstream magnet and then progressively the upstream magnets are inserted during the course of the introduction of magnetic particles into the trapping chamber. In an alternative embodiment, the sequence of insertion can be reversed such that the first inserted magnet is the leading upstream position magnet, the second inserted magnet is the next successive downstream positioned magnet, etc.
Those of skill in the relevant art will understand that there are numerous other actuating mechanisms that could be used to mechanically, electrically, and/or electromechanically position magnets within the domain of a trapping region during fluid flow. Examples include solenoid drivers, electrical motors, pneumatic drives, hydraulic drivers, and the like.
The timing of the insertion of the external magnet(s) into the trapping region, in typically embodiments, corresponds at least roughly to the time period during which magnetic particles flow through the trapping region. In other words, the movement of the external magnet with respect to the trapping region may begin at about the same time that magnetic particles are introduced to the trapping region and end at about the same time when the last magnetic particles leave the trapping region. It may be useful to characterize this duration (the total time in which the magnetic particle bearing solution flows through the trapping region) as a “separation period.” Thus, in some embodiments, this period corresponds, at least roughly, to the period of time during which the external magnetic field is dynamically varied in the trapping region (e.g., the time during which external magnets are moved with respect to the trapping region). In other cases, however, the magnetic field will be fully developed in the trapping region for some time prior to the end of the separation period. In either case, the movement of the external magnetic field with respect to the trapping region may be smooth and continuous or stepped and discontinuous, as appropriate for the particular application.
Typically, the magnetic field when fully applied to the trapping region at the end of the separation period may be maintained for a further period of time to retain the magnetic particles in the trapping region for subsequent processing such as washing, release of captured target agent, etc.
Processing Trapped Species
In some embodiments, trapped species will be released from their associated magnetic particles in while confined to a trapping region. As mentioned, various mechanisms may be employed for this purpose. One approach involves applying a bead release agent to the trapped magnetic particles. Such agents may act by cleaving a chemical linker between the beads and the captured species or by competitively binding a linking species. Of course, other cleaving or release agents may be employed as will be understood by those of skill in the art.
Trapped target species may be simply concentrated, purified and/or released as described. Alternatively they can be further analyzed and/or treated.
While a magnetic field or other capturing stimulus is applied to the trap features 325, the particles flowing into trap 301 are captured. After a sufficient number of particles are captured (which might be indicated by simply running a sample stream through device 305 for a defined period of time), valves 317 and 319 are closed. Thereafter, in one embodiment, valves 321 and 323 are opened, and a buffer is passed from line 311, through trap 301, and out line 313. This serves to wash the captured particles. After washing for a sufficient length of time, the washed particles may be recovered by eluting (by e.g., removing an external magnetic or electrical field while the buffer continues to flow), by pipetting from trap 301, by removing a lid or cover on the trap or the entire device, etc. Regarding the last option, note that in some embodiments the devices are disposable and can be designed so that the top portion or a cover is easily removed by, e.g., peeling. In any of these cases, the species may be released from their magnetic particle labels prior to further processing by one or more the techniques described above.
In another embodiment, the particles that have been captured and washed and optionally released in the trap as described above are exposed to one or more markers (e.g., labeled antibodies) for target species in the sample. Certain tumor cells to be detected, for example, express two or more specific surface antigens. To detect these tumors, more than one marker may be used. This combination of antigens occurs only in very unique tumors. To detect the presence of such cells bound to magnetic particles, valves 317 and 323 may be closed and valve 321 opened after capture in trap 301 is complete. Then a first label is flowed into trap 301 via line 311 and out via line 309. Some of the label may bind to immobilized cells in trap 301. Thereafter, valve 321 is closed and valve 323 is opened and a second label enters trap 301 via line 313. After label flows through the trap for a sufficient length of time, the captured particles/cells may be washed as described above. Thereafter, the particles/cells can be removed from trap 301 for further analysis or they may be analyzed in situ. For example, the contents of trap 301 may be scanned with probe beams at excitation for the first and second labels if such labels or fluorophores for example. Emitted light is then detected at frequencies characteristic of the first and second labels. In certain embodiments, individual cells or particles are imaged to characterize the contents of trap 301 and thereby determine the presence (or quantity) of the target tumor cells. Of course various target components other than tumor cells may be detected. Examples include pathogens such as certain bacteria or viruses.
