The present invention relates to a thermoelectric module used for cooling.
Generally, a thermoelectric module including a thermoelectric conversion element has a structure formed as a PN junction pair in which a P-type thermoelectric material and an N-type thermoelectric material are bonded between metal electrodes. When a temperature difference is given between the PN junction pair, electric power is generated by the Seeback effect, thereby the thermoelectric element can function as an apparatus generating electric power. Further, the thermoelectric element may be used as a temperature control apparatus by the Peltier effect, in which one side of the PN junction pair is cooled while the other side is heated.
In this regard, the Peltier effect is a phenomenon that, when a DC voltage is applied from the outside, holes of the P-type material and electrons of the N-type material move, which causes heat generation and heat absorption at opposite ends of the material. The Seeback effect refers to a phenomenon that, when heat is supplied from an external heat source, electrons and holes move which causes a current flow in a material, thereby generating electricity.
Such an active cooling using the thermoelectric material is recognized as a compact and eco-friendly method because of improved the thermal stability of the element, no vibration, no noise, and no need to use a separate condenser and refrigerant. Application fields of the active cooling using the thermoelectric material may include a refrigerant-free refrigerator, an air conditioner, various micro-cooling systems, and the like, and particularly, when the thermoelectric element is attached to various kinds of memory devices, the performance of the devices can be improved since maintaining the devices at a uniform and stable temperature is possible while reducing the volume as compared to a conventional cooling method.
As a factor to measure a performance of the thermoelectric material, a ZT value of dimensionless figure of merit (hereinafter, referred to as “thermoelectric figure of merit”) defined by the following Equation 1 is used.
Here, S is a Seeback coefficient, G is electrical conductivity, T is absolute temperature, and κ is thermal conductivity.
Recently, methods for improving thermoelectric efficiency in various perspectives have been reported.
However, in the majority of cases, the elements formed of the P-type thermoelectric material and the N-type thermoelectric material are manufactured by a bulk-type based on the same specification even when being applied to a cooling apparatus, which actually has shown a limit to cooling efficiency due to different electrical conducting characteristics between the P-type thermoelectric material and the N-type thermoelectric material.
The present invention is directed to providing a thermoelectric module configured to have a structure capable of enhancing cooling efficiency by forming a volume of one of thermoelectric semiconductor elements facing each other to be greater than that of the other in a unit cell formed with the thermoelectric semiconductor elements to enhance electrical conductivity characteristics.
One aspect of the present invention provides a thermoelectric module which includes at least one unit cell having a first semiconductor element and a second semiconductor element which are electrically connected, wherein volumes of the first semiconductor element and the second semiconductor element are mutually different. In this case, the first semiconductor element may be formed of a P-type semiconductor element and the second semiconductor element may be formed of an N-type semiconductor element, and a cooling module implemented by a structure in which the volume of the N-type semiconductor element is formed to be relatively greater than that of the P-type semiconductor element is provided.
According to the embodiment of the present invention, by forming a volume of one of thermoelectric semiconductor elements facing each other to be greater than that of the other in a unit cell formed with the thermoelectric semiconductor elements, electrical conductivity characteristics can be improved, thereby having an effect of enhancing the cooling efficiency.
Particularly, by forming a volume of an N-type semiconductor element to be greater than that of a P-type semiconductor element facing the N-type semiconductor element by changing a diameter of a cross section or a height of the N-type semiconductor element, the thermoelectric cooling efficiency is raised, and in addition, the cross section of the thermoelectric element can be formed in a circular or an elliptical shape having a curvature to form a printed-type thick film, thereby having an effect of raising the efficiency in a manufacturing process.
Hereinafter, configurations and operations according to the present invention will be described in detail with reference to the accompanying drawings. In the description with reference to the accompanying drawings, like elements are designated by the same reference numerals regardless of drawing numbers, and duplicated descriptions thereof will be omitted. Although the terms “first,” “second,” etc. may be used herein to describe various elements, these elements should not be limited by these terms. These terms are only used to distinguish one element from another.
As shown in
The formation of the volumes of the semiconductor elements disposed facing each other in the unit cell to be different may be implemented by methods, on the whole, of forming entire shapes of the semiconductor elements to be different, forming a diameter of a cross section at one of the semiconductor elements to be wider than the other in the semiconductor elements having the same height, or forming heights or diameters of the cross sections of the semiconductor elements to be different in the semiconductor elements having the same shape.
