HEAT EXCHANGE PROMOTION MEMBER AND HEAT EXCHANGER

Abstract

Provided is a heat exchange promotion member and a heat exchanger that can improve heat transfer performance while holding down an increase in pressure drag of a fluid that exchanges heat with the heat exchange promotion member. A heat dissipation fin 14 of the present invention is a heat exchange promotion member that exchanges heat with a flowing fluid. The heat dissipation fin 14 includes a planar part 12 which is a surface substantially parallel to the fluid flowing direction and a raised part 13 that protrudes from the planar part 12 toward the fluid. The raised part 13 has a portion slanted relative to the direction in which the fluid flows, and there are a plurality of the raised parts 13 formed spaced apart from one another in the fluid flowing direction.

Claims

1-9. (canceled)

10. A heat exchanger comprising: a plurality of heat dissipation fins that are arranged at constant intervals and exchange heat with a fluid; and a heat transfer tube that is thermally coupled with the heat dissipation fins and allows a heat medium to flow thereinside, the heat medium transporting heat energy, wherein the heat dissipation fins each include a planar part which is a flat surface substantially parallel to a direction in which the fluid flows and a raised part that extends in a direction intersecting with the direction in which the heat medium flows and that protrudes from the planar part toward the fluid, the raised part has a portion slanted relative to the direction in which the fluid flows, and the heat dissipation fins each have a plurality of shapes formed at substantially constant intervals in the direction in which the fluid flows, each of the shapes being a combination of the planar part and the raised part.

11. The heat exchanger according to claim 10, wherein the raised part alternately has a first raised portion slanted to one direction along a flow of the fluid and a second raised portion slanted to a different direction along the flow of the fluid, and a portion where the first raised portion and the second raised portion are continuous with each other forms a substantially letter-V shape.

12. The heat exchanger according to claim 10, wherein an angle at which the raised part is slanted from a direction orthogonal to a flow of the fluid is from at least 30° to not greater than 80°.

13. The heat exchanger according to claim 10, wherein a width of the raised part is from at least 0.6 mm to not greater than 4.5 mm.

14. The heat exchanger according to claim 10, wherein the raised part protrudes from the planar part by a length of from at least 0.2 mm to not greater than 1.5 mm.

15. The heat exchanger according to claim 10, wherein a cross section of the raised part at a tip end portion side is a substantially semicircular shape.

16. The heat exchanger according to claim 10, wherein there are at least four to not greater than sixteen pieces of the raised parts in a direction orthogonal to a flow of the heat medium.

17. A heat exchanger comprising: a plurality of heat dissipation fins that are arranged at constant intervals and exchange heat with a fluid; and a heat transfer tube that is thermally coupled with the heat dissipation fins and allows a heat medium to flow thereinside, the heat medium transporting heat energy, wherein the heat dissipation fins each include a planar part which is a flat surface substantially parallel to a direction in which the fluid flows and a raised part that extends in a direction intersecting with the direction in which the heat medium flows and that protrudes from the planar part toward the fluid, the raised part has a portion slanted relative to the direction in which the fluid flows, there are a plurality of the raised parts formed spaced apart from one another in the direction in which the fluid flows, when the direction in which the fluid flows is a first direction and a direction orthogonal to the first direction is a second direction, the heat transfer tube has a first heat transfer tube group and a second heat transfer tube group that are arranged in the first direction the first heat transfer tube group has a plurality of the heat transfer tubes arranged in the second direction, the second heat transfer tube group has a plurality of the heat transfer tubes arranged in the second direction, a plurality of the raised parts are formed between the first heat transfer tube group and the second heat transfer tube group, a plurality of the raised parts are formed between the heat transfer tubes included in the first heat transfer tube group, and a plurality of the raised parts are formed between the heat transfer tubes included in the second heat transfer tube group.

18. The heat exchanger according to claim 17, wherein the heat transfer tubes included in the first heat transfer tube group and the heat transfer tubes included in the second heat transfer tube group are arranged in a zigzag manner.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0036] FIG. 1 is a diagram showing a heat exchanger including a heat exchange promotion member according to an embodiment of the present invention, FIG. 1A being a view of the heat exchanger seen in the Y direction and FIG. 1B being a view of the heat exchanger seen in the Z direction.

