US20140076519A1 - Methods for Stabilizing Flow in Channels and System Thereof - Google Patents

Abstract

A method and system for stabilizing flow includes introducing a flow into a channel with a minimum cross-sectional dimension of less than three millimeters and triggering a release of one or more bubbles in the flow at one or more locations in the channel. The one or more locations are spaced in from an inlet and an outlet to the channel.

Description

• This application is a divisional of U.S. patent application Ser. No. 12/497,180, filed Jul. 2, 2009, which is a divisional of U.S. patent application Ser. No. 10/939,896, filed Sep. 13, 2004, now U.S. Pat. No. 7,575,046, which claims the benefit of U.S. Provisional Patent Application Ser. No. 60/504,267, filed Sep. 18, 2003, which are hereby incorporated by reference in their entirety.
FIELD OF THE INVENTION
• The present invention generally relates to microchannels and minichannels and, more particularly, to methods and systems for stabilizing flow and/or improving heat transfer performance in microchannels and minichannels and systems thereof.
BACKGROUND
• In a cooling system with a network of multiple parallel microchannels and minichannels, each having a hydraulic diameter less than three mm, a liquid used for cooling is introduced. As the liquid flows through the network, initially heat transfer is by convection from the walls of the microchannels and minichannels.
• As the liquid flows further downstream through the network, additional heating of the liquid occurs. Eventually, the wall temperature of the microchannels and minichannels rises above the local saturation temperature of the liquid. However, boiling of the liquid does not occur unless there are proper nucleation cavities present. If one or more nucleation cavities are present, nucleation occurs over the nucleation cavity or cavities and the liquid boils. The range of possible nucleation cavities in the microchannels and minichannels can be expanded by the application of a sufficiently high degree of superheat to the microchannels and minichannels.
• Prior to this nucleation occurring and during the superheating, the liquid in the microchannels and minichannels, at least in the vicinity of the nucleation sites, becomes superheated. At this point, a bubble present or formed in this liquid experiences a very rapid bubble growth. The rapid bubble growth leads to severe pressure fluctuation in the microchannel or minichannel, which can result in a reverse flow of the liquid. Experimental evidence and a description of the mechanism leading to this instability is described in Kandlikar, S. G. “Heat Transfer Mechanisms During Flow Boiling In Microchannels.” Proceedings of the First International Conference on Microchannels and Minichannels Apr. 24-25, 2003, Rochester, N.Y., USA ICMM2003-1005, S. G. Kandlikar, Editor ASME Publication, 2003, which is herein incorporated by reference in its entirety. The rapid bubble growth may also adversely affect the heat transfer performance, including heat transfer degradation and/or reduction in critical heat flux, of the cooling system.
SUMMARY OF THE INVENTION
• A method for stabilizing flow during flow boiling in accordance with embodiments of the present invention includes introducing a flow into a channel with a minimum cross-sectional dimension of less than three millimeters and triggering a release of one or more bubbles in the flow at one or more locations in the channel to stabilize the flow. The one or more locations are spaced in from an inlet and an outlet to the channel.
• A system for stabilizing flow during flow boiling in accordance with embodiments of the present invention includes the channel and the triggering system. The channel has a minimum cross-sectional dimension of less than three millimeters. The triggering system triggers a release of one or more bubbles in the flow at one or more locations in the channel to stabilize the flow. The one or more locations are spaced in from an inlet and an outlet to the channel.
• The present invention provides a method and system for the efficient removal of the heat potential of flow boiling in a channel or channels, such as microchannels and minichannels. The present invention overcomes the severe oscillatory nature of the flow during flow boiling by initiating the nucleation and flow boiling at specific locations in the channel or channels. The locations are chosen such that the local superheat in the wall and/or surrounding liquid is relatively low and does not lead to the rapid bubble growth that leads to flow and pressure oscillations. Flow and pressure oscillations can lead to flow reversal and premature drying out and to a reduction in cooling performance. To assist in initiating nucleation the present invention heats a region with or immediately preceding a location with nucleation cavities. To provide additional flow stability the present invention may also incorporate local pressure reduction devices.
BRIEF DESCRIPTION OF THE DRAWINGS
• FIG. 1 is a cross-sectional view of a system with a low pressure zone for stabilizing flow which is flowing from left to right in a microchannel or minichannel in accordance with embodiments of the present invention;
• FIGS. 2A and 2B are cross-sectional views of systems with a low pressure zone for stabilizing flow which is flowing from left to right in a microchannel or minichannel in accordance with other embodiments of the present invention;
• FIG. 3 is a cross-sectional view of the system shown inFIG. 1 with a heater and with a flow direction from left to right in accordance with other embodiments of the present invention;
• FIGS. 4A and 4B are cross-sectional views of the systems with a low pressure zone as shown inFIGS. 2A and 2B respectively with nucleation cavities and with a flow direction from left to right in accordance with other embodiments of the present invention;
