Patent Application
20090145502
The present invention relates to a flow system, in particular for use in a micro fluidic system. The flow system of the present invention exhibits a flow resistance which is less temperature sensitive than the flow resistance of prior art flow systems.
Flow systems, in particular flow systems with flow restrictors, can be used for accurately controlling the flow rates of fluidic systems, in particular micro fluidic systems. This may, e.g., be obtained by use of a constant pressure pump. The flow resistance of a flow system depends linearly on the viscosity of the fluid being transported in the flow system. The viscosity of a fluid, however, varies significantly with temperature. For example, in the case of water the viscosity decreases on average by 2.3% per ° C. when the temperature increases from 20° C. to 30° C. Furthermore, this variation is typically non-linear and therefore difficult to control or compensate for. Accordingly, the flow resistance of a flow system varies significantly and non-linearly with temperature, and in order to obtain constant flow rates with high precision it is therefore necessary to keep the temperature at least substantially fixed.
Constant flow rates with high precision are, e.g., desirable when the flow system is or forms part of a drug delivery system or a high precision fluid analysis apparatus, such as a medical device for analysing body fluids, e.g. an apparatus for measuring the concentration of blood glucose in a blood sample. Such apparatuses should operate reliably and consistently regardless of the time and place of use. In case the flow system is portable, which may, e.g., be the case for a blood glucose measurement apparatus, it is very likely that a user would consider using it in environments of varying temperature, e.g. indoors as well as outdoors, at various times of the year, etc. It is therefore very undesirable that the flow resistance of flow systems in the apparatus varies significantly with the temperature.
The document U.S. Pat. No. 3,977,600 describes a temperature responsive fluid flow regulator having a body piece with fluid inlet and outlet passageways and an intermediate fluid chamber. An elastomeric member is disposed within the body piece and is confined therein and has an orifice aligned with the outlet. The member is responsive to temperature changes, and a restraining member confines it such that an increase in temperature causes a reduction in the size of the orifice to thus control the flow of fluid through the regulator. An adjustable needle is also utilized for further controlling the flow through the regulator.
The elastomeric member has a central and circularly-shaped orifice extending therethrough, and the orifice is aligned with and thus is in fluid-flow communication with the body piece outlet so that flow can go from the body piece chamber and past the elastomeric member and through the body piece outlet.
The elastomeric member is free to expand in response to an increase in the temperature in the fluid flowing through the unit, and the elastomeric member is of a characteristic which will cause it to expand in response to a temperature increase as mentioned. Accordingly, when the temperature of the fluid increases, the only expansion possible with regard to the elastomeric member is to have the elastomeric member expanding in a direction toward its center and to thereby reduce its orifice, and thus there is a regulating or a reduction of the flow of fluid past the elastomeric member.
This system is however not easily applied in a micro fluidic system where such moving mechanical parts as the adjustable needle would not be desirable. Other ways to calibrate the system to the desired flow resistance/temperature relation would be needed.
It is, thus, an object of the invention to provide a flow system which is less temperature sensitive than prior art flow systems, and where the calibration of the system to the desired flow resistance/temperature relation is passively build into the system.
It is a further object of the invention to provide a flow system having a flow resistance which is at least substantially independent of an ambient temperature, at least within a specified temperature interval.
It is an even further object of the invention to provide a flow system exhibiting a reliable and at least substantially constant flow rate.
It is an even further object of the invention to provide a micro fluidic system exhibiting an at least substantially constant flow rate without the need to control an ambient temperature.
According to a first aspect of the invention the above and other objects are fulfilled by providing a flow system comprising:
The first part has at least one flow channel formed therein. At least one flow channel may be positioned in an outer region of the first part. Thus, it may be a groove formed in an outer surface of the first part. Alternatively or additionally, at least one flow channel may be positioned in an interior region of the first part. In this case the flow channel may be formed by drilling a channel in the first part. Alternatively and preferably, the first part may be formed by two or more sections made from the same material, one section having the flow channel formed therein as a groove in an outer surface, and another section forming a lid to the groove.
