The invention relates to centrifugal processing systems and apparatus.
Today blood collection organizations routinely separate whole blood by centrifugation into its various therapeutic components, such as red blood cells, platelets, and plasma.
Conventional blood processing systems and methods use durable centrifuge equipment in association with single use, sterile processing chambers, typically made of plastic. The centrifuge equipment introduces whole blood into these chambers while rotating them to create a centrifugal field.
Whole blood separates within the rotating chamber under the influence of the centrifugal field into higher density red blood cells and platelet-rich plasma. An intermediate layer of white blood cells and lymphocytes forms an interface between the red blood cells and platelet-rich plasma.
Conventional blood processing methods use durable centrifuge equipment in association with single use, sterile processing systems, typically made of plastic. The operator loads the disposable systems upon the centrifuge before processing and removes them afterwards.
Conventional centrifuges often do not permit easy access to the areas where the disposable systems reside during use. As a result, loading and unloading operations can be time consuming and tedious.
Disposable systems are often preformed into desired shapes to simplify the loading and unloading process. However, this approach is often counterproductive, as it increases the cost of the disposables.
The invention provides improved blood processing systems and methods that create unique dynamic flow conditions within a compact, easily handled processing chamber.
One aspect of the invention provides systems and methods for centrifugally separating whole blood into red blood cells, plasma, and a platelet concentrate. The systems and methods rotate a first rotating separation zone about a rotational axis. The first rotating separation zone has radially spaced apart walls with a high-G side and a low-G side located closer to the rotational axis than the high-G side. A blood flow path in the first rotating separation zone extends circumferentially about the rotation axis. The first rotating separation zone includes an entry region where whole blood enters the first rotating separation zone to begin separation. The first rotating separation zone also includes a terminal wall that is circumferentially spaced from the entry region, where separation is halted.
The systems and methods direct whole blood into the first rotating separation zone through a first path adjacent the entry region, to begin separation of the whole blood into red blood cells toward the high-G side and plasma constituent carrying platelets toward the low-G side. The systems and methods direct red blood cells separated in the first rotating separation zone in a first circumferential flow direction toward the terminal wall. The systems and methods halt blood flow in the first circumferential flow direction at the terminal wall. The systems and methods successively increase surface hematocrit in the first rotating separation zone in the first circumferential flow direction by separating the plasma constituent from the red blood cells. The systems and methods direct separated red blood cells from the first rotating separation zone through a second path adjacent the terminal wall, where the surface hematocrit in the first rotating separation zone is the most. The systems and methods direct plasma constituent separated in the first rotating separation zone in a second circumferential flow direction opposite to the first circumferential flow direction toward a different region in the first rotating separation zone that is circumferentially spaced away from the terminal wall, where the surface hematocrit in the first rotating separation zone is the least. The systems and methods separate the plasma constituent into platelet concentrate and plasma in a second rotating separation zone.
The invention may be embodied in several forms without departing from its spirit or essential characteristics. The scope of the invention is defined in the appended claims, rather than in the specific description preceding them. All embodiments that fall within the meaning and range of equivalency of the claims are therefore intended to be embraced by the claims.
FIGS. 25A/B/C are enlarged perspective views of an interior ramp used in association with either one of the blood processing assemblies shown in FIGS. 16/17 or 18/19 for controlling flow of PRP from the chosen assembly;
FIGS. 33A/B/C are a series of diagrammatic views showing the operation of the interface control system shown in
FIGS. 34A/B are flow charts showing the operation of the interface control circuit associated with the interface control system shown in
FIGS. 35A/B show, respectively, the platelet counts and mean platelet volumes sampled during a 45 minute procedure using a separation chamber that embodies the features of the invention; and
FIGS. 36A/B show, respectively, the platelet counts and mean platelet volumes sampled during a 45 minute procedure using another separation chamber than embodies the features of the invention.
A. Single Stage Whole Blood Separation Systems
In use, the system separates whole blood within the chamber 10 into red blood cells (RBC) and plasma rich in platelets (called platelet-rich plasma, or PRP). This specification and drawings will identify red blood cells as RBC; platelet-rich plasma as PRP; and whole blood as WB.
The system includes a holder 12 that rotates the chamber 10 about an axis 14 (see FIG. 2), to thereby create a centrifugal field within the chamber 10. The centrifugal field extends from the rotational axis 14 radially through the chamber 10.
As
While rotating, the chamber 10 receives WB through a first port 20. The WB follows an axial flow path in the chamber 10. That is, it flows in a path that is generally parallel to the rotational axis 14 (as
In the geometry shown in
WB separates within the chamber 10 under the influence of the centrifugal field into RBC and PRP. As
An intermediate layer called the interface 26 forms between the RBC and PRP. The interface 26 constitutes the transition between the formed cellular blood components and the liquid plasma component. Large amounts of white blood cells and lymphocytes populate the interface 26.
Platelets, too, can leave the PRP and settle on the interface 26. This settling action occurs when the radial velocity of the plasma near the interface 26 is not enough to keep the platelets suspended in the PRP. Lacking sufficient radial flow of plasma, the platelets fall back and settle on the interface 26.
One aspect of the invention establishes flow conditions within the chamber 10 to “elute” platelets from the interface 26. The elution lifts platelets from the interface 26 and into suspension in the PRP.
To establish beneficial elution conditions within the chamber 10, the PRP collection port 24 and the WB inlet port 20 are juxtaposed so that the PRP exits the chamber 10 in the same region where WB enters the chamber 10.
The illustrated embodiment, as shown in
The invention also arranges the RBC collection port 22 and the PRP collection port 24 so that PRP exits the chamber 10 in a region opposite to the region where RBC exit the chamber 10, relative to the axial flow of WB in the chamber 10.
The illustrated embodiment, as
It should be appreciated that the centrifugal field is not sensitive to “top” and “bottom” port placement. The particular “top edge” and “bottom edge” relationship of the ports 20; 22; and 24 shown in
The chamber 10 shown in
In the prior chamber 10A shown in
In the prior chamber 10B shown in
To further enhance the platelet elution conditions within the chamber 10, the distance between the low-G wall 16 and the interface 26 is preferably smaller in the region of the RBC collection port 22 than in the region of the PRP collection port 24. The illustrated embodiment (see
The same result can be obtained without continuously or uniformly tapering the low-G wall 16 along the entire length of the axial flow path between the PRP collection port 24 and the RBC collection port 22. The low-G wall 16 can begin its taper farther away from the PRP collection port 24 than
The axial flow processing chamber 10 configured according to this aspect of the invention serves to increase platelet yields due to the interplay of two principal dynamic flow conditions, one radial and the other axial in direction.
First, due to the juxtaposition of the WB inlet port 20 and the PRP collection port 24, the chamber 10 produces a dynamic radial plasma flow condition near the PRP collection port 24. The radial flow condition is generally aligned along the centrifugal force field. The radial plasma flow condition continuously elutes platelets off the interface 26 into the PRP flow next to the PRP collection port 24.
Second, by narrowing the gap between the low-G wall 16 and the interface 26 next to the RBC collection port 22, compared to the gap next to the PRP collection port 24, the chamber 10 produces a dynamic axial plasma flow condition between the two ports 22 and 24. The axial flow condition is generally transverse the centrifugal force field. The axial plasma flow condition continuously drags the interface 26 back towards the PRP collection port 24, where the higher radial plasma flow conditions exist to sweep the platelets off the interface 26.
WB enters the chamber 10 at a given entry hematocrit, which indicates the volume of RBC per unit volume of WB. A typical healthy donor has a predonation hematocrit of about 42.5%.
The hematocrit of the blood lying on the boundary between the RBC and plasma along the interface 26 (called the surface hematocrit) remains at or substantially the same as the entry hematocrit in the entry region Re of the chamber 10 near the WB inlet port 20.
The size of the entry region Re varies according to the hematocrit of the blood entering the chamber 10. For a given chamber configuration, the lower the entry hematocrit is, the smaller the entry region Re becomes.
The size of the entry region Re also depends upon the strength of the centrifugal field within the chamber and the surface area of the chamber.