In another embodiment, nucleic acid from a sample enters trap 301 via line 307 and is captured by an appropriate mechanism (examples set forth below). Subsequently, valve 317 is closed and PCR reagents (nucleotides, polymerase, and primers in appropriate buffers) enter trap 101 via lines 311 and 313. Thereafter all valves (317, 319, 321, and 323) are closed and an appropriate PCR thermal cycling program is performed on trap 301. The thermal cycling continues until an appropriate level of amplification is achieved. Subsequently in situ detection of amplified target nucleic acid can be performed for, e.g., genotyping. Alternatively, the detection can be accomplished downstream of trap 301 in, e.g., a separate chamber which might contain a nucleic acid microarray or an electrophoresis medium. In another embodiment, real time PCR can be conducted in trap 301 by introducing, e.g., an appropriately labeled intercalation probe or donor-quencher probe for the target sequence. The probe could be introduced with the other PCR reagents (primers, polymerase, and nucleotides for example) via line 311 or 313. In situ real time PCR is appropriate for analyses in which expression levels are being analyzed. In either real time PCR or end point PCR, detection of amplified sequences can, in some embodiments, be performed in trap 301 by using appropriate detection apparatus such as a fluorescent microscope focused on regions of the trap.
For amplification reactions, the capture elements 325 capture and confine the nucleic acid sample to reaction chamber 301. Thereafter, the flow through line 307 is shut off and a lysing agent (e.g., a salt or detergent) is delivered to chamber 301 via, e.g., line 311 or 313. The lysing agent may be delivered in a plug of solution and allowed to diffuse throughout chamber 101, where it lyses the immobilized cells in due course. This allows the cellular genetic material to be extracted for subsequent amplification. In certain embodiments, the lysing agent may be delivered together with PCR reagents so that after a sufficient period of time has elapsed to allow the lying agent to lyse the cells and remove the nucleic acid, a thermal cycling program can be initiated and the target nucleic acid detected.
In other embodiments, sample nucleic acid is provided in a raw sample and coupled to magnetic particles containing appropriate hybridization sequences. The magnetic particles are then sorted and immobilized in trap 301. After PCR reagents are delivered to chamber 301 and all valves are closed, PCR can proceed via thermal cycling. During the initial temperature excursion, the captured sample nucleic acid is released from the magnetic particles.
The nucleic acid amplification technique described here is a polymerase chain reaction (PCR). However, in certain embodiments, non-PCR amplification techniques may be employed such as various isothermal nucleic acid amplification techniques; e.g., real-time strand displacement amplification (SDA), rolling-circle amplification (RCA) and multiple-displacement amplification (MDA). Each of these can be performed in a trap such as chamber 301 shown in
Example Magnetic Trapping Structures
Most fundamentally, a trapping station is defined by the boundaries of a region or channel in a fluidics device. Fluid flows through the trapping station and encounters a magnetic field generated by one or more external magnets proximate the trapping station. In addition, a trapping station may optionally employ a magnetic field gradient generator (MFGs). MFG elements (e.g., strips, pins, dots, grids, random arrangements, etc.) shape the external magnet field to produce a locally high magnetic field gradient in the trapping station.
Generally, the features or elements in these patterns may be made from various materials having permeabilities that are significantly different from that of the fluid medium in the device (e.g., the buffer). As indicated, the elements may be made from a ferromagnetic material. In a specific embodiment, the patterns are defined by nickel features on a glass or polymer substrate. In alternative embodiments, the MFG structures are combined with other types of capture structures such as electrodes, specific binding moieties (e.g., regions of nucleotide probes or antibodies), physical protrusions or indentations, etc.