The first part and the second part are arranged relatively to each other in such a way that, in response to a change in an ambient temperature, the first and the second parts cooperate to cause corresponding change(s) in the flow channel(s). As described above the viscosity of a fluid normally decreases as the ambient temperature increases, and vice versa. Accordingly the flow resistance of a flow channel in which the fluid is being transported will change as the ambient temperature changes. According to the invention this change in flow resistance is counteracted by selecting the first and second materials in an appropriate manner, and by designing and positioning the first and second parts relatively to each other in an appropriate manner, as a result obtaining physical changes to at least one section of the flow channel(s), thereby causing a change in the flow resistance of at least that/these section(s). This change at least substantially counteracts the change in flow resistance caused by the change in viscosity of the fluid. Thereby it is obtained that the resulting flow resistance of the flow system is at least substantially independent of the ambient temperature. This is very advantageous because it is thereby possible to maintain an at least substantially constant flow resistance of the flow system, regardless of the ambient temperature, at least within a specified temperature range. A desired flow resistance is thereby obtained without the need for controlling the ambient temperature, and the problems described above can thereby be relieved.
The section(s) may form a smaller or larger part of the flow channel(s). In one embodiment the flow system may comprise only one flow channel, and the section may be the complete flow channel.
In one embodiment the first coefficient of thermal expansion may be higher than the second coefficient of thermal expansion. In this case the first and second parts may be arranged relatively to each other in such a way that the second part restricts thermal expansion of the first part in at least one direction.
In this case the first part will expand or contract more than the second part as the ambient temperature changes. The first and second parts may therefore advantageously be positioned relatively to each other in such a way that the second part restricts the thermal expansion of the first part in such a way that the material of the first part is forced into the flow channel(s) when the ambient temperature increases, and retracts from the flow channel(s) when the ambient temperature decreases. Thereby the size of a cross section of the flow channel(s) and/or the shape of an outer contour of a cross section of the flow channel(s) will change, and accordingly the flow resistance of the flow channel will increase/decrease when the ambient temperature increases/decreases.
The difference between the first coefficient of thermal expansion and the second coefficient of thermal expansion may be sufficiently large to ensure that thermal expansions of the second part are negligible as compared to thermal expansions of the first part. In this embodiment it may be assumed that the second part does not expand as the ambient temperature increases while the first part does expand, and the second part may therefore efficiently restrict the thermal expansion of the first part in the direction(s) where the second part is positioned relatively to the first part.
The first material may comprise a polymer material, including, but not limited to, polystyrene (PS), polyethylene terephthalate glycol (PETG), cyclic olefin copolymer (COC), and/or any other suitable polymer material.
The second material may comprise a metal and/or a semiconductor, including, but not limited to, silicon, aluminium, copper, and/or any other suitable metal or semiconductor.
Alternatively or additionally, the first and second materials may comprise any other suitable materials having appropriate properties with regard to coefficient of thermal expansion.
Alternatively, the second coefficient of thermal expansion may be higher than the first coefficient of thermal expansion, and the first and second parts may be arranged relatively to each other in such a way that the first part restricts thermal expansion of the second part in at least one direction. In this case the second material may comprise a polymer material and/or the first material may comprise a metal and/or a semiconductor. The materials mentioned above will also be suitable in this case.
The first part and/or the second part may further be provided with one or more additional channels, said additional channel(s) being positioned in such a way that it/they cooperate with the first and second parts in causing corresponding change(s) in the flow channel(s). In this embodiment the additional channel(s) preferably has/have a size, shape and position which allows some material to enter the additional channel(s) when the ambient temperature increases and the first or second part accordingly expands. Thereby the amount of material which is forced into the flow channel(s) may be reduced. Thus, by selecting the size, shape and position of the additional channel(s) appropriately and with due consideration to the coefficients of thermal expansion of the first and second materials as well as the size, shape and position of the flow channel(s), it is possible to control the amount of material entering the flow channel(s) when the ambient temperature increases, and thereby it is possible to control the resulting increase in flow resistance.
The corresponding change(s) in the flow channel(s) may comprise a change in a cross sectional area of at least one of the flow channel(s) and/or it may comprise a change in a shape of at least one of the flow channel(s). This has already been described above.
The specified temperature interval preferably comprises temperatures at which it is likely that the flow system will be used. Thus, it preferably comprises temperatures which would be experienced under normal conditions, such as room temperature/indoor temperature as well as outdoor temperatures at which it is likely that the flow system will be used. Thus, the specified temperature range may be −15° C. to 50° C., such as 0° C. to 30° C., such as 10° C. to 25° C., or any other suitable temperature interval.