As
Further details of the distribution of RBC during centrifugation in a chamber are set forth in Brown, “The Physics of Continuous Flow Centrifugal Cell Separation,” Artificial Organs, 13(1):4-20 (1989), from which
As
This, in turn, increases the radial velocity at which plasma is displaced by the separating RBC mass in response to the centrifugal force field. As the RBC mass moves toward the high-G wall 18, the plasma is displaced in a radial flow path toward the low-G wall 16. As a result, relatively large radial plasma velocities occur in the entry region Re.
These large radial velocities toward the low-G wall 16 elute large numbers of platelets from the RBC mass. As a result, fewer platelets remain entrapped on the interface 26 here than elsewhere in the chamber 10.
The purposeful arrangement of the ports 20; 22; and 24 in the separation chamber 10 also contributes to further enhanced elution of platelets. The WB inlet port 20 is diametrically spaced from the RBC collection port 22, but the WB inlet port 20 is alongside the PRP collection port 24. This isolation between the WB inlet port 20 and the RBC collection port 22 forces the RBC to traverse the entire axial length of the chamber 10 during processing. This maximizes its exposure to the centrifugal force field.
The isolation between the RBC collection port 22 and the PRP collection port 24 directs the RBC toward the RBC collection port 22. At the same time, it directs the PRP stream in the opposite direction toward the PRP collection port 24.
Furthermore, due to the displaced low-G wall 16, the distance between the low-G wall 16 and the interface 26 increases between the region of the RBC collection port 22 and the PRP collection port 24. As a result, the plasma layer along the interface 26 increases in radial depth in the intended direction of PRP flow, i.e., away from the RBC collection port 22 and toward the axially spaced PRP collection port 24. The plasma near the RBC collection port 22 is closer to the high-G centrifugation field than the plasma near the PRP collection port 24.
This shift in the relative position of the plasma between the two ports 22 and 24 causes the lighter plasma to move along the interface 26. The plasma moves swiftly away from the relatively more confined region closer to the high-G field (i.e., next to the RBC collection port 22), toward the relatively more open region closer to the low-G field (i.e., next to the PRP collection port 24).
This swiftly moving axial plasma flow actually drags the interface 26—and platelets entrapped within in—continuously toward the PRP collection port 24. There, the radial plasma velocities are the greatest to supply the greatest elution effect, lifting the entrapped platelets free of the interface 26 and into the PRP stream for collection through the port 24.
The close juxtaposition of the WB inlet port 20 and the PRP collection port 24 will alone result in improved platelet elutriation in the chamber 10, without altering the radial position of the low-G wall 16 relative to the interface 26. The enhanced radial flow conditions will alone keep the majority of the platelet population in suspensions in the PRP for collection.
The remaining minority of the platelet population constitutes platelets that are physically larger. These larger platelets typically occupy over 15×10−15 liter per platelet (femtoliters, or cubic microns), and some are larger than 30 femtoliters. In comparison, most platelets average about 8 to 10 femtoliters (the smallest of red blood cells begin at about 30 femtoliters).
These larger platelets settle upon the interface 26 quicker than most platelets. These larger platelets are most likely to become entrapped in the interface 26 near the RBC collection port 22.
The axial plasma flow conditions established along the interface 26 by the displaced low-G wall 16 moves these larger, faster settling platelets with the interface 26. The axial plasma flow moves the larger platelets toward the PRP collection port 24 into the region of high radial plasma flow. The high radial plasma flow lifts the larger platelets from the interface 26 for collection.
The complementary flow conditions continuously lift platelets of all sizes from the interface 26 next to the PRP collection port 24. They work to free platelets of all sizes from the interface 26 and to keep the freed platelets in suspension within the PRP.
Simultaneously (as
As a result, the PRP exiting the PRP collection port 24 carries a high concentration of platelets and is substantially free of the other blood components.
B. Two Stage Separation Systems
As
In use, the container 31A constitutes an axial flow chamber in which RBC and PRP are separated from whole blood in a first processing stage. The container 31A embodies the features of the axial flow chamber 10, as previously described.
In use, the container 31B constitutes an axial flow chamber in which the PRP is further separated into platelet concentrate and platelet-depleted plasma (also called platelet-poor plasma) in a second processing stage. The specification and drawings will refer to platelet concentrate as PC and platelet-poor plasma as PPP. The container 31B embodies other aspects of the invention, which will be described in greater detail later.
In this configuration, the assembly 28 can be used in association with a commercially available blood processing centrifuge, like the CS-3000® Blood Separation Centrifuge made and sold by the Fenwal Division of Baxter Healthcare Corporation (a wholly owned subsidiary of the assignee of the present invention).
As
As FIGS. 6A/B show, each holder 32A/32B can be pivoted opened to receive its separation container 31A/31B. Each holder 32A/32B can then be pivoted closed (as
In conventional use, the rotor 30 rotates (typically at about 1600 RPM), subjecting the holders 32A/32B and their entrapped separation containers 31A/31B to a centrifugal force field. Typically, the centrifugal force is field is about 375 G's along the high-g wall of the assembly 28.
As
PRP is conveyed from the first container 31A into the second stage container 31B. The second container 31B receives PRP through the port 35 for centrifugal separation into PC and PPP. The port 37 conveys PPP from the container 31B, leaving the PC behind within the container 31B for collection. A normally closed outlet port 39 is provided to later convey the PC from the container 31B.
As
The pump P2 pulls PRP away from the container 31A, until the detector 33 senses the presence of RBC. This indicates that the boundary between the RBC and the plasma has “spilled” past the detector 33. The pump P2 then pumps back toward the first container 31A until the sensed “spill-over” clears the interface detector 33. The pump P2 then reverses again to pull PRP away from the container 31A until the detector 33 senses another “spill-over.” This process repeats itself.
Employing the well-known Cullis seal-less centrifuge principle, a non-rotating (zero omega) holder (not shown) holds the upper portion of the umbilicus 29 in a non-rotating position above the rotor. The holder 40 (see
This relative rotation of the umbilicus 29 and the rotor 30 keeps the umbilicus 29 untwisted, in this way avoiding the need for rotating seals.
Each separation container 31A and 31B conforms to the interior configuration defined by its respective holder 32A and 32B, when closed.
1. First Stage Separation Chamber
More particularly, as
When closed, the holder 32A sandwiches the flexible separation container 31A between the high-G surface 44 and the surface of the low-G surface 46 (as
As
When filled with blood during processing, the peripherally sealed region of the container 31A expands against the high-g surface 44 and the facing low-g surface of the pressure plate 46, assuming their prescribed contours.
As
As
When the holder 32A is closed, mating regions 52A; 54A; and 56A on the low-G pressure plate 46 (see
In the illustrated embodiment, the low-G pressure plate surface 46 preferably tapers outward toward the high-G surface at a slope of about 0.25 degree.
When closed, the holder 32A thereby shapes the peripherally sealed region of the container 31A to establish an axial flow processing chamber 10 like that shown in
In use, the first stage separation chamber 32B preferably presents an effective collection area of between about 70 to about 120 cm2, with an associated processing volume of between about 45 ml to about 100 ml.
2. The Second Stage Separation Chamber
As
Like the holder 32A, the high-G surface 51 of the holder 32B includes a recessed region 57 from which a pattern of raised sealing surfaces 59 project (see FIGS. 6B and 10A).
Like the holder 32A, when the holder 32B is closed, the pressure plate low-G surface 53 presses against the sealing surfaces 59. This crimps the walls of the separation container 31B closed along the sealing surfaces 59. The interior configuration of the second stage axial flow separation chamber 61 is thereby formed, as
As
The raised sealing surfaces 59 also establish an interior wall 63 that separates the first and second regions R1 and R2. The wall 63 stretches into the chamber 61, extending in the same direction as the axial flow path. The wall 63 terminates within the chamber 61 to form a passage 65 linking the two regions R1 and R2. It should be appreciated that position of the wall 63 within the chamber 61 can vary. It can be closer to the PRP inlet port 35 than shown in
As just described, the configuration of the second stage chamber 61 is like that shown in
A chamber like that shown in
The prior A-35 Chamber typically has a collection area of about 160 cm2 for separating PRP into PC and PPP. When used for this purpose, this chamber typically presents a radial thickness (or depth) on the order of about 1.4 cm. The chamber thereby has a processing volume of about 200 mL.
Conventional wisdom believed that the processing volume for second stage platelet separation chamber should exceed the processing volume of the first stage separation chamber.