Figures of the diameters of the thermoelectric semiconductor elements which are illustrated in the views and embodiments of the present invention described below are formed as examples, are not limited thereto, and may be formed in various ranges of designs including the examples.
Referring to
In the unit cell including a thermoelectric element illustrated in
Particularly, as shown in the views, in the embodiment of the present invention, unlike a conventional bulk-type semiconductor element, cross sections of the first semiconductor element and the second semiconductor element form a circle, which enables forming a printed-type thick film in a design of a cylindrical shape, thereby enhancing manufacturing efficiency. The N-type semiconductor may be formed using a mixture in which main ingredient material formed of a bismuth telluride based (BiTe based) material including selenium (Se), nickel (Ni), aluminum (Al), copper (Cu), silver (Ag), lead (Pb), boron (B), gallium (Ga), tellurium (Te), bismuth (Bi), and/or indium (In) and Bi or Te corresponding to 0.001 to 1.0 wt % of the total weight of the main ingredient material are mixed. In other words, the main ingredient material is a Bi—Se—Te material, in which Bi or Te corresponding to 0.001 to 1.0 wt % of the total weight of the Bi—Se—Te is further added to form the mixture. That is, when 100 g of weight of Bi—Se—Te is input, it is preferable that Bi or Te is additionally added in the range of 0.001 g to 1.0 g. As described above, the weight range of the material added to the main ingredient material is significant in that the improvement of a ZT value cannot be expected outside the range of 0.001 wt % to 0.1 wt % as the thermal conductivity is not lowered while electric conductivity drops.
The P-type semiconductor material is preferably formed using a mixture in which a main ingredient material formed of a BiTe based material including antimony (Sb), nickel (Ni), aluminum (Al), copper (Cu), silver (Ag), lead (Pb), boron (B), gallium (Ga), tellurium (Te), bismuth (Bi), and/or indium (In) and Bi or Te corresponding to 0.001 to 1.0 wt % of the total weight of the main ingredient material are mixed. In other words, the main ingredient material is a Bi—Sb—Te material, in which Bi or Te corresponding to 0.001 to 1.0 wt % of the total weight of the Bi—Sb—Te is further added to form the mixture. That is, when 100 g of weight of Bi—Sb—Te is input, it is preferable that Bi or Te is additionally added in the range of 0.001 g to 1 g. As described above, the weight range of the material added to the main ingredient material is significant in that improvement of the ZT value cannot be expected outside the range of 0.001 wt % to 0.1 wt % as the thermal conductivity is not lowered while electrical conductivity drops.
In the above-described embodiment, when forming the thermoelectric semiconductor elements to have the same heights, it is preferable that a radius ratio of a horizontal cross section between the first semiconductor element and the second semiconductor element satisfy the range of 1:(1.01 to 1.5). That is, in the case that the first semiconductor element is formed as the P-type semiconductor element and the diameter of the cross section satisfy 1.4 mm, the diameter of the N-type semiconductor has a greater diameter than that and is formed in the range of 1.41 mm to 2.10 mm. This is because, in the radius ratio range of 1:1.01 of the horizontal cross section between the first semiconductor element and the second semiconductor element, it is difficult to implement the effect of improving the electrical conductivity characteristics due to little variation of the volume of the N-type semiconductor element when the ratio is less than 1.01, and when the ratio is more than 1.5, a phenomenon that the cooling performance of the thermoelectric element is conversely a little bit degraded occurs while the electrical conductivity characteristics may be satisfied.
As described in the embodiments of
[Table 1]
Characteristics of a conventional bulk-type thermoelectric element generally have the following performance.
That is, in the case of the conventional bulk-type thermoelectric element, when the semiconductor elements in a pair are formed as the structure shown in
In the present experiment, variations of the resistivity, the Qc, and the Delta Tmax (° C.) were measured in the case of increasing the volume by sequentially increasing the radius of the cross section of the second semiconductor element (the N-type semiconductor) at each rate of 0.7, 0.8, 0.9, and 1.0, while the radius of the cross section of the first semiconductor element (the P-type semiconductor) was fixed to 0.7 mm. Each height of the thermoelectric elements was printed as 0.5 mm.