At least the at least one section of the flow channel(s) may be or comprise a flow restriction. This may, e.g., be in the form of a capillary tube or another kind of tube having a section with a smaller cross sectional area than the remaining part of the tube. Such a flow restriction is preferably in the form of a channel and forms part of the flow system. The flow restriction may have any suitable geometry, including a square, a rectangular, a triangular, a circular, an oval or any other suitably shaped cross section.
The first coefficient of thermal expansion and/or the second coefficient of thermal expansion may be within the range 10−6 per ° C. to 10−3 per ° C., such as within the range 10−5 per ° C. to 10−4 per ° C. However, as mentioned above, in order to obtain the desired effect, the first coefficient of thermal expansion and the second coefficient of thermal expansion should not be identical or even similar. In case the first or second material is the polystyrene material known as PS158K manufactured by BASF the coefficient of thermal expansion is approximately 0.8×10−4 per ° C.
According to a second aspect of the invention the above and other objects are fulfilled by providing a micro fluidic system comprising an inlet opening, an outlet opening and at least one flow system according to the first aspect of the invention.
It should be noted that a skilled person would readily recognise that any feature described in combination with the first aspect of the invention can also be combined with the second aspect of the invention, and vice versa.
In the present context the term ‘micro fluidic system’ should be interpreted to mean a system having dimensions which are sufficiently small to at least substantially prevent turbulence in a fluid flowing in the system.
The micro fluidic system may be or form part of a fluid analysis device, e.g. a medical device, such as a device for measuring a parameter of a body fluid, e.g. a concentration of blood glucose in a blood sample. In this case it is very desirable that the flow resistance of the micro fluidic system is at least substantially independent of the ambient temperature, at least within a specified temperature interval, since it is thereby ensured that the device operates in a reliable and consistent manner, even if the ambient temperature changes.
Alternatively, the micro fluidic system may be or form part of an infusion system or a drug delivery system, e.g. an insulin pump device.
The invention will now be further described with reference to the accompanying drawings in which
The material making up the first part 2 has a coefficient of thermal expansion which is higher than the coefficient of thermal expansion of the material making up the second part 3. Therefore, when the ambient temperature increases, the first part 2 would, in the absence of the second part 3, expand more than the second part 3. The difference between the coefficients of thermal expansion may be chosen in such a way that thermal expansion of the second part 3 is negligible as compared to thermal expansion of an isolated first part 2, and it may therefore be assumed that the second part 3 does not expand as the ambient temperature increases. Accordingly, it will not be possible for the material of the first part 2 to expand in the directions where the second part 3 abuts the first part 2. As a consequence, the thermal stress build-up in the first part 2 will result in closing up of the flow channel 4 and the additional channel 5. Thereby the size and/or the shape of the outer contour of the flow channel 4 is/are changed in such a way that the flow resistance of the flow channel 4 is increased.
Knowing the initial size/shape of the flow channel 4, the coefficients of thermal expansion of the first part 2 and the second part 3, as well as the temperature interval in which it is most likely that the flow system 1 will be used, it is possible to design the size, shape and position of the additional channel 5 in such a way that the increase in flow resistance caused by the thermal expansion of the first part 2 as described above at least substantially counter-balances the decrease in flow resistance caused by the increase in temperature of the fluid being transported by the flow system 1. Thereby it is obtained that the resulting flow resistance of the flow channel 4 is at least substantially constant even though the ambient temperature varies.
In the example of
Thus, in the example shown in
The material making up the first part 2 has a coefficient of thermal expansion which is lower than the coefficient of thermal expansion of the material making up the second part 3. The difference in the coefficients of thermal expansion may be sufficient to assume that thermal expansion of the first part 2 is negligible as compared to thermal expansion of an isolated second part 3 when the ambient temperature varies within a specific temperature interval. Thus, it may be assumed that the first part 2 does not undergo thermal expansion, and the first part 2 will thereby restrict the expansion of the material of the second part 3, similarly to the situation described above, but with the first 2 and second 3 parts in reverse ‘roles’.