The larger processing volume was believed to be beneficial, because it gave the platelets more time to separate (or “sediment”) from the PRP within the chamber. Conventional wisdom also believed that the larger desired processing volume in the second stage chamber would subject the platelets to less damage or activation due to shear stress during processing (see, e.g., column 10, lines 26 to 39 of the Cullis et al. '172 Patent).
According to the present invention, the axial flow processing chamber 61 shown in
In one operative embodiment, the chamber 61 configured according to the invention presents the same collection area as the prior A-35 Chamber (i.e., about 160 cm2), but has a maximum radial (or channel) depth of only 2 mm. In this operative embodiment, the chamber 61 presents a processing volume of just 30 mL, compared to the 200 mL processing volume typical for the prior A-35 Chamber.
Surprisingly, despite its considerably smaller processing volume and radial depth, the following Example demonstrates that the chamber 61 provides a significant increase in platelet collection efficiencies, compared to the prior A-35 Chamber.
A study compared the conventional 200 ml A-35 chamber to the 30 ml, reduced depth chamber described above (which will be called the “30 ml Chamber”). Both chambers had a collection area of 160 cm2.
The study used a paired run protocol. During the protocol, 59 normal donors underwent a platelet collection procedure with the A-35 chamber. The same donors underwent another platelet collection procedure with the 30 ml Chamber. The order of the collection procedures was randomized among the donors, with the procedures performed about a month apart.
Both procedures were conducted on a CS-3000® Centrifuge operated at a speed of 1600 RPM. All operating parameters for the first procedure were repeated in the second procedure. Six different blood centers participated in the study.
The results were correlated and statistically verified.
The study showed that the 30 ml Chamber provided significantly improved platelet collection. Compared to the A-35 Chamber, the 30 ml Chamber showed a 13.3% increase in platelet yield (p<0.0001), which represents a significant increase in the net number of platelets collected during a given procedure.
Compared to the A-35 Chamber, the 30 ml Chamber provided increased platelet yields without damage or activation of the platelets. The platelet concentrate collected using the 30 ml Chamber could be filtered immediately after resuspension, without platelet loss. On the other hand, platelet concentrate collected using the A-35 Chamber required a rest period of at least 2 hours before it could be filtered without incurring a significant loss in platelet count.
Using the conventional dimensionless Reynolds Number (Re) as a point of comparison, one would conclude that the nature of the fluid flow in the A-35 Chamber and the 30 ml Chamber are virtually identical. The A-35 has a Re of 2.9, and the 30 ml Chamber has a Re of 7, which are not significantly different values.
One aspect of the invention provides a new dimensionless parameter (λ) that more accurately characterizes the combined attributes of angular velocity, channel thickness, kinematic viscosity, and axial height of the platelet separation chamber 61. The new parameter (λ) is expressed as follows:
where:
As Table 1 shows, the parameter (λ) value clearly characterizes and differentiates the unique nature and domain of the flow regime established within the chamber 61 (referred to as the “New” chamber), compared to the conventional A-35 chamber.
As Table 1 shows, the parameter (λ) value for the prior A-35 Chamber is 5109. The parameter (λ) value for the chamber that embodies the features of the invention is only 14, less than 1% of the prior chamber.
According to this aspect of the invention, a parameter (λ) value for a chamber that is less than about 700 will produce significantly greater platelet yields. As the parameter (λ) value of a given chamber increasingly exceeds about 700, the chamber produces flow conditions that lead to greater overall shear stress during processing (leading to platelet activation) and to greater Coriolis-effect swirling (which limits the effective surface area available for platelet perfusion).
The new parameter (λ) value expresses for a given rotating frame of reference what the magnitude of Coriolis-effect swirling and shear stress will be. The parameter (λ) value has the same meaning whether the flow within the chamber is axial (i.e., along the axis of rotation) or circumferential (i.e., about the axis of rotation). Regardless of the direction of flow with respect to the rotational axis, the lower the absolute parameter (λ) value is for a given system, the lower will be the expected magnitude of Coriolis-effect swirling in the system.
The chamber 61 has a parameter (λ) value that is less than about 700, it is better perfused during processing and subjects the platelets to less shear stress, even at dramatically reduced chamber depths (i.e. radial thickness).
The aspects of the invention previously described in the context of an axial flow blood separation chamber can also be employed in providing a circumferential flow blood processing chamber with enhanced platelet separation efficiencies.
In use, the chamber 58 rotates on a rotor 60 about an axis 62 (see FIG. 12), to thereby create a centrifugal field within the chamber 58. Just as with the axial flow chamber 10 shown in
While rotating, the chamber 58 receives WB through a first port 68. The WB follows a circumferential flow path in the chamber 58; that is, it flows in a circumferential path about the rotational axis 62 (as
In this geometry, the transverse top and bottom edges of the chamber 58 (which lie along the circumferential flow path) are usually longer than the longitudinal side edges (which lie across the circumferential flow path). The circumferential flow chamber 58 usually forms the shape of a tube that is elongated in the direction of rotation. Still, other configurations defining a circumferential flow path can be used.
WB separates within the tubular chamber 58 under the influence of the centrifugal field into RBC and PRP. As
According to the invention, the PRP collection port 72 and the WB inlet port 68 are juxtaposed so that the PRP exits the circumferential flow chamber 58 in the same region where WB enters the chamber 58. In the illustrated embodiment, as shown in
Also according to the invention, the RBC collection port 70 and the PRP collection port 72 are arranged so that PRP exits the chamber 58 in a region opposite to the region where RBC exit the chamber 58, relative to the circumferential flow of WB in the chamber 58. In the illustrated embodiment, as
The chamber 58 shown in
In the prior circumferential flow chamber 58A shown in
In the prior circumferential flow chamber 58B shown in
In both the
As
The WB inlet port 68 is oppositely spaced from the RBC collection port 70 (in the circumferential flow direction), forcing the RBC to traverse the entire axial length of the chamber 58, thereby maximizing their exposure to the centrifugal separation forces. The isolation between the RBC collection port 70 and the PRP collection port 72 also directs the RBC toward the RBC collection port 70, while directing the PRP stream in the opposite direction toward the PRP collection port 72.
Like the chamber 10 shown in
As previously described with reference to
As
The circumferential flow chamber 58 that embodies the invention can be variously constructed.
Either assembly 74 or 76 can be used in association with a blood processing centrifuge 78, like that shown in
As
When upright, the bowl and spool elements 80 and 82 are presented for access by the user. A mechanism permits the spool and bowl elements 80 and 82 to assume a mutually separated position, as
The mechanism also permits the spool and bowl elements 80 and 82 to assume a mutually cooperating position, as
When closed, the spool and bowl elements 80 and 82 can be pivoted as an assembly into a suspended position, as
In the illustrated embodiments, each circumferential flow chamber assembly 74 and 76 provides multi-stage processing. A first stage separates RBC and PRP from WB. A second stage separates PC and PPP from the PRP.
While the interior of either circumferential flow chamber assembly 74 or 76 can be variously arranged, FIGS. 16/17 and 18/19 show the interior of the alternative circumferential flow chambers divided into two side-by-side processing compartments 84 and 86. In use, centrifugal forces in the first compartment 84 separate whole blood into RBC and PRP. Centrifugal forces in the second processing compartment 86 separate the PRP from the first stage into PC and PPP.
In both alternative circumferential flow chambers, a first peripheral seal 88 forms the outer edge of the circumferential flow chamber assembly 74 or 76. A second interior seal 90 divides the circumferential flow chamber assembly 74 or 76 into the first processing compartment 84 and the second processing compartment 86. The second seal 90 extends generally parallel to the rotational axis of the chamber assembly 74 or 76; that is, it extends across the circumferential flow of the chamber assembly 74 or 76. The second seal 90 constitutes a longitudinal edge common to both first and second processing compartments 84 and 86.
Each processing compartment 84 and 86 serves as a separate and distinct separation chamber and will therefore be referred to as such.
In each alternative circumferential flow chambers, five ports 92/94/96/98/100 open into the compartmentalized areas formed in the processing chamber assembly 74 or 76. The ports 92/94/96/98/100 are arranged side-by-side along the top transverse edge of the respective chamber 84 and 86.