• FIG. 5 is a cross-sectional view of a system with nucleation cavities for stabilizing flow in a microchannel or minichannel along one surface in accordance with other embodiments of the present invention;
• FIG. 6 is a cross-sectional view of a system with nucleation cavities for stabilizing flow in a microchannel or minichannel in a systematic or random pattern in accordance with other embodiments of the present invention;
• FIG. 7 is a cross-sectional view of a system with a low pressure zone and nucleation cavities for stabilizing flow in a microchannel or minichannel in accordance with embodiments of the present invention; and
• FIG. 8 is a cross-sectional view of a system for stabilizing flow in a microchannel or minichannel in a systematic or random pattern with a heater in accordance with other embodiments of the present invention.
DETAILED DESCRIPTION
• Systems10(1)-10(10) for stabilizing flow F in one or more channels12(1)-12(10) in accordance with embodiments of the present invention are illustrated inFIGS. 1-8. The systems10(1)-10(10) each have a channel12(1)-12(10) which each includes one or more low pressure devices14(1)-14(3), low pressure zones16(1)-16(4), heating device18(1)-18(2), and/or nucleation cavities20(1)-20(7), although the systems10(1)-10(10) each can include other types and numbers of elements arranged in other manners. The present invention provides a number of advantages including providing systems and methods for efficiently removing the heat potential of flow boiling in microchannels and minichannels. The present invention overcomes the severe oscillatory nature of the flow F during flow boiling by initiating the nucleation and flow boiling at specific locations in the channel or channels. The locations are chosen such that the local superheat in the wall of the channel or channels and/or surrounding flow is relatively low and does not lead to the rapid growth of bubbles that lead to flow and pressure oscillations.
• Referring more specifically toFIGS. 1-8, each of the channels12(1)-12(10) is either a minichannel or a microchannel. A minichannel has a minimum cross-sectional dimension between about 200 microns to three millimeters and a microchannel has a minimum dimension of about 200 microns or less. The cross-sectional dimension is measured across the channel in a direction which is substantially perpendicular to the direction of the flow. Although hydraulic diameter is described in, Kandlikar, S. G. “Heat Transfer Mechanisms During Flow Boiling In Microchannels.” Proceedings of the First International Conference on Microchannels and Minichannels Apr. 24-25, 2003, Rochester, N.Y., USA ICMM2003-1005, S. G. Kandlikar, Editor ASME Publication, 2003, the above classification is used for microchannels and minichannels herein. In these embodiments, the channels12(1)-12(10) each have a circular, cross-sectional shape, although each of the channels12(1)-12(10) could have other cross-sectional shapes. The arrow F represents the flow flowing in the channels12(1)-12(10) and also indicates the direction of that flow. A variety of different types of flow F, such as fluids, can pass through the channels12(1)-12(10) and the flow F can go in other directions.
• Referring toFIG. 1, the system10(1) for stabilizing flow F includes the channel12(1) with the low pressure device14(1), although system10(1) can include other types and numbers of elements arranged in other manners. The flow F is a liquid in this and the other systems10(1)-10(10) described herein, although other types of mediums can be used for the flow F. The channel12(1) has a wall which defines a passage22(1) that is substantially straight and includes an inlet24(1) and an outlet26(1), although the channel12(1) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• The low pressure device14(1) is positioned in the channel12(1) and is spaced in from the inlet24(1) and the outlet26(1), although other numbers and types of pressure drop elements in other locations can be used. A pressure drop element, such as pressure device14(1) refers to any element or configuration that creates a pressure drop, flashing, increased resistance to backflow, and/or creation of a low pressure zone. The flashing leads to the presence of vapor phase in the flow which prevents any further superheating of the wall and/or the flow F. Excess superheat is the cause for rapid bubble growth that leads to instability in the flow F.
• The low pressure device14(1) extends fully or partially around the inner periphery of the channel12(1) and forms a high pressure region28(1) upstream of the low pressure device14(1) and forms a low pressure region30(1) downstream of the low pressure device14(1). A passage32(1) extends through the low pressure device14(1) to connect the high pressure region28(1) to the low pressure region30(1). The passage32(1) has a cone-shaped, inner periphery with the larger opening to this cone-shaped, inner periphery facing the high pressure region28(1), although the passage32(1) could have other shapes and configurations.
• Referring toFIG. 2A, the system10(2) for stabilizing flow F includes the channel12(2) with the low pressure zone16(1), although system10(2) can include other types and numbers of elements arranged in other manners. Elements inFIG. 2A which correspond to those described with reference toFIG. 1 will have like reference numerals. The channel12(2) has a wall which defines a passage22(2) that has a high pressure region28(2) which is narrower than and upstream from a low pressure region30(2). The passage22(2) also includes an inlet24(2) and an outlet26(2), although the channel12(2) and passage22(2) could have other configurations with other numbers, shapes, and types of regions and other numbers of walls and openings. The low pressure zone16(1) is adjacent the transition from the high pressure region28(2) to the low pressure region30(2). A passage32(2) connects the high pressure region28(2) to the low pressure region30(2).
