The disclosure relates to apparatus and methods for metering and vaporizing fluids and in particular to a micro-fluidic device containing multiple micro-fluidic pumps and one or more vaporization heaters for vaporizing fluids provided by the micro-fluidic pumps.
Micro-fluidic devices are used to manipulate microscopic volumes of liquid inside micro-sized structures. Applications of such devices include precise liquid dispensing, drug delivery, point-of-care diagnostics, industrial and environmental monitoring and lab-on-a-chip devices. Lab-on-a-chip devices can provide advantages over conventional and non-micro-fluidic based techniques such as greater efficiency of chemical reagents, high speed analysis, high throughput, portability and low production costs per device. In many micro-fluidic applications such as liquid dispensing, point-of-care diagnostics or lab-on-a-chip, a role of the micro-fluidic pumps is to manipulate micro-volumes of liquids inside micro-channels.
Micro-fluidic pumps generally fall into two groups: mechanical pumps and non-mechanical pumps. Mechanical pumps use moving parts which exert pressure on a liquid to move a liquid from a supply source to a destination. Piezoelectric pumps, thermo-pneumatic pumps, and electro-osmotic pumps are included in this group. An electro-osmotic pump uses surface charges that spontaneously develop when a liquid contacts with a solid. When an electric field is applied, the space charges drag a body of the liquid in the direction of the electric field.
Another example of a non-mechanical pump is a pump exploiting thermal bubbles. By expanding and collapsing either a bubble with diffusers or bubbles in a coordinated way, a thermal bubble pump can transport liquid through a channel. Several types of thermal bubble pumps are known in the art.
Micro-fluidic bubble pumps are typically used to move micro quantities of fluid from a supply location to a destination so that a metered amount of liquid is delivered to the destination location. However, there is a need to deliver metered quantities of vaporized fluids from a supply location to a destination for various applications including vapor therapy, flavored e-cigarettes, chemical vapor reactions, and the like.
One problem with conventional bubble pumps is that the bubble pumps are limited by size and fluid flow constraints. Increasing the number of bubble pumps and the length of the bubble pumps increases the volume and pressure, respectively of liquid flowing out of the bubble pumps, and also increases the area required for dispensing liquids from the bubble pumps. For some applications, the size of the bubble pumps is critical. Accordingly, conventional bubble pumps may not be useful in a variety of applications that may require a small size with higher fluid pressures and/or increased fluid flow volumes.
In view of the foregoing, there is a need to provide a micro-fluidic vapor from a reduced size micro-fluidic ejection device. Accordingly, there is provided, in one embodiment, a micro-fluidic device. The device includes a semiconductor substrate attached to a fluid supply source. The substrate contains at least one vaporization heater, one or more bubble pumps for feeding fluid from the fluid supply source to the at least one vaporization heater, a fluid supply inlet from the fluid supply source in fluid flow communication with each of the one or more bubble pumps, and a vapor outlet in vapor flow communication with the at least one vaporization heater. The one or more bubble pumps each have a fluid flow path selected from a linear path, a spiral path, a circuitous path, and a combination thereof from the supply inlet to the at least one vaporization heater.
In another embodiment of the disclosure there is provided a method of vaporizing two or more fluids in micro-fluidic quantities. The method includes feeding two or more fluids to a micro-fluidic device that includes a semiconductor substrate attached to a fluid supply source. The substrate contains at least one vaporization heater, two or more bubble pumps for feeding fluid from the fluid supply source to the at least one vaporization heater, a fluid supply inlet from the fluid supply source in fluid flow communication with each of the two or more bubble pumps, and a vapor outlet in vapor flow communication with the at least one vaporization heater, wherein the two or more bubble pumps each have a fluid flow path selected from a linear path, a spiral path, a circuitous path, and a combination thereof from the supply inlet to the at least one vaporization heater. The two or more bubble pumps are energized to provide the two or more fluids to the at least one vaporization heater, the two or more fluids are vaporized with the at least one vaporization heater.