The ports 92/94/96/98/100 are all axially oriented; that is, their axes are aligned with the axis of rotation, transverse the circumferential fluid flow path within the chamber assembly 74 or 76 itself. Three ports 92/94/96 serve the first chamber 84. Two ports 98/100 serve the second chamber 86.
In both alternative circumferential flow chamber assemblies 74 and 76, an umbilicus 102 (see
As
Using either alternative circumferential flow chamber assembly 74 or 76, the two omega speed at which the suspended spool and bowl elements 80 and 82 rotate is about 3400 RPM. Given the dimensions of the spool and bowl elements 80 and 82, 3400 RPM will develop a centrifugal force field of about 900 G's along the high-G wall 66 of the chambers 84 and 86.
A. The First Stage Processing Chamber
In the embodiment shown in
A third interior seal 110 is located between the PRP collection port 72 and the WB inlet port 68. The third seal 110 includes a first region 112 that is generally parallel to the second interior seal 90, thereby extending across the circumferential WB flow path. The third interior seal 110 then bends in a dog-leg portion 114 away from the WB inlet port 68 in the direction of circumferential WB flow. The dog-leg portion 114 terminates beneath the inlet of the PRP collection port 72.
A fourth interior seal 116 is located between the WB inlet port 68 and the RBC collection port 74. The fourth seal 116 includes a first region 118 that is generally parallel to the second and third interior seals 90 and 110, thereby extending across the circumferential WB flow path. The fourth interior seal 116 then bends in a dog-leg portion 120 away from the RBC collection port 74 in the direction of circumferential WB flow. The dog-leg portion 120 extends beneath and beyond the dog-leg portion 114 of the third seal 110. It terminates near the longitudinal side edge of the first chamber 84 that is opposite to the longitudinal side edge formed by the second interior seal 90.
Together, the third and fourth interior seals 110/116 form a WB inlet passage 122 that first extends along the axis of rotation (i.e., between the first regions 112/118 of the two seals 110/116). The WB inlet passage 122 then bends to open in the direction of intended circumferential flow within the first chamber 84 (i.e., between the dog-leg portions 114/120 of the two seals 110/116).
The WB inlet passage 122 first channels WB away from the WB inlet port 68 in an axial flow path. It then channels WB circumferentially, directly into the circumferential flow path, where separation into RBC and PRP begins.
The third interior seal 110 also forms a PRP collection region 124 within the first chamber 84 (i.e., between the third seal 110 and the adjacent upper portion of the first peripheral seal 88).
Together, the fourth interior seal 116, the second interior seal 90, and the lower regions of the first peripheral seal 88 form a RBC collection passage 126 that extends first along the axis of rotation (i.e., between the second interior seal 90 and the fourth interior seal 116). The RBC collection passage 126 then bends in a circumferential path to open near the end of the intended WB circumferential flow path (i.e., between the dog-leg portion 120 of the fourth seal 116 and the lower region of the peripheral seal 88).
In the embodiment shown in
As
Together, the second and third interior seals 90 and 110 form a WB inlet passage 122, like the WB inlet passage 122 associated with the chamber 84 shown in
As
Together, the fourth interior seal 116 and the upper regions of the first peripheral seal 88 form a RBC collection passage 126, like the RBC collection passage 126 shown in
As
The dynamic flow conditions within each alternative circumferential flow chamber assembly 74 or 76 are the same. These conditions direct PRP toward the PRP collection region 124 for collection through the inlet of the PRP collection port 72.
As
The RBC collection passage 126 receives RBC at its open end and from there channels the RBC to the RBC collection port 74. As
In each alternative circumferential flow chamber assembly 74 and 76 (as
In the particular embodiments shown, the low-G wall 64 tapers into the chamber 84 in the direction of circumferential WB flow. The taper proceeds from the second interior seal 90 toward the opposite longitudinal end of the chamber.
The tapering low-G wall 64 includes a stepped-up barrier 128 or dam in the region where the RBC collection passage 126 opens. As
As
While various configurations can be used, in a preferred arrangement, the low-G wall 64 tapers about 2 mm into the chamber 74 where it joins the barrier 128. The barrier 128 extends from there at about a 45 degree angle toward the high-G wall 66, forming a raised planar surface. The passage 129 formed between the planar surface and the high-G wall 66 is about 1 mm to 2 mm in radial depth and about 1 mm to 2 mm in circumferential length.
As previously described (and as
The desired contours for the low-G wall 64 of the alternative chamber assemblies 74 and 76 can be preformed on the exterior surface of the spool element 82. In the illustrated embodiment, the interior surface of the bowl element 82 is isoradial with respect to the rotational axis.
Also in both alternative embodiments (as
The taper of the dog leg portion 120 is preferably gauged relative to the taper of the low-G wall 64 to keep the cross sectional area of the RBC collection passage 126 substantially constant. This keeps fluid resistance within the passage 126 relatively constant, while maximizing the available separation and collection areas outside the passage 126. The taper of the dog leg portion 120 also facilitates the removal of air from the passage 126 during priming.
As
In the illustrated embodiment (see FIG. 22), a hinged flap 132 extends from and overhangs a portion of the spool element 82. The flap 132 is preformed to present the desired contour of the ramp 130.
When flipped down (as
As shown diagrammatically in
As will be described in greater detail later, the interface controller 134 monitors the location of the interface 26 on the ramp 130. As FIGS. 25A/B/C show, the position of the interface 26 upon the ramp 130 can be altered by controlling the relative flow rates of WB, the RBC, and the PRP through their respective ports 68/70/72. The controller 134 varies the rate at which PRP is drawn from the chamber 84 to keep the interface 26 at a prescribed location on the ramp 26 (which
The ramp 130 and associated interface controller 134 keep RBC, white blood cells, and lymphocytes present in the interface 26 from entering the PRP collection port 72. The collected PRP is thereby essentially free of the other cellular components present in the interface 26.
B. The Second Stage Processing Chamber
In the embodiment of the chamber assembly shown in FIGS. 16/17, the fourth port 98 constitutes a PPP collection port 136, and the fifth port 100 constitutes a PRP inlet pdrt 138. In the embodiment shown in FIGS. 18/19, the opposite is true: the fourth port 98 constitutes the PPP inlet port 138, and the fifth port 100 constitutes the PPP collection port 136.
In each chamber assembly 74/76, the umbilicus 102 connects the PRP collection port 72 of the first chamber 84 with the PRP inlet port 138 of the associated second chamber 86. The second chamber 86 thereby receives PRP from the first chamber 84 for further separation into PPP and PC. The umbilicus 102 conveys separated PPP from the second chamber 86 through the associated PPP collection port 136. In each assembly 74/76, the PC remains behind in the second chamber 86 for later resuspension and collection.
In the alternative embodiments shown in FIGS. 16/17 and 18/19, a fifth interior seal 140 extends between the PRP inlet port 138 and the PPP collection port 136. The fifth seal 140 includes a first region 142 that is generally parallel to the second seal 90, thereby extending across the circumferential flow path. The fifth interior seal 140 then bends in a dog-leg portion 144 away from the PRP inlet port 138 in the direction of circumferential PRP flow within the second chamber 86. The dog-leg portion 144 terminates near the longitudinal side edge of the second chamber 86 that is opposite to the longitudinal side edge formed by the second interior seal 90.
In the FIGS. 16/17 embodiment, the fifth interior seal 140, the second interior seal 90, and the lower regions of the first peripheral seal 88 together form a PPP collection passage 146 that extends first along the axis of rotation (i.e., between the second interior seal 90 and the fifth interior seal 140) and then bends in a circumferential path to open near the end of the intended PRP circumferential flow path (i.e., between the dog-leg portion 144 of the fifth seal 140 and the lower region of the peripheral seal 88). The PPP collection passage 146 receives PPP at its open end and from there channels the PPP to the PPP collection port 136.
In the FIGS. 18/19 embodiment, a similar PPP collection passage 146 is formed between the fifth interior seal 140 and the upper region of the peripheral seal 88.
In each alternative circumferential flow chamber assembly 74/76, PRP entering the second chamber 86 via the PRP inlet port 138 is caused to flow first in an axial path from the axially oriented PRP inlet port 138 alongside the axially extending fifth seal 140. The flow direction of the PRP then turns to a circumferential path away from the fifth seal 140 toward the opposite longitudinal side edge.