Other types of MFG structures comprise ferromagnetic materials that do not form well-defined shapes or regular features. Instead, the structures form randomly placed features such as randomly dispersed powder, filings, granules, etc. These structures are affixed to one or more walls of the trapping station adhesives, pressure bonding, etc.
In an alternative embodiment, the trapping station contains no MFG structures. Instead, magnetic capture is based solely on the strength of the external magnetic field, without the aid of a field shaping element such as MFG structures.
Fluidics and Sorting Chamber Design
While some embodiments of this invention are implemented in micro-scale microfluidic systems, it should be understood that methods, apparatus, and systems of this invention are not limited to microfluidic systems. Typical sizes of larger trapping chambers range between about 1 and 100 millimeters in length (in the direction of flow), between about 1 and 100 millimeters in width and between about 1 micrometer and 10 millimeters depth (although typically about 1 millimeter or less). The depth and width together define the cross section through which fluid flows. The depth represents the dimension in the direction that the magnetic field penetrates into the channel, typically a direction pointed away from the position of the external magnet. In certain embodiments, the chambers have an aspect ratio (length to width) that is greater than 1, e.g., about 2 to 8.
In general, the applied magnetic field should be sufficiently great to capture or trap magnetic particles flowing in a fluid medium. Those of skill in the art will recognize that the applied magnetic force must be significantly greater than the hydrodynamic force exerted on the particles by the flowing fluid. This may limit the depth dimension of the trapping station.
In certain embodiments, the integrated fluidics systems are microfluidic systems. Microfluidic systems may be characterized by devices that have at least one “micro” channel. Such channels may have at least one cross-sectional dimension on the order of a millimeter or smaller (e.g., less than or equal to about 1 millimeter). Obviously for certain applications, this dimension may be adjusted; in some embodiments the at least one cross-sectional dimension is about 500 micrometers or less. In some embodiments, as applications permit, a cross-sectional dimension is about 100 micrometers or less (or even about 10 micrometers or less—sometimes even about 1 micrometer or less). A cross-sectional dimension is one that is generally perpendicular to the direction of centerline flow, although it should be understood that when encountering flow through elbows or other features that tend to change flow direction, the cross-sectional dimension in play need not be strictly perpendicular to flow. Often a micro-channel will have two or more cross-sectional dimensions such as the height and width of a rectangular cross-section or the major and minor axes of an elliptical cross-section. Either of these dimensions may be compared against sizes presented here. Note that micro-channels employed in this invention may have two dimensions that are grossly disproportionate—e.g., a rectangular cross-section having a height of about 100-200 micrometers and a width on the order or a centimeter or more. Of course, certain devices may employ channels in which the two or more axes are very similar or even identical in size (e.g., channels having a square or circular cross-section).
Often a controller will be employed to coordinate the operations of the various systems or sub-systems employed in the overall microfluidic system. Such controller will be designed or configured to direct the sample through a microfluidic flow passage. It may also control other features and actions of the system such as the strength and orientation of a magnetic field applied to fluid flowing through the microfluidic device, control of fluid flow conditions within the microfluidic device by actuating valves and other flow control mechanisms, mixing of magnetic particles and sample components in an attachment system, generating the sample (e.g., a library in a library generation system), and directing fluids from one system or device to another. The controller may include one or more processors and operate under the control of software and/or hardware instructions.
Integration
Examples of operational modules that may be integrated with magnetic trapping sorters in fluidics devices include (a) additional enrichment modules such as fluorescence activated cell sorters and washing modules, (b) reaction modules such as sample amplification (e.g., PCR) modules, restriction enzyme reaction modules, nucleic acid sequencing modules, target labeling modules, chromatin immunoprecipitation modules, crosslinking modules, and even cell culture modules, (c) detection modules such as microarrays of nucleic acids, antibodies or other highly specific binding agents, and fluorescent molecular recognition modules, and (d) lysis modules for lysing cells, disrupting viral protein coats, or otherwise releasing components of small living systems. Each of these modules may be provided before or after the magnetic sorter. There may be multiple identical or different types of operational modules integrated with a magnetic sorter in a single fluidics system. Further, one or more magnetic sorters may be arranged in parallel or series with respect to various other operational modules. Some of these operational modules may be designed or configured as traps in which target species in a sample are held stationary or generally constrained in particular volume.