[0037] FIG. 2 is a perspective view of a heat dissipation fin according to the embodiment of the present invention.

[0038] FIG. 3 is a diagram showing a raised part formed at the heat dissipation fin according to the embodiment of the present invention, FIG. 3A being a view of the raised part seen in the Y direction and FIG. 3B being a sectional view taken along a cutting-plane line A-A in FIG. 3A.

[0039] FIG. 4 is a diagram showing the heat dissipation fin according to the embodiment of the present invention, FIG. 4A being a perspective view of the heat dissipation fin and FIG. 4B being a sectional view showing the flow of fluid in the vicinity of the upper surface of the heat dissipation fin.

[0040] FIG. 5 is a diagram showing the heat dissipation fin according to the embodiment of the present invention, FIG. 5A being a diagram showing the distribution of friction coefficient at the lower surface of the heat dissipation fin and FIG. 5B being a diagram showing the distribution of friction coefficient at the upper surface of the heat dissipation fin.

[0041] FIG. 6A shows a change in a flow field in a case where the heat dissipation fin is flat, and FIG. 6B shows a change in a flow field of the heat dissipation fin according to the embodiment of the present invention.

[0042] FIG. 7 is a diagram showing the heat dissipation fin according to the embodiment of the present invention, FIG. 7A being a graph showing the relation between a Reynolds number and a j-factor and FIG. 7B being a graph showing the relation between a Reynolds number and an f-factor.

[0043] FIG. 8 is a graph showing the correlation between the rate of improvement in the low-temperature-side heat transfer rate and the rate of increase in airflow resistance.

[0044] FIG. 9 is a diagram showing a heat exchanger including heat exchange promotion members according to another embodiment of the present invention, FIG. 9A being a view of the heat exchanger seen in the Y direction and FIG. 9B being a view of the heat exchanger seen in the X direction.

[0045] FIG. 10 is a diagram showing a heat exchanger including heat exchange promotion members according to yet another embodiment of the present invention, FIG. 10A being a perspective view and FIG. 10B being a sectional view.

[0046] FIG. 11 is a diagram showing a state where heat exchange promotion members according to still another embodiment of the present invention are housed in a casing, FIG. 11A being a perspective view and FIG. 11B being a top view showing the heat exchange promotion member.

DESCRIPTION OF EMBODIMENTS

[0047] An embodiment of the present invention is described in detail below based on the drawings. Although the following description shows an example where a heat exchange promotion member according to the present embodiment is used in a fin-and-tube heat exchanger, the heat exchange promotion member of the present embodiment can also be used in heat exchangers of other modes. For example, the heat exchange promotion member of the present embodiment can be used in, e.g., a plate heat exchanger or a heat transfer surface of a heat exchanger having a rectangular flow channel, which is specifically a heat transfer surface of an EGR cooler. In the following description, the X direction is a direction parallel to the direction in which a fluid flows, the Y direction is the direction of the thickness of a heat dissipation fin 14, and the Z direction is a direction orthogonal to the X direction and the Y direction.

[0048] The configuration of a heat exchanger 10 is described with reference to FIG. 1. FIG. 1A is a view of the heat exchanger 10 seen in the Y direction, and FIG. 1B is a view of the heat exchanger 10 seen in the Z direction. In FIG. 1A, a fluid is flowing in the X direction.

[0049] Referring to FIG. 1A, the heat exchanger 10 is formed of a plurality of heat dissipation fins 14 and heat transfer tubes 15. The heat exchanger 10 is a device for exchanging heat between a fluid that flows through between the heat dissipation fins 14 and a heat medium that flows through the inside of the heat transfer tubes 15. The heat exchanger 10 is used as, for example, an outdoor compact heat exchanger that enables a household solid oxide fuel cell (SOFC) system to be driven continuously for a long period of time. Further, the heat exchanger 10 can also be used for a room air conditioner, a heat pump water heater, a gas water heater, an oil water heater, and the like.