As illustrated in
In contrast, when the volume of the second semiconductor element (the N-type semiconductor) was increased by increasing the radius of the cross section of the second semiconductor element at each rate of 0.8, 0.9, and 1.0, the resistivity value was measured as 1.8369 Ω, 1.5523Ω, and 1.2677Ω respectively, from which it was verified that the resistivity was lowered by a maximum of 40% or more as compared to the case of the same volume as shown in comparative example 1, thereby the electrical conductivity characteristics was improved. The Qc was measured as 90.9999, 94.5499, and 98.0999 respectively, and it was verified that the Qc was improved by a maximum of 12% or more as compared to comparative example 1. In spite of the efficiency improvement, in terms of the variation of the Delta T (° C.), the Delta T (° C.) was formed within an acceptable range that the efficiency was not much different from that of the comparative example, and it was verified that it was more excellent by 10° C. as compared to the conventional bulk-type.
Referring to
The result was similar to that when the volume of the second semiconductor element (the N-type semiconductor) was increased by increasing the radius of the cross section of the second semiconductor element at each of the rates of 0.8, 0.9, and 1.0, the resistivity was measured as 1.4977 Ω, 1.2131Ω, and 0.9285Ω respectively, which was lowering the resistivity by a maximum of 48% as compared to the resistivity of 1.7824Ω of comparative example 2, and the Qc was measured as 109.319, 112.869 and 116.419, which verified the improvement by a maximum of 10% or more as compared to 105.769 W of comparative example 2. Further, in terms of the variation of the Delta T (° C.) from comparative example 2, it was formed within an acceptable range that the efficiency was not much different from that of the comparative example, and it was verified that it was more excellent by 10° C. as compared to the bulk-type.
Referring to
The result was similar to that when the volume of the second semiconductor element (the N-type semiconductor) was increased by increasing the radius of the cross section of the second semiconductor element at each of the rates of 0.8, 0.9, and 1.0, the resistivity was measured as 1.4468 Ω, 1.1622Ω, and 0.8776Ω respectively, which was lowering the resistivity by a maximum of 49% as compared to the resistivity of 1.7315Ω of comparative example 3, and the Qc was measured as 112.067, 115.617 and 119.167, which verified the improvement by a maximum of 9.8% or more as compared to 108.517 W of comparative example 2. Further, in terms of the variation of the Delta T (° C.) from comparative example 2, it was formed within an acceptable range that the efficiency was not much different from that of the comparative example, and it was verified that it was more excellent by 10° C. as compared to the bulk-type.
Referring to
The result was similar to that when the volume of the second semiconductor element (the N-type semiconductor) was increased by increasing the radius of the cross section of the second semiconductor element at each of the rates of 0.8, 0.9, and 1.0, the resistivity was measured as 1.4299 Ω, 1.1453Ω, and 0.8606Ω respectively, which was lowering the resistivity by a maximum of 50% as compared to the resistivity of 1.7145Ω of comparative example 4, and the Qc was measured as 112.983, 116.533 and 120.083, which verified the improvement by a maximum of 9.7% or more as compared to 109.433 W of comparative example 4. Further, in terms of the variation of the Delta T (° C.) from comparative example 2, it was formed within an acceptable range that the efficiency was not much different from that of the comparative example, and it was verified that it was more excellent by 10° C. as compared to the bulk-type.
All the result of experimental examples 1 to 4 are experimental examples formed as compared to the comparative examples in the range that the ratio of the radius of the P-type semiconductor element (the first semiconductor element) to the radius of the N-type semiconductor element (the second semiconductor element) are satisfying the range of 1:(1.01˜1.50), which verifies that in any case it brings a significant improvement in terms of the resistivity, the Qc, and the Delta T (° C.) as compared to the conventional bulk-type thermoelectric element shown in Table 1. Particularly, as verified in experimental examples 1 to 4 above, the first semiconductor element and the second semiconductor element according to the embodiment of the present invention are formed by being printed in a form of a film, and the thickness is formed in the range of 0.02 mm to 0.50 mm. It is because the cooling performance as the thermoelectric element is degraded when the thickness is less than 0.02 mm, and there is little difference from the bulk-type element in terms of Qc characteristics when the thickness is more than 0.5 mm.
The detailed description of the present invention as described above has been described with reference to certain preferred embodiments thereof. However, various modifications may be made in the embodiments without departing from the scope of the present invention. The inventive concept of the present invention is not limited to the embodiments described above, but should be defined by the claims and equivalent scope thereof.
Number | Date | Country | Kind |
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10-2013-0107384 | Sep 2013 | KR | national |
Filing Document | Filing Date | Country | Kind |
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PCT/KR2014/008333 | 9/4/2014 | WO | 00 |