As should be apparent from the above examples of modules, operations that may be performed on target and/or non-target species in modules of integrated fluidics devices include sorting, coupling to magnetic particles (sometimes referred to herein as “labeling”), binding, washing, trapping, amplifying, removing unwanted species, precipitating, cleaving, diluting, ligating, sequencing, synthesis, labeling (e.g., staining cells), cross-linking, culturing, detecting, imaging, quantifying, lysing, etc.
Specific examples of biochemical operations that may be performed in the magnetic sorting modules of integrated fluidic devices include synthesis, purification, and/or screening of plasmids, aptamers, proteins, and peptides; evaluating enzyme activity; and derivatizing proteins and carbohydrates. A broad spectrum of biochemical and electrophysiological assays may also be performed, including: (1) genomic analysis (sequencing, hybridization), PCR and/or other detection and amplification schemes for DNA, and RNA oligomers; (2) gene expression; (3) enzymatic activity assays; (4) receptor binding assays; and (5) ELISA assays. The foregoing assays may be performed in a variety of formats, such as: homogeneous, bead-based, and surface bound formats. Furthermore, devices as described herein may be utilized to perform continuous production of biomolecules using specified enzymes or catalysts, and production and delivery of biomolecules or molecules active in biological systems such as a therapeutic agents. Microfluidic devices as described herein may also be used to perform combinatorial syntheses of peptides, proteins, and DNA and RNA oligomers as currently performed in macrofluidic volumes.
One increasingly important example operation using the apparatuses and methods of the present invention is automated protein purification, particularly as protein is expressed in cell culture. Protein purification may be performed manually. However, the apparatuses and methods of the present invention provide a time and labor saving automation that delivers a high purity product with low cost.
In a prophetic example, desired proteins are expressed in organisms such as virus, bacteria, insect or mammalian cells. The expressed protein may be designed such that it may be selectively isolated from background materials. This may be accomplished via adding one or more selectable amino acid tags that add a stretch of amino acid to the protein. The tag may be a His tag, FLAG tag or other epitope-based tags (E-tags). The cells (for example) are introduced to one of the sample reservoirs described herein, with magnetic particles and lyses reagents in the same or one or more reservoirs. The magnetic particles may be magnetic beads coated with a high affinity media such as NTA-agarose or other resin containing to nickel. Mixing between the various sample reservoirs is promoted via one or more of the techniques described above, e.g., pneumatic, hydraulic, or magnetic mixing. The cells are disrupted by the lysing reagent and, under suitable conditions, the magnetic particles bind with the target protein in the lysate. The raw lysate is then flowed into the magnetic separation chamber where the beads become trapped on the surface of the channel. Wash buffer is added to elute the untagged and unbound protein and other cell fragments. According to various embodiments, the magnetic separation chamber may be agitated magnetically or through other means to further remove any unbound protein stuck between trapped particles. A highly stringent wash buffer may be used to further elute unwanted particles. At this point, only the target protein and bound magnetic particles remain in the chamber with very high selectivity. The target protein may be released by using a bead release agent into a small volume, optionally for further processing. Lastly, the magnetic particles may be released. Because these various operations occur on a unitary or disposable cartridge in a machine, the procedure may be preprogrammed and automated to save time and cost. This configuration may be used to selectively trap other nucleic acid related products, such as RNA, which may be so labeled so as to be similarly selectable.