[0050] Various kinds can be used as the fluid to exchange heat with the heat dissipation fins 14, including a liquid such as water or a gas such as air. Also, various kinds can be used as the heat medium that flows through the inside of the heat transfer tubes 15, including a gas such as air, a liquid such as water, or a refrigerant used in a refrigeration cycle such as a vapor compression refrigeration cycle.

[0051] Each heat dissipation fin 14 is, for example, a plate member made of, e.g., metal with an excellent heat transfer rate, such as copper or aluminum, and here has a substantially rectangular shape with its long sides extending vertically. A large number of heat dissipation fins 14 are arranged at substantially equal intervals in their thickness direction. The heat dissipation fin 14 is one mode of a heat exchange promotion member and has an extended heat transfer surface.

[0052] Raised parts 13 are formed at each heat dissipation fin 14. The raised parts 13 are wall-shaped portions formed by partially protruding the heat dissipation fin 14 and extend in the Z direction in a meandering form. In FIG. 1A, the portion where the raised part 13 protrudes the most, i.e., a ridgeline, is indicated by a solid line. Also, a border between a flat portion and the raised part 13 of the heat dissipation fin 14 is indicated by a dotted line. There are a plurality of the raised parts 13 formed at substantially equal intervals, arranged in the X direction in which the fluid flows, and the raised parts 13 have substantially the same shape as one another. A detailed description of the shape of the raised part 13 will be given with reference to FIG. 3.

[0053] The heat transfer tubes 15 are tubular members made of metal with a high heat transfer rate such as copper and aluminum and have a meandering shape. By penetrating through the heat dissipation fin 14, the heat transfer tubes 15 are thermally coupled with the heat dissipation fin 14 at the penetration portions. Also, the heat transfer tubes 15 are arranged in a zigzag manner relative to the X direction in which the fluid flows.

[0054] Now, examples are given as to the sizes of the members forming the heat exchanger 10. As shown in FIG. 1A, the diameter DC of the heat transfer tube 15 is 10 mm, a pitch P1 between the heat transfer tubes 15 measured in the X direction in which the fluid flows is 22 mm, and a pitch Pt between the heat transfer tubes 15 measured in the Z direction orthogonal to the flow of fluid is 25.4 mm. Further, as shown in FIG. 1B, a distance H by which the heat dissipation fins 14 are spaced apart from each other in the Y direction is 1.82 mm, and thus, the heat dissipation fins 14 can be sufficiently spaced apart from each other, which can inhibit clogging of dirt, dust, and the like.

[0055] The diameter DC of the heat transfer tube 15 is the same as the diameter of a hole portion 16 (see FIG. 2) formed in the heat dissipation fin 14. The pitch P1 between the heat transfer tubes 15 measured in the X direction in which the fluid flows is the same as the pitch between the hole portions 16 measured in the X direction in which the fluid flows. The pitch Pt between the heat transfer tubes 15 measured in the Z direction orthogonal to the flow of fluid is the same as the pitch between the hole portions 16 measured in the Z direction orthogonal to the flow of fluid.

[0056] With reference to FIG. 2, the configuration of the heat dissipation fin 14 is described in detail. The heat dissipation fin 14 is, as described earlier, formed of a plate of metal that transfers heat well such as copper or aluminum, and has substantially circular hole portions 16 formed at the above-described portions where the heat transfer tubes 15 penetrate.

[0057] The heat dissipation fin 14 is a heat exchange promotion member that promotes heat exchange between the fluid and the heat medium described above. To promote heat exchange further, the heat dissipation fin 14 has the raised parts 13 formed thereat.

[0058] The raised parts 13 are portions formed by protruding part of the heat dissipation fin 14 in the +Y direction. As a whole, the raised part 13 forms a meandering wall parallel to the Z direction, which is a direction orthogonal to the X direction which is the flowing direction in which the fluid flows. Locally, the raised part 13 extends obliquely relative to the Z direction. Specifically, the raised part 13 alternately has a slanted portion where a +Z-side portion thereof is slanted toward the +X side and a slanted portion where a +Z-side portion thereof is slanted toward the −X side. The raised part 13 is formed continuously from the +Z-side end portion to the −Z-side end portion of the heat dissipation fin 14.