• Referring toFIG. 2B, the system10(3) for stabilizing flow F includes the channel12(3) with the low pressure zone16(2), although system10(3) can include other types and numbers of elements arranged in other manners. Elements inFIG. 2B which correspond to those described with reference toFIGS. 1 and 2A will have like reference numerals. The channel12(3) has a wall which defines a passage22(3) that has a high pressure region28(3) which is wider than and upstream from a low pressure region30(3). The passage22(3) also includes an inlet24(3) and an outlet26(3), although the channel12(3) and passage22(3) could have other configurations with other numbers, shapes, and types of regions and other numbers of walls and openings. The low pressure zone16(2) is adjacent the transition from the high pressure region28(3) to the low pressure region30(3). A passage32(3) connects the high pressure region28(2) to the low pressure region30(2).
• Referring toFIG. 3, the system10(4) for stabilizing flow F includes the channel12(4) with the low pressure device14(2), the heating device18(1) and the nucleation cavities20(1), although system10(4) can include other types and numbers of elements arranged in other manners. Elements inFIG. 3 which correspond to those described with reference toFIGS. 1-2B will have like reference numerals. The channel12(4) has a wall which defines a passage22(4) that is substantially straight and includes an inlet24(4) and an outlet26(4), although the channel12(4) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• The low pressure device14(2) is positioned in the channel12(4) and is spaced in from the inlet24(4) and the outlet26(4), although other numbers and types of pressure drop elements in other locations can be used as described earlier. The low pressure device14(2) extends fully or partially around the inner periphery of the channel12(4) and forms a high pressure region28(4) upstream of the low pressure device14(2) and forms a low pressure region30(4) downstream of the low pressure device14(2). A passage32(4) extends through the low pressure device14(2) to connect the high pressure region28(4) to the low pressure region30(4). The passage32(4) has a cone-shaped, inner periphery with the larger opening to this cone-shaped, inner periphery facing the high pressure region28(4), although the passage32(4) could have other shapes and configurations.
• The heating device18(1) is positioned around the wall of the channel22(4) adjacent the low pressure device14(2) and is used to superheat the adjacent portion of the channel, although other numbers and types of heating systems in other locations could be used. The heating device18(1) is also positioned over nucleation cavities20(1) which are located in the wall of the channel22(4), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(1) is based on the geometry of the channel22(4) and the range of flow conditions that the channel22(4) is subject to.
• Referring toFIG. 4A, the system10(5) for stabilizing flow F includes the channel12(5) with the low pressure zone16(3), although system10(5) can include other types and numbers of elements arranged in other manners. Elements inFIG. 4A which correspond to those described with reference toFIGS. 1-3 will have like reference numerals. The channel12(5) has a wall which defines a passage22(5) that has a high pressure region28(5) which is narrower than and upstream from a low pressure region30(5). The passage22(5) also includes an inlet24(5) and an outlet26(5), although the channel12(5) and passage22(5) could have other configurations with other numbers, shapes, and types of regions and other numbers of walls and openings. The low pressure zone16(3) is adjacent the transition from the high pressure region28(5) to the low pressure region30(5). A passage32(5) connects the high pressure region28(5) to the low pressure region30(5).
• Nucleation cavities20(2) are located in the wall of the channel22(5) adjacent the low pressure zone16(3), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(2) is based on the geometry of the channel22(5) and the range of flow conditions that the channel22(5) is subject to.
• Referring toFIG. 4B, the system10(6) for stabilizing flow F includes the channel12(6) with the low pressure zone16(4), although system10(6) can include other types and numbers of elements arranged in other manners. Elements inFIG. 4B which correspond to those described with reference toFIGS. 1-4A will have like reference numerals. The channel12(6) has a wall which defines a passage22(6) that has a high pressure region28(6) which is wider than and upstream from a low pressure region30(6). The passage22(6) also includes an inlet24(6) and an outlet26(6), although the channel12(6) and passage22(6) could have other configurations with other numbers, shapes, and types of regions and other numbers of walls and openings. The low pressure zone16(4) is adjacent the transition from the high pressure region28(6) to the low pressure region30(6). A passage32(6) connects the high pressure region28(6) to the low pressure region30(6).
• Nucleation cavities20(3) are located in the wall of the channel22(6) adjacent the low pressure zone16(4), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(3) is based on the geometry of the channel22(6) and the range of flow conditions that the channel22(6) is subject to.
• Referring toFIG. 5, the system10(7) for stabilizing flow F includes the channel12(7) with nucleation cavities20(4), although system10(7) can include other types and numbers of elements arranged in other manners. Elements inFIG. 5 which correspond to those described with reference toFIGS. 1-4B will have like reference numerals. The channel12(7) has a wall which defines a passage22(7) that is substantially straight and includes an inlet24(7) and an outlet26(7), although the channel12(7) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• Nucleation cavities20(4) are spaced apart substantially the same distance along a section of the wall of the channel22(7), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(4) is based on the geometry of the channel22(7) and the range of flow conditions that the channel22(7) is subject to.