The centrifugal forces generated during rotation of the chamber separate the PRP into PC and PPP. The more dense PC separate out into a layer that extends along the high-G wall 66. The less dense PPP is displaced toward the low-G wall 64 for collection through the PPP collection passage 146.
The inventor has discovered that the introduction of PRP along an axial flow path parallel to the axis of rotation into a circumferential flow path about the axis of rotation creates a non-turbulent vortex region 148, called a Taylor column, at the outlet of the PRP inlet port 138, as
The vortex region 148 circulates about an axis that is aligned with the axis of the PRP inlet port 138. The vortex region 148 stretches from the outlet of the port 138 longitudinally across the circumferential flow path of the chamber 86. As
Within the vortex region 148, axial flow velocity decreases in a generally linear fashion across the circumferential flow path of the chamber 86. This occurs as the axial flow of fluid entering the chamber 86 perfuses uniformly into a circumferential flow entering the separation zone.
A similar vortex region 148 forms at the opposite longitudinal end of the second chamber 86 at the entrance to the PPP collection passage 146, as
The vortex region 148 created at the outlet of the PRP inlet port 138 uniformly disperses PRP in the desired circumferential flow path into the centrifugal field. This maximizes the exposure of the entering PRP to the effects of the centrifugal field across the effective surface area of the second chamber 86. Maximum possible separation of PC from the entering PRP results.
It should be noted that similar vortex region 148 flow conditions are formed in the first chamber 84 as well, where fluid either enters or leaves the established circumferential flow path through an axial flow path. As
In both alternative chamber assemblies 74/76 (as
Also in both alternative chamber assemblies 74/76 (as
As with the taper of the dog leg portion 120, the taper of the circumferential leg of the PPP collection passage 146 is preferably gauged relative to the taper of the low-G wall 64 to keep the cross sectional area of the PPP collection passage 146 substantially constant. This keeps fluid resistance within the passage 146 relatively constant. The taper of the circumferential leg of PPP collection passage 146 also facilitates the removal of air from the passage 146 during priming.
The dimensions of the various regions created in the processing chamber can of course vary according to the processing objectives. Table 2 shows the various dimensions of a representative embodiment of a processing chamber of the type shown in FIGS. 16/17 or 18/19. Dimensions A through F referenced in Table 2 are identified for their respective chamber assemblies in
The two stage circumferential flow chambers shown in either FIGS. 16/17 or FIGS. 18/19 can be used to do continuous platelet collection. The chambers can be used in associated either with a system 150 that employs one phlebotomy needle (as
A. Single Needle Enhanced Yield Platelet Collection System
The platelet collection system 150 shown in
The processing controller 154 operates the single needle system 150 in a draw cycle and a return cycle.
During the draw cycle, the controller 154 supplies the donor's WB through the needle 156 to a chosen one of the processing chamber assemblies 74/76. There, the WB is centrifugally separated into RBC, PC, and PPP.
During the return cycle, the controller 154 returns RBC and PPP to the donor through the needle 156, while separation within the chosen processing chamber assembly 74/76 continues without interruption. The harvested PC is retained for long term storage. If desired, all or some PPP can be retained for storage, too.
The system 150 includes a draw reservoir 158, which pools a quantity of the donor's WB during the draw cycle. The system 150 also includes a return reservoir 160, where a quantity of RBC collect for periodic return to the donor during the return cycle.
Processing containers associated with the system 150 include a container 162 that holds anticoagulant for use during the procedure and a container 164 that holds saline solution for use in priming and purging air from the system 150 before the procedure. The system further includes collection containers 166 for receiving PC (and optionally PPP) for storage.
When the controller 154 operates the system 150 in the draw cycle, a first branch 168 directs WB from needle 156 to the draw reservoir 158, in association with the draw pumping station 170 and a clamp 172. An auxiliary branch 174 delivers anticoagulant to the WB flow in association with an anticoagulant pumping station 176.
A second branch 178 conveys the WB from the draw reservoir 158 to the WB inlet port 68 of the chosen processing chamber assembly 74/76, in association with the WB inlet pumping station 180. The draw pumping station 170 operates at a higher flow rate (at, for example, 100 ml/min) than the WB inlet pumping station 180, which operates continuously (at, for example, 50 ml/min).
The processing controller 154 includes a first scale 182 that monitors the weight volume of WB collected in the draw reservoir 158. The first scale 182 intermittently operates the draw pumping station 170 to maintain a desired weight volume of WB in the draw reservoir 158.
Once the desired volume of WB is present in the draw reservoir 158, the WB inlet pumping station 180 operates to continuously convey WB into the chosen processing chamber assembly 74/76.
The draw pumping station 170 continues to operate periodically during the draw cycle in response to the scale 182 to maintain the desired weight volume of WB in the draw reservoir 158.
The WB enters the first stage chamber 84, where it is separated into RBC and PRP. This separation process has already been described.
A third branch 184, in association with the plasma pumping station 186, draws the PRP from the PRP collection port of the first processing chamber 84. The third branch 184 conveys the PRP to the PRP inlet port 138 of the second processing chamber 86. There, the PRP is further separated into PC and PPP. This separation process has already been described.
As will be described in greater detail later, the processing controller 154 monitors the location of the interface on the ramp 130 via the interface controller 134. The controller 154 operates the plasma pumping station 186 to keep the maximum rate of the variable plasma pumping station 186 (for example, 25 ml/min) less than the WB inlet pumping station 180.
A fourth branch 188 conveys the RBC from the RBC collection port 74 of the first stage processing chamber 84. The fourth branch 188 leads to the return reservoir 160.
The processing controller 154 includes a second scale 190 that monitors the weight volume of RBC in the return reservoir 160. When a preselected weight volume exists, the controller 154 shifts the operation of the system 150 from its draw cycle to its return cycle.
In the return cycle, the controller 154 stops the draw pumping station 170 and starts a return pumping station 192. A fifth branch 194 associated with the return pumping station 192 conveys RBC from the return reservoir 160 to the needle 156.
Meanwhile, while in the return cycle, the controller 154 keeps the WB inlet pumping station 180 and plasma pumping station 186 in operation to continuously process the WB pooled in the draw reservoir 158 through the first processing chamber 84.
During both draw and return cycles, PRP enters the PRP inlet port 138 of the second stage processing chamber 86. The PPP exits the PPP collection port 136 of the second stage processing chamber through a sixth branch 196 and into the return reservoir 160, joining the RBC there pooled.
Alternatively, by closing the clamp 198A and opening the clamp 198B, the PPP can be conveyed through a seventh branch 200 to one or more collection containers 166.
After a procedure, the PC collected within the second processing compartment 86 is transferred via the seventh branch 200 to one or more collection containers 166 for storage.
B. Double Needle Platelet Collection System
The platelet collection system 152 shown in
The associated processing controller 154 operates the system 152 in a continuous cycle, during which the donor's WB is continuously supplied through the needle 202A to the chosen processing chamber assembly 74/76 for separation into RBC, PC, and PPP, while RBC and PPP are continuously returned to the donor through the needle 202B.
As in the single needle system 150, the harvested PC is retained for long term storage. If desired, all or some PPP can be diverted from the donor for storage.
As in the single needle system 150, the processing containers associated with the double needle system 152 include a container 162 that holds anticoagulant and a container 164 that holds saline solution for use in priming and purging air from the system 152.
The system 152 also includes similar collection containers 166 for receiving PC (and optionally PPP) for storage.
Under the control of the controller 154, a first branch 204 directs WB from the needle 202A to the WB inlet port 68 of the first stage processing chamber 84, in association with the WB inlet pumping station 206, which operates continuously at, for example, 50 ml/min. An auxiliary branch 174 delivers anticoagulant to the WB flow in association with an anticoagulant pumping station 176.
The WB enters and fills the first processing chamber 84 in the manner previously described, where centrifugal forces generated during rotation of the chosen chamber assembly 74/76 separate the WB into RBC and PRP.
A second branch 208, in association with the plasma pumping station 210, draws the PRP layer out the PRP collection port 72 of the first stage processing chamber 84, conveying the PRP to the PRP inlet port 138 of the second stage processing chamber 86, where it undergoes further separation into PC and PPP.