A further embodiment of the disclosure provides a method for reacting and vaporizing micro-fluidic quantities of two or more different fluids. The method includes providing a micro-fluidic device that contains a semiconductor substrate attached to two or more fluid supply sources. The substrate includes at least one vaporization heater, a bubble pump for feeding fluid from each of the two or more fluid supply sources to the at least one vaporization heater, a fluid supply inlet from each of the two or more fluid supply sources in fluid flow communication with each bubble pump, and a vapor outlet in vapor flow communication with the at least one vaporization heater, wherein each bubble pump has a fluid flow path selected from a linear path, a spiral path, a circuitous path, and a combination thereof from the supply inlet to the at least one vaporization heater. Each bubble pump is operated to provide the two or more different fluids to the at least one vaporization heater. The two or more fluids are reacted on the at least one vaporization heater to provide a reaction product, and the reaction product is vaporized with the at least one vaporization heater.
Accordingly, embodiments of the disclosure provide a compact micro-fluidic vaporizing device that may be used to mix and/or react and vaporize fluids for a variety of applications. The devices enable the pumping and vaporization of fluids at higher pressure than conventional devices and enable larger quantities of fluids to be vaporized without increasing the size of the device.
Further advantages of the embodiments will become apparent by reference to the detailed description of exemplary embodiments when considered in conjunction with the drawings, wherein like reference characters designate like or similar elements throughout the several drawings as follows:
Micro-fluid bubble pumps are miniature electronic devices that can be used to eject fluids onto surfaces. In the case of the present disclosure, the bubble pumps are used to provide pre-determined amounts of one or more fluids to at least one vaporization device in order to mix and/or react the fluids and provide a vaporized fluid. Vaporized fluids have application in a variety of devices including, but not limited to, vapor therapy, air fresheners, drug delivery, micro-scale laboratories on chips, e-cigarettes, and the like. In some embodiments, two or more different fluids are provided to a single vaporization device. In other embodiments, two or more fluids are provided to different vaporization devices. In yet other embodiments, a predetermined volume of a single fluid is provided to one or more vaporization devices. Increasing the volume or pressure of fluid or the use of two or more different fluids in a bubble pump and vaporization device typically requires an increase in the size of the device. However, embodiments of the disclosure may provide a unique bubble pump and vaporization device arrangement that enables minimization of the size of the device.
Pumping of fluids to a vaporization device using a micro-fluid bubble pump is achieved by supercritical heating of a fluid. While the supercritical temperature of a fluid is higher than the boiling point, only a thin layer of the liquid is involved in forming thermal vapor bubbles. For example, while the supercritical temperature of water is about 300° C., the thermal bubbles can be formed by heating less than 0.5 μm thick layer of water on top of a heater to the supercritical temperature for a few micro-seconds. Accordingly, less than one percent of the liquid may experience the supercritical temperature. The supercritical temperature of the fluid lasts for a few micro-seconds, hence the temperature of the bulk of the fluid will remain at an initial temperature of the fluid in the bubble pump. The thermal vapor bubble thus formed provides a high initial pressure of around 100 Atm. The pressure of the vapor bubble may be used to move fluid through the bubble pump from an inlet end thereof to a terminal end thereof.
In operation, a voltage pulse is applied to each of the heater resistors 20 in sequence generating thermal bubbles in a predetermined manner. For example, every resistor heater 20 can form a bubble from the left to the right in the channel 22 in sequence to push fluid in the same direction through the channel 22 from the fluid inlet via 26 to the vaporization heater 14. The voltage pulses may be continuous, in sequence from left to right, or may be reversed to move liquid from right to left in the channel 22. The direction of flow of fluid through the bubble pump 16 is determined by the sequence of resistor heaters 20 that are activated. In order to move liquid from one end of the channel 22 to the other end, after firing a resistor heater 20, the resistor heater is allowed to cool down before the next firing sequence in order to prevent overheating and boiling of liquid on the resistor heater 20.
The channel 22 together with a cover layer 28 form a closed channel for moving fluid therethrough. Unlike traditional thermal ink jet nozzle plates used for ejecting ink, the cover layer 28 here has no nozzle holes through which to eject fluid. Rather, the cover layer 28 retains the fluid in the channel 22 as bounded by walls of the channel and the cover layer 28. In this way, fluid is moved through the channel 22 according to a path of travel on from the fluid inlet via 26 to the vaporization heater 14 as defined by the channel 22. Fluid is only introduced into the channel 22 from a fluid inlet via 26 and the vaporized fluid exits from the channel through vapor outlet 30 in the cover layer 28. The size of the channel is determined by the fluid being pumped, the size of the resistor heaters 20 used to move the fluid and the vaporization rate of the fluid.