• Referring toFIG. 6, the system10(8) for stabilizing flow F includes the channel12(8) with nucleation cavities20(5), although system10(8) can include other types and numbers of elements arranged in other manners. Elements inFIG. 6 which correspond to those described with reference toFIGS. 1-5 will have like reference numerals. The channel12(8) has a wall which defines a passage22(8) that is substantially straight and includes an inlet24(8) and an outlet26(8), although the channel12(8) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• Nucleation cavities20(5) are randomly located along a section of the wall of the channel22(8), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(5) is based on the geometry of the channel22(8) and the range of flow conditions that the channel22(8) is subject to.
• Referring toFIG. 7, the system10(9) for stabilizing flow F includes the channel12(9) with the low pressure device14(3) and nucleation cavities20(6), although system10(9) can include other types and numbers of elements arranged in other manners. Elements inFIG. 7 which correspond to those described with reference toFIGS. 1-6 will have like reference numerals. The channel12(9) has a wall which defines a passage22(9) that is substantially straight and includes an inlet24(9) and an outlet26(9), although the channel12(9) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• The low pressure device14(3) is positioned in the channel12(9) and is spaced in from the inlet24(9) and the outlet26(9), although other numbers and types of pressure drop elements in other locations can be used as described earlier. The low pressure device14(3) extends fully or partially around the inner periphery of the channel12(9) and forms a high pressure region28(7) upstream of the low pressure device14(3) and forms a low pressure region30(7) downstream of the low pressure device14(3). A passage32(7) extends through the low pressure device14(3) to connect the high pressure region28(7) to the low pressure region30(7). The passage32(7) has a cone-shaped, inner periphery with the larger opening to this cone-shaped, inner periphery facing the high pressure region28(7), although the passage32(7) could have other shapes and configurations.
• Nucleation cavities20(6) are spaced apart substantially the same distance along a section of the wall of the channel22(9), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(6) is based on the geometry of the channel22(9) and the range of flow conditions that the channel22(9) is subject to.
• Referring toFIG. 8, the system10(10) for stabilizing flow F includes the channel12(10) the heating device18(2) and the nucleation cavities20(7), although system10(10) can include other types and numbers of elements arranged in other manners. Elements inFIG. 8 which correspond to those described with reference toFIGS. 1-7 will have like reference numerals. The channel12(10) has a wall which defines a passage22(10) that is substantially straight and includes an inlet24(10) and an outlet26(10), although the channel12(10) could have other configurations, such as a curved shape, and other numbers of walls and openings.
• The heating device18(2) is positioned around the wall of the channel12(10) adjacent the nucleation cavities20(7), although other numbers and types of heating systems in other locations could be used.
• Nucleation cavities20(7) are randomly located along a section of the wall of the channel22(10), although other numbers and locations for the nucleation cavities and other types of reentrant or nucleation sites can be used. The actual size and shape of the nucleation cavities20(7) is based on the geometry of the channel22(10) and the range of flow conditions that the channel22(10) is subject to.
• With the systems10(1)-10(10) described above, the instability in the flow F is reduced and performance improvement is achieved by triggering an earlier nucleation in the flow F. The triggered early nucleation in the systems10(1)-10(10) results in smaller vapor bubbles or slugs that are separated by relatively uniform liquid slugs and that do not grow too rapidly. The smaller vapor bubbles or slugs improve the heat transfer performance in the systems10(1)-10(10) because the liquid film of the small vapor bubbles or slugs covering the wall or walls in the channels12(1)-12(10) does not completely evaporate and is able to transfer heat before leaving the region. As a result, degradation in the cooling performance of systems10(1)-10(10) is avoided.
• The rapid growth of bubbles leads to reversed flow of vapor into an inlet manifold coupled to one or more of the channels12(1)-12(10). This leads to flow instabilities and flow maldistribution in parallel channels.
• The process of nucleation depends on the availability of nucleation cavities of the right size and shape which satisfy the nucleation criteria as described in an equation proposed by Hsu and Graham, rewritten in the following form by Kandlikar (Handbook of Phase Change, Taylor and Francis, 1999, which is herein incorporated by reference in its entirety) has the following form, and it provides the cavity radii range that can nucleate under a given set of local conditions. This equation, referred to asEquation 1 or eq. 1 herein, is as follows:
• $r_{\max }^{*},r_{\min }^{*}=\frac{1}{2}\left[\frac{\Delta T_{\mathrm{sat}}^{*}}{\Delta T_{\mathrm{sat}}^{*}+\Delta T_{\mathrm{sub}}^{*}}\pm \sqrt{{\left(\frac{\Delta T_{\mathrm{sat}}^{*}}{\Delta T_{\mathrm{sat}}^{*}+\Delta T_{\mathrm{sub}}^{*}}\right)}^2-\frac{1}{\left(\Delta T_{\mathrm{sat}}^{*}+\Delta T_{\mathrm{sub}}^{*}\right)}}\right]$
• where
• 
  r*=r/δ_t
• 
  ΔT*_sat=ΔT_sath_lvδ_t/(8σT_satv_lv)
• 
  ΔT*_sub=ΔT_subh_lvδ_t/(8σT_satv_lv)
• r—cavity mouth radius,
• δ_t—thickness of the thermal boundary layer, approximately=h/k, where h is the single phase heat transfer coefficient prior to nucleation and k is the thermal conductivity of liquid
• ΔT_sat—wall superheat, degree C.