The processing controller 154 monitors the location of the interface on the ramp 130 and varies the speed of the plasma pumping station 210 (using the interface controller 134, to be described later in greater detail) to keep the interface 26 at a prescribed location on the ramp 130. As before described, the controller 154 keeps the maximum rate of the variable plasma pumping station 210 (for example, 25 ml/min) less than the WB inlet pumping station 206.
A third branch 212 conveys the RBC from the RBC collection port 70 of the first stage processing chamber 84. The third branch 212 leads to the needle 202B.
The PPP exits the PPP collection port 136 of the second stage processing chamber 86 through a fourth branch 214, joining the third branch 212 (carrying RBC) leading to the needle 202B. Alternatively, by closing the clamp 216A and opening the clamp 216B, the PPP can be conveyed through a fifth branch 218 to one or more collection containers 166.
After a procedure, the PC collected within the second processing compartment 86 is transferred via the fifth branch 218 to one or more collection containers 166 for storage.
C. Enhancing Platelet Separation by Plasma Recirculation
Both single and double needle systems 150 and 152 (shown in
The control system 224 can control the recirculation of PRP in different ways.
As
The recirculation control system 224 employs a comparator 228 to compare the sensed PRP flow rate to an established desired flow rate. If the sensed rate is less than the desired flow rate, the comparator 228 sends a signal to increase rate at which the recirculation pumping station 222 operates. And, if the sensed rate is more than the desired flow rate, the comparator 228 sends a signal to decrease the rate at which the recirculation pumping station 222 operates. In this way, the comparator 228 maintains the PRP flow rate at the desired rate.
The desired PRP output rate is preselected to create within the first compartment 84 the processing conditions which maximize the concentration of platelets in the PRP stream.
The desired rate of recirculation is based upon the radial flow rate of plasma desired in the region where PRP is collected.
According to another aspect of the invention, the pumping rate of the recirculation pump 22 is maintained as a percentage (%RE) of the pumping rate of the whole blood inlet pump 180/206, governed as follows:
%RE=K*Hct−100
where:
According to this aspect of the invention, the pumping rate of the recirculation pump 22 is maintained at the predetermined percentage (%RE) of the pumping rate of the whole blood inlet pump 180/206 to maintain a surface hematocrit of about 30% to 35% in the entry region Re. The preferred surface hematocrit in the entry region Re is believed to be about 32%.
Keeping the surface hematocrit in the entry region Re in the desired range provides optimal separation of RBC from PRP, thereby optimizing the radial flow of plasma in this region. If the surface hematocrit exceeds the predetermined range, radial plasma flow in the entry region Re decreases. If the surface hematocrit falls below the predetermined range, the radial flow of PRP increases enough to sweep small RBC's and white blood cells into the PRP.
The value of the dilution factor K can vary according to operating conditions. The inventor has determined that K=2.8, when ACD anticoagulant is added to constitute about 9% of the entry whole blood volume, and a saline dilution fluid is added in an amount representing about 4% of donor body volume (i.e., 200 ml saline for 5000 ml in body volume).
In an alternate arrangement (shown in phantom lines in FIG. 29), the recirculation control system 224 recirculates PPP, instead of PRP, based upon %RE, as determined above.
In this arrangement, the system 224 uses a recirculation branch 230 and associated pumping station 232 located downstream of the second processing compartment 86. The comparator controls the pumping station 232 in one of the same manners just described to mix PPP exiting the second compartment 86 with the incoming WB entering the first compartment 84.
By mixing PRP (or PPP) with the WB entering the first processing compartment 84 to control surface hematocrit in the entry region Re, the velocity at which red blood cells settle toward the high-G wall 66 in response to centrifugal force increases. This, in turn, increases the radial velocity at which plasma is displaced through the interface 26 toward the low-G wall 64. The increased plasma velocities through the interface 26 elute platelets from the interface 26. As a result, fewer platelets settle on the interface 26.
A study evaluated a two stage separation chamber 74 like that shown in
In this study, the low-G wall 64 of the first stage chamber 84 was not tapered in the direction of circumferential flow from the PRP collection region 124. The low-G wall 64 was isoradial along the circumferential flow path in the first stage chamber 84, except for the presence of a RBC barrier 128, which stepped into the chamber across the RBC collection passage, as shown in FIG. 17. The low-G wall 64 was isoradial along the entire circumferential flow path of the second chamber 86.
The platelet transfer efficiency in the first stage chamber 84 (i.e., the percentage of available platelets entering the first stage chamber 84 that were ultimately collected in the PRP) was 93.8%. In other words, the first stage chamber 84 failed to collect only 6.2% of the available platelets in the first stage chamber 84.
The platelet transfer efficiency in the second stage chamber 86 (i.e., the percentage of available platelets in the PRP entering the second stage chamber 86 that were ultimately collected as PC) was 99%. In other words, the second stage chamber 86 failed to collect only 1% of the platelets present in the PRP in the second stage chamber 86.
The overall platelet collection efficiency of the chamber was about 81%, meaning that about 81% of the platelets in the whole blood processed were ultimately collected. This is a significantly higher amount than conventional processing can provide. In comparison, the comparable overall platelet collection efficiency for two stage CS-3000® Centrifuge chamber is about 50%.
This study demonstrates the increased separation efficiencies that result from chambers and systems that embody features of the invention.
Another study evaluated a two stage separation chamber like that in Example 2 in a platelet collection procedure on a healthy human donor. As in Example 2, a double needle system was used. The system recirculated PRP to obtain an inlet hematocrit of 34.3%.
In this study, the low-G wall 64 of the first stage chamber 84 was tapered in the direction of circumferential flow from the PRP collection region 124, like that shown in FIG. 17. The low-G wall 64 also included RBC barrier 128 like that shown in FIG. 17. The low-G wall 64 was also tapered along the entire circumferential flow path of the second chamber 86.
The second study also experienced greater collection efficiencies.
The platelet transfer efficiency in the first stage chamber 84 (i.e., the percentage of available platelets that were ultimately collected in the PRP) was 99.2%. In other words, the first stage chamber 84 failed to collect less than 1% of the available platelets.
The platelet transfer efficiency in the second stage chamber 86 (i.e., the percentage of available platelets in the PRP that were ultimately collected as PC) was 99.7%. In other words, the second stage chamber 86 collected nearly all the platelets present in the PRP.
The overall platelet collection efficiency of the chamber was 85.3%.
This study further demonstrates the enhanced separation efficiencies that the inventions can provide.
This study also shows the effect that the tapered low-G wall has in freeing greater number of platelets into the PRP stream. The effect is virtually immediate. After only 5 minutes in the second study, the platelet count was comparable to that encountered after 10 minutes in the first study.
This study also demonstrates the effect that the tapered low-G wall has in freeing larger platelets into the PRP stream. The effect, too, is virtually immediate. After the first 5 minutes of the procedure, the mean platelet size was comparable to that encountered after 30 minutes in the second study, which means that the larger platelets were already being collected. There were nearly 3 times more platelets of very large physical size (i.e., over 30 femtoliters) collected in the second study than in the first study.
The interface control system 234 mounts the element that actually views the interface on a rotating element of the centrifuge. The system 234 relies upon a time pulse signal to determine the location of the interface.
As
As
In the illustrated and preferred embodiment, the viewing head 238 also serves as a counterweight for the umbilicus holder 106 that the yoke 85 also carries (also see FIGS. 20 and 21).
In the illustrated and preferred embodiment, the light source 236 includes a red light emitting diode. Of course, other colors, like green, could be used. In this arrangement, the light detector 244 comprises a PIN diode detector.
An optical pathway 240 directs light from the source diode 236 out onto the rotating bowl assembly 80 (see FIG. 31B). In the illustrated embodiment, the bowl assembly 80 is transparent to the light emitted by the source diode 236 only in the region where the bowl assembly 80 overlies the interface ramp 130.
The remainder of the bowl assembly 80 that lies in the path of the viewing head 238 carries a light reflecting material 243. This differentiates the reflective properties of the interface region of the bowl assembly 80 from those of the remainder of the bowl assembly 80. The material 243 could be light absorbing and serve the same purpose.
Alternatively, the source diode 236 could be gated on and off with the arrival and passage of the interface region of the bowl assembly 80 relative to its line of sight.