In another embodiment, shown in
In order to obtain a predetermined pumping rate of fluid with bubble pumps 16, with resistor heaters 20 of a predetermined size, the geometric relationships among the resistor heaters 20 and between adjacent heaters 20 and the channel 22 are important. For example, a ratio of the width of the channel (CW) to the length of the heaters (HL) may be in the range of 1.0 to 2.0. The spacing (HD) between two adjacent heaters may be in the range of 1.5 HW to 4 HW. For pumps out of these ranges, the pumping rates may be significantly reduced. For example, a pump with the spacing (HD) larger than 4 HW showed a low pumping rate of less than 0.1 μl/min at the condition whereas a pump with the spacing of 1.5 HW showed over 10 μl/min. The preferred ratio of CW to HL is 1.72 and the preferred spacing (HD) is 56 μm.
The size of a resistor heaters 20 determines the required energy per fire. For the pumps disclosed in herein, the length and width of each resistor heater 20 is in the range of 10 to 100 μm. The preferred length and width are 29 μm and 17 μm, respectively. In some embodiments, the resistor heater 20 lengths and widths may have dissimilar dimensions in a common channel 22. The resistor heaters 20 may alternatively have asymmetric spacing between adjacent heaters 20.
According to an embodiment of the disclosure, the pressure of fluid in the bubble pumps 16 may be increased, if required, by lengthening the bubble pump channels and increasing the number of resistor heaters in the channel. However, as stated above, since there is a preferred spacing between heater resistors in a channel for effective pumping, the only suitable alternative is to lengthen the channels. Lengthening the channels typically requires additional substrate area which may not be practical for the use of micro-fluidic devices in small structures such as e-cigarettes. While the size of the bubble pumps may also be reduced to reduce the size of the substrate, this solution may also be impractical since it reduces the amount of fluid that can be delivered to the vaporization heater.
For example, with reference to
With regard to
Accordingly, alternative embodiments for the arrangement of multiple bubble pumps and vaporization heater(s) on a substrate are illustrated schematically in
In
A further embodiment is illustrated in
Yet another embodiment of the disclosure provides bubble pumps (BP) having channels 58 with circuitous paths from the fluid supply (FS) to the vaporization heater 60 as shown in
With reference again to
The micro-fluidic device 10 according to embodiments of the disclosure may be operated by firing resistor heaters 20 inside the channels 22 in sequence. After the last resistor heater 20 in the channel 22 is fired, the cycle repeats, starting again from the resistor heater 22 closest to the fluid inlet via 26. In principle, when a bubble grows on a resistor heater 20, the previously generated bubble needs to block the channel effectively and prevent the liquid from flowing back in the opposition direction of the resistor heater firing sequence. Two delays may be considered to optimize the performance of the pump. After one resistor heater is fired, a delay can be added before the next resistor heater is fired. It is called “fire-to-fire delay.” In addition, after a cycle is completed, and the vaporization heater 14 had been activated to vaporize the fluid, a delay may be inserted before the next pumping cycle is started. This delay is called “cycle-to-cycle delay.” These two delays and the width of the fire pulse may be controlled by manipulating a fire signal to the resistor heaters 20. When one resistor heater 20 is activated, the width of the fire pulse is designate tfire. On the other hand, tfire-to-fire delay is a time delay between activating two adjacent resistor heaters 20 with a firing pulse tfire. A duty cycle of the tfire-to-fire delay may range from about 50% to about 90. In other embodiments, the activation of one resistor heater 20 may be accomplished with a split firing pulse having a first pulse width sufficient to “warm up” the resistor heater and a second pulse width sufficient to actually nucleate a bubble of fluid. Other resistor heater 20 firing schemes as possible. A time delay between two firing cycles is designated tcycle-to-cycle delay.
It is contemplated, and will be apparent to those skilled in the art from the preceding description and the accompanying drawings, that modifications and changes may be made in the embodiments of the disclosure. Accordingly, it is expressly intended that the foregoing description and the accompanying drawings are illustrative of exemplary embodiments only, not limiting thereto, and that the true spirit and scope of the present disclosure be determined by reference to the appended claims.