• h_lv—latent heat, J/kg
• σ—surface tension, N/m
• T_sat—saturation temperature, K
• v_lv—change in specific volume during evaporation, m³/kg
• ΔT_sub—local liquid subcooling, degree C.
• r_maxand r_minare the non-dimensional minimum and maximum cavity mouth radii that will nucleate according to criteria described in eq. (1). A number of modifications to the above criteria are available, such as having the temperature at the tip of the bubble protruding in the flow F to be at least equal to or higher than the saturation temperature. The nucleation criterion is also modified for a channel or channels that are not uniform over the circumference, such as a channel or channels with rectangular cross-section, and for a channel or channels where the local wall and flow temperature fields vary with circumferential location.
• The operation of the system10(1) for stabilizing flow F will be described with reference toFIG. 1. The location where the wall and/or the flow F is expected to be slightly superheated (within a few degrees), such that flashing occurs, may be identified. The low pressure device14(1) can be positioned in the channel12(1) before that location and spaced in from the inlet24(1) and outlet26(1) to the channel12(1).
• Next, the flow F enters the inlet24(1) to the channel12(1) and flows from the high pressure region28(1) to the low pressure region30(1) through the passage32(1) in the low pressure device14(1). The flow F heading towards the low pressure device14(1) is kept in single phase flow by insulating the inner surface of the channel12(1) so that nucleation or two-phase flow does not occur prior to passing through the low pressure device14(1). The heat gain in the high pressure region28(1) of the channel12(1) is also controlled to keep the flow F from boiling.
• The low pressure zone upstream from and adjacent to the low pressure device14(1) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(1) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(1) resulting in improved heat transfer characteristics when compared with prior systems. The low pressure device14(1) also increases the resistance to backflow in the channel12(1) to provide further flow stability.
• In the system10(1), a release of bubbles can also optionally be obtained by vibrating the flow in at least a portion of the channel12(1). A variety of different types of systems and device could be used to vibrate the flow F in the channel, such as a vibrating device disposed in a portion of the flow F in the channel12(1) or the walls of the channel12(1).
• The operation of the system10(2) for stabilizing flow F will be described with reference toFIG. 2A. The operation of the system10(2) is the same as the system10(1), except as described herein. The flow F enters the inlet24(2) to the channel12(2) and flows from the high pressure region28(2) to the low pressure region30(2) through the passage32(2). The low pressure zone upstream from and adjacent to the transition from the high pressure region28(2) to the low pressure region30(2) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(2) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(2) resulting in improved heat transfer characteristics when compared with prior systems. This configuration of the channel12(2) with the high pressure region28(2) of the channel being narrower than the low pressure region30(2) also increases the resistance to backflow in the channel12(2) to provide further flow stability.
• The operation of the system10(3) for stabilizing flow F will be described with reference toFIG. 2B. The operation of the system10(3) is the same as the system10(2), except as described herein. The flow F enters the inlet24(3) to the channel12(3) and flows from the high pressure region28(3) to the low pressure region30(3) through the passage32(3). The low pressure zone upstream from and adjacent to the transition from the high pressure region28(3) to the low pressure region30(3) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(3) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(3) resulting in improved heat transfer characteristics when compared with prior systems. This configuration of the channel12(3) with the high pressure region28(3) of the channel being narrower than the low pressure region30(3) also increases the resistance to backflow in the channel12(3) to provide further flow stability.
• The operation of the system10(4) for stabilizing flow F will be described with reference toFIG. 3. The operation of the system10(4) is the same as the system10(1), except as described herein. Again, the location where the wall and/or the flow F is expected to be slightly superheated (within a few degrees), such that flashing occurs, may be identified. The low pressure device14(2) can be positioned in the channel12(4) before that location and spaced in from the inlet24(4) and outlet26(4) to the channel12(4).
• Nucleation cavities20(1) are formed in the wall of the channel12(4) at a location where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(1), but is not large enough to create modest or severe instability in the flow F due to late nucleation. The mouth opening to at least some of nucleation cavities20(1) fall within those prescribed by eq. (1) described earlier herein. A larger range of diameters for nucleation cavities20(1) may be placed individually or in clusters at the desired locations to allow for slight departures from eq. (1) due to variations in fluid properties and to allow for uncertainties and other assumptions made (including uniform heat transfer coefficient over the perimeter) in deriving eq. (1) and to allow for a range of operating conditions, including flow rates, heat fluxes, operating pressure, and inlet conditions. The nucleation cavities20(1) can be fabricated using a variety of different techniques, such as laser drilling, etching, deep ion etching, laser ablation, sintering, scraping and fin bending, roughness, or indentation. The heating device18(1) is positioned around the channel12(4) adjacent the location of the nucleation cavities20(1). The nucleation cavities20(1) can also have different sizes and shapes to initiate nucleation under different conditions and at different locations.