The interface ramp 130 carried by the spool assembly 82 is made of a light transmissive material. The light from the source diode 236 will thus pass through the transparent region of the bowl assembly 80 and the ramp 130 every time the rotating bowl assembly 80 and viewing head 238 align.
The spool assembly 82 also carries a light reflective material 242 on its exterior surface behind the interface ramp 130 (see FIG. 36). The material 242 reflects incoming light received from the source diode 236 out through the transparent region of the bowl assembly 80. The intensity of the reflected light represents the amount of light from the source diode 236 that is not absorbed by the RBC portion of the interface region.
The light detector 244 carried in the viewing head 238 receives the reflected light through an optical pathway. In the illustrated embodiment (see FIG. 31B), the optical pathway includes a lens 246, a penta prism 248, and an aperture 250.
In the illustrated embodiment, the lens 246 is about 9 mm in diameter, with the focal length of about 9 mm. In this arrangement, the lens 246 forms a real image with a magnification of about three. Alternatively, the real image could be made smaller to provide a better depth of field.
The aperture 250 is preferably small (about 0.75 mm in diameter) to allow only a small portion of the real image to reach the detector 244. The preferred viewing field of the detector 244 is therefore small, i.e., preferably on the order of about 0.25 mm in diameter.
The system 234 further includes a data link 278 for transmitting light intensity signals from the rotating viewing head 268 to an interface control circuit 270 on the stationary frame of the centrifuge. In the illustrated embodiment, the data link is optical in nature. Alternatively, slip rings could be used to transmit the light intensity signals as voltage or current signals.
The optical data link 278 includes a second light source 254. The second light source 254 is carried within the confines of a hollow light conduction passage 256 within the one omega drive shaft 257.
The optical data link 278 further includes a second light detector 268. The second detector 268 is carried on the non-rotating (i.e., zero omega) base of the centrifuge below the hollow one omega drive shaft 257. Light from the second light source 254 passes through the passage 256 and a collimating sleeve 259 to fall upon the second detector 268. Like the first detector 244, the second detector 268 can comprise a PIN diode detector.
The second light source 254 comprises at least one red light emitting diode carried within the passage 256 of the one omega shaft 257. Of course, other colors, like green, could be used.
In the illustrated embodiment (see FIG. 30), the second light source 254 includes three light emitting diodes 258 A/B/C arranged at 120 degree circumferentially spaced intervals within the passage 256. This arrangement minimizes interference due to misalignment between the second light source 254 and the second detector 268. In an alternative arrangement, the light intensity signal from the second detector 268 can be electronically filtered to eliminate interference signals caused by misalignment.
The optical data link 278 also includes an intensity control circuit 252 carried onboard the viewing head 238. The intensity control circuit 252 adjusts the input to the source diode 236 so that the intensity of light hitting the detector 244 remains constant.
The intensity control circuit 252 also connects the second light source 254 in series to the first mentioned light source 236. Thus, as the intensity control circuit 252 adjust the input to the first light source 236, it will also instantaneously adjust the input to the second light source 254. Thus the intensity of the light emitted by the source 254 is proportional to the intensity of light emitted by the source 236.
As
The emitter of the transistor 260 is coupled to an amplifier 262. One amplifier input is coupled to the light detector 244 carried within the yoke viewing head 238. Another amplifier input is coupled to a reference diode 264. The circuit 252 also includes conventional current limiting resistors 266 to protect the light emitting diodes of the sources 236 and 254.
As the intensity of light hitting the detector 244 decreases, the output of the amplifier 262 increases. The transistor 260 conducts more current. The intensities of the first and second light sources 236 instantaneously increase by equal or otherwise proportional amounts.
Likewise, as the intensity of light hitting the detector 244 increases, the output of the amplifier 262 decreases. The transistor 260 conducts less current. The intensities of the first and second light sources 236 instantaneously decrease by equal or proportional amounts.
As
From the time pulses, the interface control circuit 270 derives the physical dimension of the interface (measured in inches). The interface control circuit 270 then generates a pump control signal based upon any differences between the derived interface dimension and a desired interface dimension.
As
As the transparent interface region of the bowl assembly 80 comes into alignment with the viewing head 238, red blood cells displayed on the interface ramp 130 will enter the optical path of the viewing head 238.
The red blood cells absorb the light from the first light source 236. This absorption reduces the previously viewed intensity of the reflected light. With decreasing light intensity sensed, the control circuit 252 instantaneously increases the input to both first and second light sources 236 and 254 to maintain a constant light intensity at the first detector 244.
Under the control of the circuit 252, both light sources 236 and 254 will become brighter, assuming a new intensity level while the red blood cell band of the interface pass past the viewing head 238.
As
As
Eventually, the intensity signal will stabilize, as the most dense region of the red cell band of the interface enters the optical path of the viewing head 238. The interface control circuit 270 converts the stabilized intensity signal into the plateau 275 of the square pulse 272 shown in FIG. 33B.
When the red cell band of the interface leaves the optical path of the viewing head 238, the first detector 244 will again view fully reflected light from the reflective bowl material 243. With increasing light intensity sensed, the control circuit 252 will instantaneously decrease the input to both first and second light sources 236 and 254 to maintain a constant light intensity at the first detector 244.
Again, the first detector 244 will not see this relative decrease in intensity over time, because the control circuit 252 instantaneously maintains the intensity I1 viewed by the first detector 244 constant. However, the second detector 268 will sense this relative decrease in intensity over time. The second detector 268 generates a decreasing intensity output signal I2. The interface control circuit 270 converts this signal to the trailing edge 276 of the square pulse 272 shown in FIG. 38B. This event marks the ending time (T2) of the pulse 272.
As
The interface control circuit 270 also preferably measures the time period between two successive pulses (shown as 272A and 272B in FIG. 33C). This period of time is measured between the leading edge 274 of the first pulse 272A (T1 in
After this measurement has been made, the interface control circuit 270 then resets T3 to T1 for the next pulse measurement cycle (see FIG. 34A).
As
where:
If the rate of rotation of the bowl assembly 80 remains constant during the period of pulse measurements, the reciprocal of the frequency of rotation in seconds (1/Frot, in Hz)) can be substituted for PP.
Based upon the above relationship, DI can be derived as follows:
As
The interface control value DC can comprise a preselected fixed absolute value (in inches) that the user inputs. Alternatively, the interface control value DC can be expressed as a percentage based upon the length of the interface ramp 130 (i.e., red cells should occupy no more than 30% of the interface ramp 130).
With reference now also to
With reference to
The optical data link 278 described above is representative of a broader class of systems for transmitting a control signal between a rotating element and a stationary element without mechanical contact between the two elements.
Like the illustrated optical data link 278, such a system employs sensor means on either the rotating or stationary element. The sensor means senses an operating condition that is subject to change. The sensor means generates a first output signal that varies according to changes in the sensed operating condition.
Like the illustrated optical data link 278, such a system includes an energy emitter on the one element that carries the sensor means. The emitter emits energy to the other element without mechanical contact with the other element. The emitter modulates the emitted energy according to variations occurring in the intensity of the first output signal. Alternatively, the sensor means itself can constitute an emitter of modulated energy.
The emitted energy used by the data link 278 is light. However, sound energy or other types of electromagnetic energy could be used as well.
Like the illustrated data link 278, the system includes a detector on the other element for receiving the modulated energy emitted by the emitter. The detector demodulates the detected energy to generate a second output signal that, like the first output signal, varies according to the changes in the sensed operating condition.
Such a “connectionless” system for transmitting data between moving and stationary elements would be applicable for use for all sorts of real time control functions, not just interface control.
Various features of the inventions are set forth in the following claims.
This application is a divisional of co-pending U.S. patent application Ser. No. 09/661,331, filed Sep. 13, 2000 (now U.S. Pat. No. 6,511,411), entitled “Compact Enhanced Yield Blood Processing Systems,” which is a divisional of U.S. patent application Ser. No. 08/856,096, filed May 14, 1997 (now U.S. Pat. No. 6,228,017), which is a divisional of U.S. patent application Ser. No. 08/146,403 filed Nov. 1, 1993 (now U.S. Pat. No. 5,656,163), which is a continuation of U.S. patent application Ser. No. 07/964,771, filed Oct. 22, 1992 (now abandoned).