The present fluidic sorting devices may be integrated such that they are configured for particular purposes. For example, one may desire to have one mixing reservoir and several trapping stations. In this way, a single sample is deployed and mixed with magnetic particles (for example), such that selected targets are labeled. This single sample is routed to greater than one, or a plurality of trapping stations. The trapping stations may be configured in parallel or in series. Optionally, one or more aspects of this parallel-trapping station configuration may be under the control of a single controller for mixing, disposing on the trapping station, and eluting (such that the labeled target species are maintained in the trapping station, for example). When connected in series, target species concentration may be improved by sequential trapping to remove any incidental non-specific binding. In addition, a series trapping configuration may be used when two or more markers are required to for certain target cells, such as tumor cells. In that case, one trapping station may isolate cells having one marker (such as a first cell surface receptor) and then the selected cells may be washed so as to remove the magnetic particle (for example). The population of selected cells may be then mixed with markers for another target, such as a second cell surface receptor. The cells so labeled for this second cell surface receptor may then be trapped. After eluting (for example) the non-trapped cells, the final population will be those cells that display both the first and second cell surface receptors. This process may be repeated to collect further subpopulations. Alternatively, one may desire to remove certain targets, such as subpopulations having a first receptor but not a second cell surface receptor, for example. This process may be repeated, and the present devices may be configured, to facilitate a variety of multiple-target trapping iterations Analogous methods and device configurations may be used for selecting subpopulations of a variety of target molecules in a sample including but not limited to cell surface receptors, molecular moieties, or other types of selectable targets
Examples of Reactors and Lysis Modules in Fluidics Systems
Various features may be employed in a microfluidic reactor employed in an integrated device of this invention. The exact design and configuration will depend on the type of reaction: thermal management system, micromixers, catalyst structures and a sensing system. In certain embodiments, a thermal management system includes heaters, temperature sensors and heat transfer (micro heat exchanges). In microreactors, all components can be integrated in resulting in a very precise control of temperatures which is crucial for instance in PCR for DNA amplification.
Micromixers may be used for mixing two solutions (e.g. a sample and a reagent) to make the reaction possible. In microscale systems, mixing often relies on diffusion due to the laminar behavior of fluid at low Reynolds numbers. In one embodiment, a hydrophobic material defining a hole separates two adjacent chambers. When aqueous solutions are used, the hydrophobicity of the interface permits both chambers to be filled with fluid plugs without mixing. A pressure gradient can then be applied to force fluid through the hole in the hydrophobic layer to induce diffusion between the two plugs. In one embodiment, the hole is actually a slit in which no material is removed from the intermediate dividing layer.
Catalyst structures may be employed to accelerate a chemical reaction (e.g., cross-linking or sequencing). In microreactors, the catalyst can be implemented in the form of, e.g., fixed beads, wires, thin films or a porous surface. While beads and wires and not compatible with batch fabrication, thin films and porous surface catalysts can be integrated in the fabrication of microreactors.
A sensing system may employ chemical microsensors or biosensors, for example. Designing a microreactor with glass or plastic provides optical access to the reaction chamber and thus, all optical measurement methods.
Before the contents of a biological cell may be analyzed, the cells to be analyzed are made to burst so that the components of the cell can be separated. The methods of cell disruption used to release the biological molecules in a cell and in a virus include, e.g., electric field, enzyme, sonication, and using a detergent. Mechanical forces may also be used to shear and burst cell walls.
Cell lysis may be performed by subjecting the cells trapped in a reaction chamber to pulses of high electric field strength, typically in the range of about 1 kV/cm to 10 kV/cm. The use of enzymatic methods to remove cell walls is well-established for preparing cells for disruption, or for preparation of protoplasts (cells without cell walls, as in plant cells, for example) for other uses such as introducing cloned DNA or subcellular organelle isolation. The enzymes are generally commercially available and, in most cases, were originally isolated from biological sources (e.g. snail gut for yeast or lysozyme from hen egg white). The enzymes commonly used include lysozyme, lysostaphin, zymolase, cellulase, mutanolysin, glycanases, proteases, mannase etc. In accordance with various embodiments, the cell lysis enzyme may be added to the trapping chamber from a separate reservoir or be mixed with the sample in the beginning.