• Once the system10(4) is formed, the flow F enters the inlet24(4) to the channel12(4) and flows from the high pressure region28(4) to the low pressure region30(4) through the passage32(4) in the low pressure device14(2). The heating device18(1) heats the wall of the channel adjacent the location of the nucleation cavities20(1). Heating the nucleation cavities20(1) helps to initiate nucleation in the flow F. The heating device18(1) could be supplied with essentially constant power or with power pulses to release bubbles over the nucleation cavities20(1) periodically to initiate boiling and reduce the level of superheat attained by the flow F. The period of bubble release is determined so that the pressure oscillations in the flow F are reduced to prevent flow reversal or other detrimental effects of large superheat buildup prior to nucleation. Although a heating device18(1) is shown, other mechanisms for bubble release can be used, such as mechanisms which use vibrations, laser light, and/or ultrasound.
• The low pressure zone upstream from and adjacent to the low pressure device14(2) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This nucleation and flashing prevents any further superheating of the wall of the channel12(4) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(4) resulting in improved heat transfer characteristics when compared with prior systems. The low pressure device14(2) also increases the resistance to backflow in the channel12(4) to provide further flow stability.
• The operation of the system10(5) for stabilizing flow F will be described with reference toFIG. 4A. The operation of the system10(5) is the same as the system10(2), except as described herein. As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(2) are formed in the wall of the channel12(5) at a location where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(2), but is not large enough to create modest or severe instability in the flow F due to late nucleation.
• The flow F enters the inlet24(5) to the channel12(5) and flows from the high pressure region28(5) to the low pressure region30(5) through the passage32(5). The low pressure zone upstream from and adjacent to the transition from the high pressure region28(5) to the low pressure region30(5) along with the nucleation at the nucleation cavities20(2) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(5) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(5) resulting in improved heat transfer characteristics when compared with prior systems. This configuration of the channel12(5) with the high pressure region28(5) of the channel being narrower than the low pressure region30(5) also increases the resistance to backflow in the channel12(5) to provide further flow stability.
• The operation of the system10(6) for stabilizing flow F will be described with reference toFIG. 4B. The operation of the system10(6) is the same as the system10(3), except as described herein. As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(3) are formed in the wall of the channel12(6) at a location where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(3), but is not large enough to create modest or severe instability in the flow F due to late nucleation
• The flow F enters the inlet24(6) to the channel12(6) and flows from the high pressure region28(6) to the low pressure region30(6) through the passage32(6). The low pressure zone upstream from and adjacent to the transition from the high pressure region28(6) to the low pressure region30(6) along with the nucleation at the nucleation cavities20(3) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(6) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(6) resulting in improved heat transfer characteristics when compared with prior systems. This configuration of the channel12(6) with the high pressure region28(6) of the channel being narrower than the low pressure region30(6) also increases the resistance to backflow in the channel12(6) to provide further flow stability.
• The operation of the system10(7) for stabilizing flow F will be described with reference toFIG. 5. The operation of the system10(7) is the same as the system10(4), except as described herein. As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(4) are formed in a substantially uniform pattern along a section of the wall of the channel12(7) where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(4), but is not large enough to create modest or severe instability in the flow F due to late nucleation.
• Once the system10(7) is formed, the flow F enters the inlet24(7) and flows through the channel12(7). The nucleation cavities20(4) initiate nucleation in the flow F. This nucleation prevents any further superheating of the wall of the channel12(7) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(7) resulting in improved heat transfer characteristics when compared with prior systems.
• The operation of the system10(8) for stabilizing flow F will be described with reference toFIG. 6. The operation of the system10(8) is the same as the system10(7), except as described herein. As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(5) are formed in a random pattern along a section of the wall of the channel12(8) where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(5), but is not large enough to create modest or severe instability in the flow F due to late nucleation.
• Once the system10(8) is formed, the flow F enters the inlet24(8) and flows through the channel12(8). The nucleation cavities20(5) initiate nucleation in the flow F. This nucleation prevents any further superheating of the wall of the channel12(8) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(8) resulting in improved heat transfer characteristics when compared with prior systems.