[0059] Unlike the background art, the heat dissipation fin 14 of the present embodiment does not have slits formed therein. Thus, even if a heat exchanger using the heat dissipation fins 14 is disposed in an easily contaminated environment, such as outdoors or inside a factory, attachment of dirt and the like to the heat dissipation fins 14 can be inhibited.

[0060] With reference to FIG. 3, the specific shape of the raised part 13 is described. FIG. 3A is a view of the raised part 13 seen from the +Y side, and FIG. 3B is a section taken along a cutting-plane line A-A in FIG. 3A.

[0061] Referring to FIG. 3A, the raised part 13 extends in the Z direction in a zigzag manner, forming a meandering shape. In other words, the raised part 13 alternately has a raised portion 131 that extends straight to the +Z side and is slanted to the −X side and a raised portion 132 that extends straight to the +Z side and is slanted to the +X side. With such a configuration, the raised part 13 forms a substantially letter-V shape at an edge portion 133 which is a −X-side edge portion where the raised portion 131 and the raised portion 132 are continuous with each other and at an edge portion 134 which is a +X-side edge portion where the raised portion 131 and the raised portion 132 are continuous with each other.

[0062] An angle θ at which the raised portion 131 is slanted from the Z direction is, for example, 55°. A favorable range of the angle θ is from at least 30° to not greater than 80°, and a more favorable range is from at least 40° to not greater than 70°, and a particularly favorable range is from at least 50° to not greater than 60°. When the raised portion 131 has the angle θ slanted from the X direction within the above ranges, heat transfer characteristics can be improved, and also, pressure loss can be reduced, as will be described later.

[0063] The length LZ of the raised portion 131 measured in the Z direction is, for example, 4 mm. A favorable range of LZ is from at least 1.5 mm to 6.4 mm, a more favorable range is from at least 2.5 mm to 5.5 mm, and an even more favorable range is from at least 3.0 mm to 5.0 mm. When LZ is a value within those ranges, heat transfer characteristics can be improved, and also, pressure loss can be reduced, as will be described later.

[0064] The angle θ at which the raised portion 132 is slanted from the Z direction and the length LZ of the raised portion 132 measured in the Z direction are the same as those of the raised portion 131.

[0065] Referring to FIG. 3B, the height h of the raised portion 131 is, for example, 0.9 mm. A favorable range of h is from at least 0.2 mm to 1.5 mm, a more favorable range is from at least 0.4 mm to 1.3 mm, and an even more favorable range is from at least 0.6 mm to 1.1 mm. When h is a value within those ranges, heat transfer characteristics can be improved, and also, pressure loss can be reduced, as will be described later.

[0066] The width w of the raised portion 131 is, for example, 2.5 mm. A favorable range of w is from at least 0.6 mm to not greater than 4.5 mm, a more favorable range is from at least 1.0 mm to 4.0 mm, and an even more favorable range is from at least 2.0 mm to 3.0 mm. When w is a value within those ranges, heat transfer characteristics can be improved, and also, pressure loss can be reduced, as will be described later.

[0067] Further, the number N of waves in a span direction is calculated from N=Pt/LZ, and an example value of N is from at least 4 to not greater than 16.

[0068] With reference to FIG. 4, a description is given of advantageous effects offered by the heat dissipation fin 14 having the shape described above. FIG. 4A is a perspective view of the heat dissipation fin 14, and FIG. 4B is a diagram showing the flows of fluid in a region surrounded by a dotted line in FIG. 4A. In FIG. 4B, the flow of fluid is shown with a thin solid-line arrow.

[0069] Referring to FIG. 4A, the direction of the ridge lines of the raised parts 13 are slanted at a predetermined angle relative to the X direction, which is a fluid flowing direction. Also, as shown in FIG. 3A, the slanting directions of the raised portions 131 and the raised portions 132 constituting the raised part 13 alternate at a constant cycle (LZ shown in FIG. 3A). Also, a portion where the raised portion 131 and the raised portion 132 are continuous with each other forms a letter-V shape.