Number | Name | Date | Kind |
---|---|---|---|
3244363 | Hein | Apr 1966 | A |
3347454 | Bellamy, Jr. et al. | Oct 1967 | A |
3489145 | Judson et al. | Jan 1970 | A |
3519201 | Eisel et al. | Jul 1970 | A |
3561672 | Schultz et al. | Feb 1971 | A |
3655123 | Judson et al. | Apr 1972 | A |
3672564 | Schultz et al. | Jun 1972 | A |
3737096 | Jones et al. | Jun 1973 | A |
3748101 | Jones et al. | Jul 1973 | A |
3786919 | Deringer | Jan 1974 | A |
3825175 | Sartory | Jul 1974 | A |
3858796 | Unger et al. | Jan 1975 | A |
3953329 | Updike | Apr 1976 | A |
3957197 | Sartory et al. | May 1976 | A |
3987961 | Sinn et al. | Oct 1976 | A |
4007871 | Jones et al. | Feb 1977 | A |
4010894 | Kellogg et al. | Mar 1977 | A |
4013564 | Nose | Mar 1977 | A |
4056224 | Lolachi | Nov 1977 | A |
4091989 | Schlutz | May 1978 | A |
4094461 | Kellogg et al. | Jun 1978 | A |
4098456 | Bayham | Jul 1978 | A |
RE29738 | Adams | Aug 1978 | E |
4108353 | Brown | Aug 1978 | A |
4109852 | Brown et al. | Aug 1978 | A |
4109854 | Brown | Aug 1978 | A |
4109855 | Brown et al. | Aug 1978 | A |
4111356 | Boggs et al. | Sep 1978 | A |
4113173 | Lolachi | Sep 1978 | A |
4114802 | Brown | Sep 1978 | A |
4120448 | Cullis | Oct 1978 | A |
4120449 | Brown et al. | Oct 1978 | A |
4127231 | Khoja et al. | Nov 1978 | A |
4142670 | Ishimaru et al. | Mar 1979 | A |
4146172 | Cullis et al. | Mar 1979 | A |
4164318 | Boggs | Aug 1979 | A |
4185629 | Cullis et al. | Jan 1980 | A |
4187979 | Cullis et al. | Feb 1980 | A |
4191182 | Popovich et al. | Mar 1980 | A |
4194684 | Boggs | Mar 1980 | A |
D255935 | Cullis et al. | Jul 1980 | S |
D255936 | Cullis et al. | Jul 1980 | S |
4215688 | Terman et al. | Aug 1980 | A |
4216770 | Cullis et al. | Aug 1980 | A |
4223672 | Terman et al. | Sep 1980 | A |
4230263 | Westberg | Oct 1980 | A |
4244513 | Fayer et al. | Jan 1981 | A |
D258909 | Bergo et al. | Apr 1981 | S |
4261507 | Bäumler | Apr 1981 | A |
4266717 | Jennings et al. | May 1981 | A |
4269718 | Persidsky | May 1981 | A |
4278201 | Cailliot | Jul 1981 | A |
4278202 | Westberg | Jul 1981 | A |
4283004 | Lamadrid | Aug 1981 | A |
4283276 | Grant | Aug 1981 | A |
4316576 | Cullis et al. | Feb 1982 | A |
4330080 | Mathieu | May 1982 | A |
4343705 | Legg | Aug 1982 | A |
4344560 | Iriguchi et al. | Aug 1982 | A |
4350283 | Leonian | Sep 1982 | A |
4353795 | Romanauskas | Oct 1982 | A |
4357235 | Dilks, Jr. | Nov 1982 | A |
4379452 | DeVries | Apr 1983 | A |
4386730 | Mulzet | Jun 1983 | A |
4387848 | Kellogg et al. | Jun 1983 | A |
4402680 | Schoendorfer | Sep 1983 | A |
4405079 | Schoendorfer | Sep 1983 | A |
4411792 | Babb | Oct 1983 | A |
4419089 | Kolobow et al. | Dec 1983 | A |
4421503 | Latham, Jr. et al. | Dec 1983 | A |
4425112 | Ito | Jan 1984 | A |
4430072 | Kellogg et al. | Feb 1984 | A |
4432871 | Yamawaki et al. | Feb 1984 | A |
4445883 | Schroendorfer | May 1984 | A |
4446014 | Dilks, Jr. et al. | May 1984 | A |
4446015 | Kirkland | May 1984 | A |
4447221 | Mulzet | May 1984 | A |
4448679 | Dilks, Jr. et al. | May 1984 | A |
4464167 | Schoendorfer et al. | Aug 1984 | A |
4482342 | Lueptow et al. | Nov 1984 | A |
4493691 | Calari | Jan 1985 | A |
4530691 | Brown | Jul 1985 | A |
4531932 | Luppi et al. | Jul 1985 | A |
4605503 | Bilstad et al. | Aug 1986 | A |
4609461 | Takata et al. | Sep 1986 | A |
4627915 | Kuroda et al. | Dec 1986 | A |
4636193 | Cullis | Jan 1987 | A |
4647279 | Mulzet et al. | Mar 1987 | A |
4648866 | Malbrancq et al. | Mar 1987 | A |
4655742 | Vantard | Apr 1987 | A |
4670002 | Koreeda et al. | Jun 1987 | A |
4675117 | Neumann et al. | Jun 1987 | A |
4708712 | Mulzet | Nov 1987 | A |
4710161 | Takabayashi et al. | Dec 1987 | A |
4724317 | Brown et al. | Feb 1988 | A |
4729829 | Duggins | Mar 1988 | A |
4743227 | Takeuchi | May 1988 | A |
4769150 | Ramstack | Sep 1988 | A |
4789482 | DiLeo et al. | Dec 1988 | A |
4790807 | Neumann et al. | Dec 1988 | A |
4806252 | Brown et al. | Feb 1989 | A |
4834890 | Brown et al. | May 1989 | A |
4850995 | Tie et al. | Jul 1989 | A |
4851126 | Schoendorfer | Jul 1989 | A |
4857190 | Wada et al. | Aug 1989 | A |
4897185 | Schuyler et al. | Jan 1990 | A |
4900298 | Langley | Feb 1990 | A |
4911833 | Schoendorfer et al. | Mar 1990 | A |
4923439 | Seidel et al. | May 1990 | A |
4934995 | Cullis | Jun 1990 | A |
4936820 | Dennehey et al. | Jun 1990 | A |
4968295 | Neumann | Nov 1990 | A |
4975186 | Wada et al. | Dec 1990 | A |
D314824 | Moon | Feb 1991 | S |
4990132 | Unger et al. | Feb 1991 | A |
5006103 | Bacehowski et al. | Apr 1991 | A |
5045185 | Ohnaka et al. | Sep 1991 | A |
5067938 | Uchida et al. | Nov 1991 | A |
5089417 | Wogoman | Feb 1992 | A |
5104526 | Brown et al. | Apr 1992 | A |
5135667 | Schoendorfer | Aug 1992 | A |
5160310 | Yhland | Nov 1992 | A |
5171456 | Hwang et al. | Dec 1992 | A |
5194145 | Schoendorfer | Mar 1993 | A |
5234608 | Duff | Aug 1993 | A |
5370802 | Brown | Dec 1994 | A |
5529691 | Brown | Jun 1996 | A |
Number | Date | Country |
---|---|---|
1303702 | Jun 1992 | CA |
1304309 | Jun 1992 | CA |
0363210 | Apr 1990 | EP |
WO 9115300 | Oct 1991 | WO |
Number | Date | Country | |
---|---|---|---|
20030102272 A1 | Jun 2003 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 09661331 | Sep 2000 | US |
Child | 10337486 | US | |
Parent | 08856096 | May 1997 | US |
Child | 09661331 | US | |
Parent | 08146403 | Nov 1993 | US |
Child | 08856096 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 07964771 | Oct 1992 | US |
Child | 08146403 | US | |
Parent | 07514995 | May 1989 | US |
Child | 07748244 | US | |
Parent | 07009179 | Jan 1987 | US |
Child | 07514995 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 07814403 | Dec 1991 | US |
Child | 07964771 | US | |
Parent | 07748244 | Aug 1991 | US |
Child | 07814403 | US |