• The operation of the system10(9) for stabilizing flow F will be described with reference toFIG. 7. The operation of the system10(9) is the same as the system10(1), except as described herein. The location where the wall and/or the flow F is expected to be slightly superheated (within a few degrees), such that flashing occurs, may be identified. The low pressure device14(3) can be positioned in the channel12(9) before that location and spaced in from the inlet24(9) and outlet26(9) to the channel12(9).
• As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(6) are formed in a substantially uniform pattern along a section of the wall of the channel12(9) where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(6), but is not large enough to create modest or severe instability in the flow F due to late nucleation.
• Next, the flow F enters the inlet24(9) to the channel12(9) and flows from the high pressure region28(7) to the low pressure region30(7) through the passage32(7) in the low pressure device14(3). The low pressure zone upstream from and adjacent to the low pressure device14(3) along with the nucleation at the nucleation cavities20(6) triggers flashing to occur which leads to the presence of vapor phase, i.e. bubbles, in the flow F. This prevents any further superheating of the wall of the channel12(9) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(9) resulting in improved heat transfer characteristics when compared with prior systems. The low pressure device14(1) also increases the resistance to backflow in the channel12(9) to provide further flow stability.
• The operation of the system10(10) for stabilizing flow F will be described with reference toFIG. 8. The operation of the system10(10) is the same as the system10(4), except as described herein. As described in greater detail with reference to the nucleation cavities20(1) in system10(4), nucleation cavities20(7) are formed in a random pattern along a section of the wall of the channel12(10) where the superheat of the flow F is moderate to initiate nucleation over the nucleation cavities20(7), but is not large enough to create modest or severe instability in the flow F due to late nucleation. The heating device18(2) is positioned around the channel12(10) adjacent the location of the nucleation cavities20(7).
• Once the system10(10) is formed, the flow F enters the inlet24(10) and flows through the channel12(10). The heating device18(2) heats the wall of the channel adjacent the location of the nucleation cavities20(7). Heating the nucleation cavities20(7) helps to initiate nucleation in the flow F. This nucleation prevents any further superheating of the wall of the channel12(10) and/or flow F. The flow F with the bubbles is able to effectively transfer heat to the flow F through the wall of the channel12(10) resulting in improved heat transfer characteristics when compared with prior systems.
• Another way for improving heat transfer performance and stability in systems, such as system10(1)-10(10) involves the use of dissolved gases in the flow F. The dissolved gases helps in early nucleation and thereby limit the superheat of the flow F and bubble growth rate after bubble formation. The flow F containing dissolved gases can be used either alone with naturally occurring nucleation cavities or can be used in conjunction with other embodiments described herein. The dissolved gases form bubbles that attach on the wall of the channel and/or are in the flow F thus effectively creating interfaces between liquid and gas or gas vapor mixture where evaporation can occur at relatively low liquid and/or wall superheats.
• Yet another way for improving heat transfer performance and stability involves the introduction of microbubbles in the flow F. The microbubbles may be made of gases that are not soluble, or have limited solubility in the liquid. Any technique for generation of microbubbles can be implemented. The presence of microbubbles limits the liquid superheat as the liquid evaporates at the bubble interface and limits this liquid superheat. The bubbles may attach on the wall and/or flow in the liquid thus effectively creating interfaces between liquid and gas or gas vapor mixture where evaporation can occur at relatively low liquid and/or wall superheats.
• The present invention provides methods and systems to stabilize the flow during flow boiling in a channel or channels. The systems10(1)-10(10) described herein are merely exemplary and other combinations of the teachings in each can be used. The present invention utilizes pressure reduction and/or strategically placed nucleation cavities to achieve flow boiling under stable and workable operating conditions. The present invention can be used during flow boiling in any channel or channels to achieve stable flow and efficient heat removal. The various methods and systems for stabilizing flow, such as the methods and systems which use low pressure zone(s), use one or more nucleation cavities, heat portions or all of the channel(s), introduce non-soluble gases, microbubbles, or higher volatile liquid, can each be combined with one or more of the other embodiments to provide further flow stability.
• Having thus described the basic concept of the invention, it will be rather apparent to those skilled in the art that the foregoing detailed disclosure is intended to be presented by way of example only, and is not limiting. Various alterations, improvements, and modifications will occur and are intended to those skilled in the art, though not expressly stated herein. These alterations, improvements, and modifications are intended to be suggested hereby, and are within the spirit and scope of the invention. Additionally, the recited order of processing elements or sequences, or the use of numbers, letters, or other designations therefor, is not intended to limit the claimed processes to any order except as may be specified in the claims. Accordingly, the invention is limited only by the following claims and equivalents thereto.