When the ambient temperature increases the material of the second part 3 will attempt to expand. However, this expansion is restricted by the first part 2. The material of the portion 6 of the second part 3 which is positioned in the recess of the first part 2 will expand sideways, thereby introducing stress in the first part 2, at least in an area near the flow channel 4. This will cause the width of the first part 2 to increase, and, as a consequence, the height of the first part 2 is decreased as described by the theory of elasticity. Thereby the width of the flow channel 4 is increased, and the height of the flow channel 4 is decreased. This change in the dimensions of the flow channel 4 will cause an increase in the flow resistance of the flow channel 4. It should be noted that, in order to obtain this effect, the recess in the first part 2 should be positioned sufficiently close to the flow channel 4 to ensure that the sideways expansion of the portion 6 is transferred to the region near the flow channel 4.
Furthermore, the material of the portion 6 is prevented from expanding in a downwards direction due to the remaining portion of the second part 3. As a consequence, material from the portion 6 will push material from the first part 2, which is present between the portion 6 and the flow channel 4, into the flow channel 4, thereby further reducing the height of the flow channel 4. However, in most cases this effect will be less significant than the effect described above.
As it is the case with the embodiment shown in
In the embodiment of
As it is the case with the embodiments shown in
In the embodiment of
The embodiment of
In the embodiment shown in
In the embodiment of
In the embodiment of
It should be noted that various other designs of flow systems 1 could be envisaged, and that the embodiments shown in
Furthermore, it should be noted that when the ambient temperature decreases all of the mechanisms described above are reversed, i.e. the material having the highest coefficient of thermal expansion will contract and the flow resistance of the flow channel 4 will decrease. At the same time the viscosity of the fluid being transported in the flow system 1 increases as a consequence of the decrease in temperature, thereby increasing the flow resistance. Again, the two effects will at least substantially counter-balance each other.
The right part of
wherein L is the length of a flow restricting section of the flow channel 4, a is the coefficient of thermal expansion of the material making up the first part 2, and n is the viscosity of the fluid being transported in the flow channel 4. It has been assumed that the coefficient of thermal expansion of the second part (not shown) is zero, i.e. it has been assumed that the thermal expansion of the second part is negligible as compared to thermal expansion of the first part 2. This has been described above. Furthermore, as it appears from the Figure, B is the height of the flow channel 4, W is the width of the flow channel 4, d is the distance between the flow channel 4 and the additional channel 5, and D is the height of the first part 2.
In order to ensure that the flow resistance of the flow channel 4 is independent of the ambient temperature within a certain temperature range, the above equation should be equal to zero. Solving for D/d yields:
Using the following values:
B=20 mm
W=20 mm
a=5×10−4 K−1
n=0.89×10−3 Pa s
dn/dT=−0.0205×10−3 Pa s K−1
the above equation yields D/d=26.5. Thus, if the polymer chip has a thickness of 2 mm, d is given by 75.5 μm. Accordingly, the depth of the additional channel 5 is 1.90 mm. It should be noted that in the calculations performed above, effects arising from a lid of the first part 2, i.e. material positioned above the flow channel 4, are omitted. In order to take such effects into account, it may be assumed that ‘d’ in the above calculations represents an effective combined height of the lid and the portion of the first part 2 positioned between flow channel 4 and the additional channel 5.
The calculation above is an example of how it is possible to design the size, shape and position of the additional channel 5 in such a way that the changes in flow resistance caused by a change in viscosity due to a change in ambient temperature can be counteracted by a change in flow resistance caused by a change in the size and/or shape of the flow channel 4 due to the same change in ambient temperature. Thereby the additional channel 5 insures a passive calibration of the thermal expansion of the first part 2 into the flow channel 4 to give the desired flow resistance/temperature relation, the calibration being build into the system.
While the present invention has been illustrated and described with respect to a particular embodiment thereof, it should be appreciated by those of ordinary skill in the art that various modifications to this invention may be made without departing from the spirit and scope of the present invention.
| Number | Date | Country | Kind |
|---|---|---|---|
| PA 2005 01483 | Oct 2005 | DK | national |
This application is entitled to the benefit of and incorporates by reference essential subject matter disclosed in International Patent Application No. PCT/DK2006/000593 filed on Oct. 24, 2006 and Denmark Patent Application No. PA 2005 01483 filed Oct. 24, 2005.
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/DK2006/000593 | 10/24/2006 | WO | 00 | 9/17/2008 |
