Temperature Control Unit for Gaseous or Liquid Medium
20180164003 ยท 2018-06-14
Inventors
Cpc classification
F28D7/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
H10N10/17
ELECTRICITY
F23K1/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23K5/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2321/003
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23K2300/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2321/0252
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Y02T10/12
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
F23K2400/10
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02M31/125
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2321/023
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23K5/002
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F25B2321/0251
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
International classification
F25B21/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F02M31/125
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23K5/02
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
F23K1/04
MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
Abstract
For a temperature control unit for gaseous or liquid medium with a highly dynamic temperature regulation of the medium, the temperature control unit is designed with a base body and a cooling body between which are arranged multiple thermoelectric modules, and with a media line in the base body, wherein the media line is arranged in the base body in the form of a single-start spiral from the outside to the inside, and it is provided that the multiple thermoelectric modules are arranged in a plurality of rows on the base body, wherein the module heating power of a thermoelectric module situated further toward the outside radially is greater than the module heating power of a thermoelectric module situated further toward the inside radially.
Claims
1. A temperature control unit for temperature control of a gaseous or liquid medium by means of a number of thermoelectric modules which are arranged between a base body and a cooling body, and a media line through which the gaseous or liquid medium flows being arranged in the base body, wherein the media line is arranged in the base body in the form of a single-start spiral from the outside to the inside, wherein the multiple thermoelectric modules are arranged in a plurality of rows on the base body, wherein the module heating power of a thermoelectric module arranged further toward the outside radially is greater than the module heating power of a thermoelectric module arranged further toward the inside radially.
2. The temperature control unit according to claim 1, wherein the media line is bended out of the plane of the spiral and is led out from the base body at the inside.
3. The temperature control unit according to claim 1, wherein the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein is in the range of 0.5 to 1.
4. The temperature control unit according to claim 3, wherein the mass ratio is 0.75.
5. The temperature control unit according to claim 1, wherein a groove into which the media line is pressed is provided in the base body.
6. The temperature control unit according to claim 1, wherein the base body is surrounded by a base body jacket, wherein a plurality of radial connecting webs which are connected to the base body jacket are arranged over the circumference of the base body.
7. The temperature control unit according to claim 6, wherein the base body jacket is partially hollow.
8. The temperature control unit according to claim 1, wherein a cooling line, through which cooling medium for cooling the cooling body flows as needed, is arranged in the cooling body.
9. The temperature control unit according to claim 8, wherein the cooling line is arranged in the form of a spiral.
10. The temperature control unit according to claim 1, wherein the heating power in the radially outer region of the base body, as the sum of the module heating powers of the thermoelectric modules in the radially outer region, is greater than the heating power in the radially inner region of the base body, as the sum of the module heating powers of the thermoelectric modules in the radially inner region.
11. The temperature control unit according to claim 1, wherein the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein is in the range of 0.7 to 0.8.
12. The temperature control unit according to claim 2, wherein the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein is in the range of 0.5 to 1.
13. The temperature control unit according to claim 2, wherein the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein is in the range of 0.7 to 0.8.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0021] The present invention shall be described in further detail herein below with reference to
[0022]
[0023]
[0024]
[0025]
[0026]
[0027]
DETAILED DESCRIPTION
[0028]
[0029]
[0030] Thus, depending on the polarity of the power supply voltage, which is supplied, for example, via terminals 8, it is possible to provide both heating and cooling with such a thermoelectric module 7. Heating here means that heat is supplied to the base body 2, and cooling means that heat is withdrawn from the base body 2. The heat flow between the base body 2 and the cooling body 5 can thus be influenced with the thermoelectric modules 7.
[0031] The thermoelectric modules 7 are in direct or indirect (for example, via a heat transfer element to improve the thermal conduction) thermal contact with the base body 2 via a first heating surface 9a (not visible in
[0032] The base body 2 is illustrated in detail in
[0033] The base body jacket 21 may additionally be designed to be partially hollow, by incorporation of peripheral slots 24 into the base body jacket 21, also forming cavities for additional thermal insulation.