[0070] Consequently, swirls 171 to 175 are formed at the upper surface of the heat dissipation fin 14. The swirls 171, 173, and 175 are formed on the upper surface of a planar part 12 of the heat dissipation fin 14. The planar part 12 is a surface substantially parallel to the flow of fluid. Meanwhile, the swirls 172 and 174 are formed above the raised parts 13. In the swirls 171 to 175, a fluid flows, swirling about a rotation axis parallel to the X-axis. The rotation direction of the swirls 171, 173, and 175 formed above the planar part 12 is opposite from the rotation direction of the swirls 172 and 174 formed above the raised parts 13. Specifically, from the viewpoint in FIG. 4B, the rotation direction of the swirls 171, 173, and 175 is counterclockwise, and the rotation direction of the swirls 172 and 174 is clockwise. Due to this phenomenon, a strong secondary flow is produced in a section perpendicular to the flow direction, promoting heat transfer at the heat dissipation fin 14.

[0071] Also, as described with reference to FIG. 3A, the raised part 13 forms a substantially letter-V shape at a portion where the raised portion 131 and the raised portion 132 are continuous with each other. Due to this shape of the raised part 13, a flow of fluid moving around to the back of the heat transfer tube 15 is formed, as will be described later. Thus, a wake behind the heat transfer tube 15 notably decreases, drastically decreasing pressure drag and holding down an increase in pressure loss. A wake is a region behind the heat transfer tube 15 where a fluid stagnates, and heat exchange efficiency is low in a wake.

[0072] Further, as shown in FIG. 4B, the sectional shape of the heat dissipation fin 14 is what is called a pulse-wave shape having the planar part 12 and the raised part 13 alternately. Thus, the substantially flat planar parts 12 exist at constant intervals in the fluid flow direction, and a sheer stress (frictional force) is enhanced. As a result, heat transfer between the heat dissipation fin 14 and the fluid is promoted, and an increase in pressure loss is held down.

[0073] Further, as is apparent from FIG. 4B, the raised parts 13 protrude only upwards (the +Y direction) and do not protrude downward (the −Y direction). With such a configuration, friction drag at the upper surface of the heat dissipation fin 14 (the surface facing the +Y direction) is larger than the friction drag at the lower surface of the heat dissipation fin 14 (the surface facing the −Y direction).

[0074] This phenomenon is described with reference to FIG. 5. FIG. 5A shows the distribution of friction coefficient at the lower surface of the heat dissipation fin 14, and FIG. 5B shows the distribution of friction coefficient at the upper surface of the heat dissipation fin 14. In FIGS. 5A and 5B, the density of color indicates the magnitude of the friction coefficient. In a comparison between the distribution chart in FIG. 5A and the distribution chart in FIG. 5B, the friction coefficient at the lower surface of the heat dissipation fin 14 shown in FIG. 5A is relatively small. Thus, the flow of fluid at the upper surface of the heat dissipation fin 14 and the flow of fluid at the lower surface of the heat dissipation fin 14 become asymmetrical, which enhances the flow that moves around to the back of the heat transfer tube 15, reducing the profile drag caused by the existence of the heat transfer tube 15.

[0075] Referring back to FIG. 4B, when the heat dissipation fin 14 has the above-described shape, the fluid favorably flows along the upper surface of the heat dissipation fin 14 without separating therefrom while maintaining its laminar flow state at the upper surface of the heat dissipation fin 14. Hence, heat transfer between the heat dissipation fin 14 and the fluid can be promoted.

[0076] With reference to FIG. 6, advantageous effects offered by the present embodiment are described. FIG. 6A shows a change in a flow field in a case where the heat dissipation fin 14 is a flat plate, and FIG. 6B shows a change in a flow field in a case where the heat dissipation fin 14 has the above-described raised parts 13 formed thereat. In FIGS. 6A and 6B, the efficiency of heat exchange between the heat dissipation fin 14 and the fluid is low at regions that are light in color.