In addition to potential problems with the enzyme stability, the susceptibility of the cells to the enzyme can be dependent on the state of the cells. For example, yeast cells grown to maximum density (stationary phase) possess cell walls that are notoriously difficult to remove whereas midlog growth phase cells are much more susceptible to enzymatic removal of the cell wall. If an enzyme is used, it may have to be sorted and removed from the desired material before further analysis.
Sonication uses a high-frequency wave that mechanically burse the cell walls. Ultrasound at typically 20-50 kHz is applied to the sample via a metal probe that oscillates with high frequency. The probe is placed into the cell-containing sample and the high-frequency oscillation causes a localized high pressure region resulting in cavitation and impaction, ultimately breaking open the cells. Cell disruption is available in smaller samples (including multiple samples under 200 μL in microplate wells) and with an increased ability to control ultrasonication parameters. The present invention may be used with a thermal management system as described above such that the sample is kept in cool conditions, for example, to avoid undue heat due to sonication, where the heat may denature the desired protein.
Detergent-based cell lysis is an alternative to physical disruption of cell membranes, although it is sometimes used in conjunction with homogenization and mechanical grinding. Detergents disrupt the lipid barrier surrounding cells by disrupting lipid:lipid, lipid:protein and protein:protein interactions. The ideal detergent for cell lysis depends on cell type and source and on the downstream applications following cell lysis. Animal cells, bacteria and yeast all have differing requirements for optimal lysis due to the presence or absence of a cell wall. Because of the dense and complex nature of animal tissues, they require both detergent and mechanical lysis to effectively lyse cells.
In general, nonionic and zwitterionic detergents are milder, resulting in less protein denaturation upon cell lysis, than ionic detergents and are used to disrupt cells when it is critical to maintain protein function or interactions. CHAPS, a zwitterionic detergent, and the Triton X series of nonionic detergents are commonly used for these purposes. In contrast, ionic detergents are strong solubilizing agents and tend to denature proteins, thereby destroying protein activity and function. SDS, and ionic detergent that binds to and denatures proteins, is used extensively for studies assessing protein levels by gel electrophoresis and western blotting. If protein purification is desired, and the cells have partitioned the protein into sub-cellular membrane bound moieties, such as inclusion bodies, other detergents, such as the commercially available TWEEN may be used as an additional reagent to disrupt such inclusion bodies.
A mechanical method for cell disruption uses glass or ceramic beads and a high level of agitation to shear and burst cell walls. This process works for easily disrupted cells, is inexpensive, but has integration issues for the micorfluidic device. In one embodiment, beads are used in a closed chamber holding the sample and are agitated with an electric motor. In other embodiments, high pressure is applied to fluid containing the cell samples while forcing the fluid to flow through a very narrow channel. Shear between the cell and channel walls under such conditions would disrupt the cell.
Examples of Detectors in Integrated Flow Systems
In various applications envisaged for integrated microsystems it will be necessary to quantify the material present in a channel at one or more positions similar to conventional laboratory measurement processes. Techniques typically utilized for quantification include, but are not limited to, optical absorbance, refractive index changes, fluorescence emission, chemiluminescence, various forms of Raman spectroscopy, electrical conductometric measurements, impedance measurements (e.g., impedance cytometry) electrochemical amperiometric measurements, acoustic wave propagation measurements.
Optical absorbance measurements are commonly employed with conventional laboratory analysis systems because of the generality of the phenomenon in the UV portion of the electromagnetic spectrum. Optical absorbance is commonly determined by measuring the attenuation of impinging optical power as it passes through a known length of material to be quantified. Alternative approaches are possible with laser technology including photo acoustic and photo thermal techniques. Such measurements can be utilized with the integrated fluidics devices discussed here with the additional advantage of potentially integrating optical wave guides on microfabricated devices. The use of solid-state optical sources such as LEDs and diode lasers with and without frequency conversion elements would be attractive for reduction of system size.