Claims (16)

What is claimed is:

1. A system for stabilizing flow during flow boiling, the system comprising:

at least one of a minichannel and a microchannel having channel walls between an inlet and an outlet defining a passage capable of receiving flow;

a high pressure region upstream from a transition to a low pressure region within the passage;

a low pressure zone within the passage adjacent the transition from the high pressure region to the low pressure region;

one or more nucleation cavities having a radius within a range which satisfies criteria for nucleation located in the wall of the channel adjacent the low pressure zone fashioned to trigger a release of one or more bubbles in the flow at one or more locations in the at least one of the minichannel and the microchannel that effectively transfer heat to the flow through the wall of the channel and increase resistance to backflow in the channel and stabilize the flow.

2. The system as set forth inclaim 1, further comprising a vibrating system adjacent the low pressure zone.

3. The system as set forth inclaim 1, further comprising a heating device adjacent the low pressure zone.

4. The system as set forth inclaim 2, further comprising a heating device adjacent the low pressure zone.

5. The system as set forth inclaim 1, wherein one or more of the criteria for nucleation are based on at least one of a geometry of the at least one of the minichannel and the microchannel and a range of conditions for the flow.

6. The system as set forth inclaim 1, further comprising at least one insulator upstream from the low pressure zone on at least a portion of an inner surface of the at least one of the minichannel and the microchannel.

7. The system as set forth inclaim 1, wherein the at least one of the minichannel and the microchannel is a minichannel with a minimum cross-sectional dimension of less than three millimeters.

8. The system as set forth inclaim 1, wherein the at least one of the minichannel and the microchannel is a microchannel with a minimum cross-sectional dimension of less than about 200 microns.

9. The system as set forth inclaim 1, further comprising additional nucleation cavities spaced apart substantially the same distance along a section of the channel wall.

10. The system as set forth inclaim 1, further comprising additional nucleation cavities randomly located along a section of the channel wall.

11. The system as set forth inclaim 1, wherein the flow further comprises dissolved gasses.

12. The system as set forth inclaim 1, wherein the flow further comprises microbubbles.

13. The system as set forth inclaim 1, wherein the flow further comprises non-soluble gasses.

14. The system as set forth inclaim 1, wherein the flow further comprises volatile liquid.

15. The system as set forth inclaim 1, wherein the low pressure zone is downstream from the transition from the high pressure region to the low pressure region.

16. The system as set forth inclaim 1, wherein the nucleation cavities are in the low pressure region downstream from the low pressure zone.

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