[0077] Referring to FIG. 6A, a large wake is formed at a portion behind the heat transfer tube 15 (the portion surrounded by a white circle), and heat exchange efficiency is low there. This is because heat transfer between the surface of the heat dissipation fin 14 and the fluid is not favorably performed behind the heat transfer tube 15 due to the surface of the heat dissipation fin 14 being flat.

[0078] In FIG. 6B, a wake like the one shown in FIG. 6A is not generated at a portion behind the heat transfer tube 15 (the portion surrounded by a white circle), and heat exchange is therefore favorably performed. This demonstrates that when the raised parts 13 of a predetermined shape are formed at the surface of the heat dissipation fin 14 as described above, the fluid flows around to the back of the heat transfer tube 15, and heat transfer is thereby performed favorably between the surface of the heat dissipation fin 14 and the fluid.

[0079] With reference to a graph in FIG. 7, advantageous effects offered by the present embodiment are described. FIG. 7A is a diagram showing the correlation between the Reynolds number and the j-factor of the fluid that exchanges heat with the heat dissipation fin, and FIG. 7B is a diagram showing the correlation between the Reynolds number and the f-factor of the same fluid. The j-factor indicates heat transfer characteristics, and the f-factor indicates pressure loss.

[0080] In FIG. 7A, the horizontal axis represents the Reynolds number, and the vertical axis represents the j-factor. The graph here shows the characteristics of heat dissipation fins of various shapes; the solid line indicates the characteristics of a plane fin, the loosely-dotted line indicates the characteristics of a louvered fin, the densely-dotted line indicates the characteristics of a slitted fin, the dash-dot line indicates the characteristics of a wavy fin, and the dash-dot-dot line indicates the characteristics of a fin having dimples formed therein.

[0081] Further, the j-factor is measured under the condition that the Reynolds number is a particular value, and this graph shows the value for the plane fin measured under the above condition with a “white-filled circle,” the value for the wavy fin (with two wavy parts) with a “black-filled circle,” the value for the wavy fin (with four wavy parts) with a “black-filled square,” and the heat dissipation fin having the shape according to the present embodiment with a “black-filled triangle.”

[0082] As is clear from the graph, by using the heat dissipation fin 14 according to the present embodiment, the j-factor can be 107% larger than that of the plane fin, and therefore, heat exchange efficiency can be improved dramatically.

[0083] In a graph shown in FIG. 7B, the horizontal axis represents the Reynolds number, and the vertical axis represents the f-factor. As with FIG. 7A, the solid line indicates the characteristics of a plane fin, the loosely-dotted line indicates the characteristics of a louvered fin, the densely-dotted line indicates the characteristics of a slitted fin, the dash-dot line indicates the characteristics of a wavy fin, and the dash-dot-dot line indicates the characteristics of a fin having dimples formed therein. As a result of measuring a f-factor with the Reynolds number being a particular value as in FIG. 7A, the f-factor for the present embodiment indicated with a “black-filled triangle” is 78% larger than that of the plain fin.

[0084] Judging from the above, by using the heat dissipation fin 14 of the present embodiment, an increase in the j-factor can be 107% and an increase in the f-factor can be only 78%, compared to those of the plane fin. Thus, an increase in pressure loss can be suppressed while improving heat transfer performance. Thus, by using the heat dissipation fin 14 thus configured in a heat exchanger, heat exchange can be performed efficiently with low operational energy. Further, a heat exchanger using the heat dissipation fin 14 according to the present embodiment can reduce frosting and allows easy defrosting.

[0085] With reference to FIG. 9, the configuration of a heat exchanger 10 according to a different mode is described. FIG. 9A is a view of the heat exchanger 10 seen in the Y direction, and FIG. 9B is a view of the heat exchanger 10 seen in the X direction.

[0086] Referring to FIGS. 9A and 9B, the basic configuration of the heat exchanger 10 shown here is the same as that of the one shown in FIG. 1, and the heat exchanger 10 is configured as a plate heat exchanger. In a plate heat exchanger, a plurality of heat exchangers 10 are stacked and arranged at predetermined intervals. Also, in the vicinity of each of the four corners of the heat exchangers 10, a hole portion 18 is formed to allow a fluid-flowing tube to penetrate therethrough.