Refractive index detectors have also been commonly used for quantification of flowing stream chemical analysis systems because of generality of the phenomenon but have typically been less sensitive than optical absorption. Laser based implementations of refractive index detection could provide adequate sensitivity in some situations and have advantages of simplicity. Fluorescence emission (or fluorescence detection) is an extremely sensitive detection technique and is commonly employed for the analysis of biological materials. This approach to detection has much relevance to miniature chemical analysis and synthesis devices because of the sensitivity of the technique and the small volumes that can be manipulated and analyzed (volumes in the picoliter range are feasible). For example, a 100 pL sample volume with 1 nM concentration of analyte would have only 60,000 analyte molecules to be processed and detected. There are several demonstrations in the literature of detecting a single molecule in solution by fluorescence detection. A laser source is often used as the excitation source for ultrasensitive measurements but conventional light sources such as rare gas discharge lamps and light emitting diodes (LEDs) are also used. The fluorescence emission can be detected by a photomultiplier tube, photodiode or other light sensor. An array detector such as a charge coupled device (CCD) detector can be used to image an analyte spatial distribution.
Raman spectroscopy can be used as a detection method for microfluidic devices with the advantage of gaining molecular vibrational information, but with the disadvantage of relatively poor sensitivity. Sensitivity has been increased through surface enhanced Raman spectroscopy (SERS) effects but only at the research level. Electrical or electrochemical detection approaches are also of particular interest for implementation on microfluidic devices due to the ease of integration onto a microfabricated structure and the potentially high sensitivity that can be attained. The most general approach to electrical quantification is a conductometric measurement, i.e., a measurement of the conductivity of an ionic sample. The presence of an ionized analyte can correspondingly increase the conductivity of a fluid and thus allow quantification. Amperiometric measurements imply the measurement of the current through an electrode at a given electrical potential due to the reduction or oxidation of a molecule at the electrode. Some selectivity can be obtained by controlling the potential of the electrode but it is minimal. Amperiometric detection is a less general technique than conductivity because not all molecules can be reduced or oxidized within the limited potentials that can be used with common solvents. Sensitivities in the 1 nM range have been demonstrated in small volumes (10 nL). The other advantage of this technique is that the number of electrons measured (through the current) is equal to the number of molecules present. The electrodes required for either of these detection methods can be included on a microfabricated device through a photolithographic patterning and metal deposition process. Electrodes could also be used to initiate a chemiluminescence detection process, i.e., an excited state molecule is generated via an odixation-reduction process which then transfers its energy to an analyte molecule, subsequently emitting a photon that is detected.
Acoustic measurements can also be used for quantification of materials but have not been widely used to date. One method that has been used primarily for gas phase detection is the attenuation or phase shift of a surface acoustic wave (SAW). Adsorption of material to the surface of a substrate where a SAW is propagating affects the propagation characteristics and allows a concentration determination. Selective sorbents on the surface of the SAW device are often used. Similar techniques may be useful in the devices described herein.
The mixing capabilities of the microfluidic systems lend themselves to detection processes that include the addition of one or more reagents. Derivatization reactions are commonly used in biochemical assays. For example, amino acids, peptides and proteins are commonly labeled with dansylating reagents or o-phthaldialdehyde to produce fluorescent molecules that are easily detectable. Alternatively, an enzyme could be used as a labeling molecule and reagents, including substrate, could be added to provide an enzyme amplified detection scheme, i.e., the enzyme produces a detectable product. There are many examples where such an approach has been used in conventional laboratory procedures to enhance detection, either by absorbance or fluorescence. A third example of a detection method that could benefit from integrated mixing methods is chemiluminescence detection. In these types of detection scenarios, a reagent and a catalyst are mixed with an appropriate target molecule to produce an excited state molecule that emits a detectable photon.
This application claims priority under U.S.C. §119 to provisional application 61/124,565, titled “MAGNETIC CELL SORTING SYSTEM WITH MIXING MODULES,” filed on Apr. 16, 2008, the disclosure of which is incorporated herein in its entirety for all purposes.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/US09/40866 | 4/16/2009 | WO | 00 | 2/11/2011 |
Number | Date | Country | |
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Parent | 61124565 | Apr 2008 | US |
Child | 12937983 | US |