[0034]
[0035] The use of a media line 6 in the form of a single-start spiral is very complex from the standpoint of manufacturing technology because in this case the media line 6 extends in all three dimensions.
[0036] In an alternative embodiment, the media line 6 is arranged on the base body 2 in the form of a two-start planar spiral (also known as Fermat's spiral), as described with reference to
[0037] The single-start or two-start spiral need not necessarily be designed as a circular spiral but instead may also have other shapes such as rectangular, square, etc. Due to the spiral shape, the temperature control unit 1 can have a very compact design because the spiral passes can be arranged close to one another. Therefore, a great many running meters of media line 6 can be accommodated in a small space, which increases the available surface for temperature control of the medium flowing through the media line 6.
[0038] To be able to implement a dense packing of the media line 6, bending radii must not come below stipulated minimum bending radii in the shaping of the media line 6. A meandering layout of the media line would be disadvantageous in this regard because the required bending radii for a dense packing are considerably smaller than those with a spiral layout. With increasing pressure demands with regard to the media line 6, the minimum bending radius usually also increases because of the required increase in wall thickness. Therefore, a meandering layout has a particularly negative effect when there are high pressure demands, as in the present case.
[0039]
[0040] The thermoelectric modules 7 are preferably arranged on the base plate 20 in the form of circles, or adapted to the spiral form, and in multiple rows (that is at various radial distances) (
[0041] The module heating power of a thermoelectric module 7 is generally understood to be the rated power at a rated current/rated voltage, as well as the power that occurs at a certain current/voltage deviating from the rated current/rated voltage. Consequently, according to the invention, thermoelectric modules 7 with different rated powers, thermoelectric modules 7 that can be adjusted differently with different or identical rated powers, or combinations thereof may be used.
[0042] If an electric power supply voltage is applied to a thermoelectric module 7, then as is known one of the heating surfaces 9a, 9b of the thermoelectric module 7 is cooled off while at the same time the opposing heating surface 9a, 9b is heated. The maximum temperature spread between the heating surfaces 9a, 9b depends on the operating temperature (temperature on the warmer heating surface) of the thermoelectric module 7. The higher the operating temperature, the higher the maximum achievable temperature spread between the cold and hot heating surfaces 9a, 9b. Therefore, with the available thermoelectric modules 7, temperatures of up to 200 C. can be achieved on the hot heating surface, with the cold heating surface not exceeding 100 C. A highly dynamic regulation of the temperature is made possible by simply reversing the polarity of the power supply voltage. This regulation is supported in the temperature control unit 1 according to the invention, in that the cooling body 5 is used as a buffer storage in heating operation, i.e., when the medium in the media line 6 is to be heated. To this end the thermal storage mass, however, should not be designed to be as small as possible as is suggested in the prior art, but instead a certain storage mass is desired in order to achieve this.
[0043] It has been found to be advantageous if the mass ratio of the thermal storage mass of the cooling body 5 to the thermal storage mass of the base body 2 and the media line 6 arranged therein is selected to be in the range of 0.5 to 1, advantageously 0.7 to 0.8. A most especially advantageous temperature regulability of the temperature control unit 1 was achieved at a mass ratio in the range of 0.75 or at a mass ratio of 0.75. A tested temperature control unit 1, for example, had a thermal storage mass of the cooling body 5 of 5.4 kg and a thermal storage mass of the base body 2 and the media line 6 arranged therein of 7.2 kg, which yields a mass ratio of 0.75.