[0087] While the heat exchanger 10 is in operation, a high-temperature fluid and a low-temperature fluid flow in each heat exchanger 10 in the Y-axis direction. In the heat exchanger 10, the raised parts 13 are formed at predetermined intervals in such a manner as to form a substantially letter-V shape with respect to the flow of the high-temperature fluid or the low-temperature fluid. With such a configuration, the high-temperature fluid and the low-temperature fluid can effectively exchange heat with the heat exchanger 10.

[0088] Referring to FIG. 10, the heat dissipation fin 14 here is formed in a substantially corrugated manner. FIG. 10A is a perspective view of the heat dissipation fins 14, and FIG. 10B is a sectional view taken along a cutting-plane line B-B in FIG. 10A.

[0089] Referring to FIGS. 10A and 10B, when the heat dissipation fin 14 is seen in the Z direction, the heat dissipation fin 14 is formed in a corrugated shape in the X direction. The raised parts 13 are formed on the surface of the heat dissipation fin 14 facing +X. In this way, the corrugated heat exchanger 10 can effectively exchange heat with the fluids.

[0090] As shown in FIG. 10A, in the heat exchanger 10, high-temperature-side flow channels 22 and low-temperature-side flow channels 23 are formed alternately, arranged in the X direction with the heat dissipation fin 14 interposed therebetween. Also, the raised parts 13 are formed to protrude toward the high-temperature-side flow channels 22 and are also formed to protrude toward the low-temperature-side flow channels 23. Here, a fluid at relatively high temperature flows downward in the high-temperature-side flow channel 22, and a fluid at relatively low temperature flows upward in the low-temperature-side flow channel 23. In this way, effective heat exchange can be performed between the high-temperature fluid flowing through the high-temperature-side flow channel 22 and the low-temperature fluid flowing through the low-temperature-side flow channel 23 via the heat dissipation fin 14.

[0091] FIG. 11 is a diagram showing the heat exchanger 10 having a casing 19. FIG. 11A is a perspective view of the heat exchanger 10, and FIG. 11B is a top view of only the heat dissipation fin 14 taken out.

[0092] Referring to FIG. 11A, the heat dissipation fins 14 are housed in the casing 19. On the side surface of the heat exchanger 10 facing the −Y side, an introduction port 20 is formed at the lower edge side, and a discharge port 21 is formed at the upper edge side. For example, a low-temperature fluid is introduced into the casing 19 through the introduction port 20, and the low-temperature fluid after exchanging heat with the heat dissipation fins 14 is discharged to the outside through the discharge port 21.

[0093] Although not shown, an introduction port and a discharge port are also formed in the side surface of the casing 19 facing the +Y side, and a high-temperature fluid is introduced into the casing 19 through the introduction port, and the high-temperature fluid after exchanging heat with the heat dissipation fins 14 is discharged to the outside through the discharge port.

[0094] Although the embodiment of the present invention has thus been described above, the present invention is not limited to this and can be modified without departing from the gist of the present invention. Also, the above-described modes can be combined with each other.

[0095] The heat dissipation fin 14 described above is applicable not only to the heat exchanger 10, but also to, for example, a crossflow heat exchanger or a heat exchanger for automobiles, i.e., a condenser, an evaporator, a radiator, or the like.

REFERENCE SIGNS LIST

[0096] 10 heat exchanger [0097] 12 planar part [0098] 13 raised part [0099] 131 raised portion [0100] 132 raised portion [0101] 133 edge portion [0102] 134 edge portion [0103] 14 heat dissipation fin [0104] 15 heat transfer tube [0105] 16 hole portion [0106] 171 swirl [0107] 172 swirl [0108] 173 swirl [0109] 174 swirl [0110] 175 swirl [0111] 18 hole portion [0112] 19 casing [0113] 20 introduction port [0114] 21 discharge port [0115] 22 high-temperature-side flow channel [0116] 23 low-temperature-side flow channel