[0044] In one embodiment as shown in
[0045] At a constant heating demand of the temperature control unit 1, i.e., at a constant power supply voltage of the thermoelectric module 7, a stable temperature spread is established on the thermoelectric modules 7. As soon as less thermal energy or heat for temperature control of the medium is needed, the power supply voltage to the thermoelectric modules 7 is reduced so that the temperature spread also becomes lower. The temperature on the heating surface 9a of the thermoelectric module 7, which is in contact with the base plate 20, therefore drops. At the same time, the temperature on the opposite heating surface 9b rises. Thus, there is a temperature gradient between the heating surface 9b and the cooling body 5, which is adjacent thereto, so that heat flows into the cooling body 5 and is not dissipated to the surroundings immediately because of the thermal storage mass of the cooling body 5, but instead is stored temporarily (at least for a limited period of time). This temporarily stored thermal energy is available to the temperature control or temperature control unit 1 as support when more thermal energy is again needed for temperature control of the medium. In this case, the power supply voltage would be raised again so that the temperature spread on the thermoelectric modules 7 would increase again. The temperature on the heating surface 9b with which the cooling body 5 is in contact would thus drop in comparison with the temperature of the cooling body 5. This results in an inverted temperature gradient, thus resulting in thermal energy (heat), which is stored in the cooling body 5, then flowing into the base body 2 and thus supporting the thermoelectric modules 7. Because of the thermal storage mass of the cooling body 5, it is possible for the temperature control unit 1 to respond very rapidly and precisely to load changes or changes in temperature, and the typical overshooting temperature control can be prevented to the greatest extent. However, this requires the thermal storage mass of the cooling body 5 to be not too large or too small in comparison to the thermal storage mass of the base body 2 and the media line 6 arranged therein.
[0046] The total surface area of the cooling body 5 should be designed as a function of the operating temperature to be expected, so that the heat stored in the cooling body 5 is not dissipated too rapidly to the surroundings but instead remains stored in the cooling body 5 for a sufficient period of time. The surface is therefore not to be dimensioned to be as large as possible and optimized for the dissipation of heat, as it would be in a traditional cooling body, but on the contrary, it is to be dimensioned so that the heat remains stored in the cooling body 5.
[0047] Complete thermal insulation of the cooling body 5 from the surroundings would also be disadvantageous because in the case of frequent reversals of polarity, the temperature in the cooling body 5 might escalate.
[0048] For various media, the material of the media line 6 and the heating power of the thermoelectric modules 7 or the module heating powers of the thermoelectric modules 7 may optionally be adapted. However, the general basic principle with the cooling body 5 as a storage mass for support of the temperature control unit 1 remains unaffected.
[0049] For certain gaseous media such as natural gas, there is a great cooling in accordance with the Joule-Thomson effect due to the required depressurization. With these gases, the temperature control unit 1 must usually only preheat the gaseous medium. Cooling of these gases by the temperature control unit 1 is usually not necessary. Therefore, it is normally also sufficient for these applications to work only with the temperature spread of the thermoelectric modules 7. Reversal of the polarity to switch from heating to cooling is rather not necessary.
[0050] Other gaseous media, such as hydrogen, do not have this pronounced effect of extreme cooling due to the required depressurization. On the contrary, there may even be a heating due to depressurization. In temperature control of liquid media, often no depressurization is necessary because the liquid medium is already at the correct pressure.
[0051] In the case of gases without a pronounced Joule-Thomson effect or with liquid media, the temperature control unit 1 therefore must often switch between heating and cooling the gaseous medium in order to keep the temperature constant as a function of the pressure and the flow rate. In particular in the case of cooling, however, it may happen that because of the lower surface area of the cooling body 5, the produced heat, in particular the waste heat of the thermoelectric modules 7, cannot be dissipated rapidly enough. Therefore, when the temperature control unit 1 is being used with such gaseous or liquid media, provisions may also be taken to additionally cool the cooling body 5 as needed. Therefore, a cooling line 12 may be introduced into the cooling body 5 through which a cooling liquid is conducted for the additional cooling of the cooling body 5. Such a design is indicated in
[0052] In the exemplary embodiment shown in
[0053] If a separate line is used as cooling line 12 in the cooling body 5 (like the media line 6 in the base body), then the cooling line 12 would also be part of the thermal storage mass of the cooling body 5.
[0054] To be able to connect the cooling line 12 in the cooling body 5, a cooling medium supply connection 34 and a cooling medium removal connection 33 may be provided on the cooling body. The cooling medium is preferably supplied centrally from the inside and discharged at the outside.