相变以冷制冷方法及其循环系统 技术领域 Phase change cooling method and its circulation system
本发明涉及制冷技术, 特别涉及一种使相变制冷所产生的蒸气在绝热 膨胀工况下、 在温度低于制冷工质蒸发温度的环境中冷凝并恢复原有相态 的相变以冷制冷方法及其循环系统. 背景技术 The present invention relates to refrigeration technology, and in particular to a method for condensing vapor generated by phase change refrigeration in an adiabatic expansion condition in an environment whose temperature is lower than the evaporation temperature of a refrigerant and recovering the original phase state for cold refrigeration. Method and its circulatory system. BACKGROUND
现有相变制冷技术的各类制冷方法, 均是使相变制冷所产生的蒸气在 温度高于制冷工质蒸发温度的环境中冷凝并恢复原有相态; 并且通常是在 常温环境中冷凝并恢复原有相态; 必须提高制冷工质蒸气的压力. 现有各 类制冷技术的制冷方法, 均是一面制冷, 一面产热; 在制冷供冷过程中, 必须向外界环境排放热量; 并且通常是产热量多于制冷量. 就环境总效果 而言, 现有制冷技术的制冷方法不是制冷, 而是在制热; 通常形成越制冷 越产热, 越产热越不能制冷的恶性循环工况。 制冷机的供冷温度和排热环 境温度之间的温差必须限定在一个很小的范围内, 否则扩大这一温差, 现 有制冷技术的制冷效率便会极低, 甚至根本无法制冷; 致使现有制冷技术 为了得到 -40 'C以下的冷量, 不得不采用多级复叠式制冷, 并且每级都必须 耗能. 发明的公开 Various refrigeration methods of the existing phase change refrigeration technology condense the vapor generated by phase change refrigeration in an environment whose temperature is higher than the evaporation temperature of the refrigerant and restore the original phase state; and usually it is condensed in a normal temperature environment And restore the original phase state; the pressure of the refrigerant refrigerant must be increased. The existing refrigeration methods of all types of refrigeration technology are one-side refrigeration and one-side heat generation; during the cooling and cooling process, heat must be discharged to the external environment; and Generally, the heat production is more than the cooling capacity. As far as the overall environmental effect is concerned, the existing refrigeration technology is not refrigeration, but heating; usually a vicious cycle is formed where the more refrigeration the more heat, the more heat the more it cannot be cooled. condition. The temperature difference between the cooling temperature of the refrigerator and the temperature of the exhaust heat environment must be limited to a small range; otherwise, if the temperature difference is enlarged, the cooling efficiency of the existing refrigeration technology will be extremely low, or even impossible to cool at all. In order to obtain the cooling capacity below -40 'C, there are refrigeration technologies that have to use multi-stage cascade refrigeration, and each stage must consume energy. Disclosure of the Invention
为了克月 上述缺点, 本发明的目的是提供一种新的相变以冷制冷方法 及其循环系统, 不向外界环境排放热量, 供冷温度可以在常温至深冷低温 之间任意设定, 制冷效率高. In order to overcome the above shortcomings, the object of the present invention is to provide a new phase-change refrigeration method and its circulation system, which does not emit heat to the external environment, and the cooling temperature can be arbitrarily set between normal temperature and cryogenic low temperature. High cooling efficiency.
本发明的技术方案如下: 一种相变以冷制冷方法及其循环系统, 其首 级制冷利用现有各类制冷技术提供原始冷量, 它可以是相变制冷中的蒸气 压缩制冷、 耗康式制冷、 吸收式制冷, 可以是半导体制冷, 可以是磁制冷; 可以是上述制冷技术中的任意一种单级制冷; 也可以是由上述制冷技术中 The technical solution of the present invention is as follows: A phase-change refrigeration method and its circulation system. The first-stage refrigeration utilizes various existing refrigeration technologies to provide the original cooling capacity. Refrigeration and absorption refrigeration can be semiconductor refrigeration or magnetic refrigeration; it can be any single-stage refrigeration in the refrigeration technology mentioned above;
- 1 - 确认本
任意一种組成的多级复叠式制冷; 还可以是由上述制冷技术中的多种技术 组成的多级复叠式制冷; 系统是由首级制冷、 任意中间级制冷、 末级制冷 循环组成的二级以上的多級复叠制冷循环, 首级制冷作为原始制冷, 末级 制冷负责将上一级制冷提供的冷量扩增并负责对外供冷, 任意中间级制冷 负责将原始冷量从 0级、 1 级至 n级扩增; 任意中间级和末级制冷方法为 相变以冷制冷循环方法, 它们均利用上一级制冷所提供的更低温度的冷 来冷凝本级相变制冷所产生的蒸气, 使制冷工质蒸气在温度低于其原蒸发 温度的环境中、 在绝热膨胀工况下恢复原有相态, 实现相变以冷制冷循环; 首级制冷所产生的热量由次一级相变以冷制冷循环所提供的冷量吸收, 使 首级制冷的产冷温度和排热环境温度之差, 减小到使首级制冷实现正常制 冷; 首级制冷的产冷温度、 任意中间级制冷的相变汽化温度、 以及末级制 冷的相变汽化温度按各级连接次序逐级增高, 首级制冷产冷温度为低, 末 级制冷相变汽化温度为高; 在相变以冷制冷方法及其循环系统中, 除末级 制冷循环中的对外制冷供冷部份外, 其余各级制冷循环以及末级制冷循环 中的其他功能部分均与外界环境绝热, 使各级相变以冷制冷循环中的制冷 工质蒸气从压力较高的蒸发空间流向压力较低的冷凝空间时实行绝热膨 胀, 使制冷工质蒸气在绝热膨胀中冷凝时只释放显热、 不释放凝结热。 -1-Confirmation Any kind of multi-stage cascade refrigeration; it can also be a multi-stage cascade refrigeration composed of multiple technologies in the above refrigeration technology; the system is composed of first-stage refrigeration, any intermediate-stage refrigeration, and last-stage refrigeration cycle The multi-stage cascade refrigeration cycle of more than two stages, the first stage refrigeration is used as the original refrigeration, the last stage refrigeration is responsible for amplifying the cooling capacity provided by the previous stage refrigeration and responsible for external cooling, and any intermediate stage refrigeration is responsible for changing the original refrigeration capacity from Stage 0, stage 1 to stage n expansion; any intermediate and final stage refrigeration methods are phase change and cold refrigeration cycle methods, they all use the lower temperature cooling provided by the previous stage refrigeration to condense the phase change refrigeration at this stage The generated vapor makes the refrigerant refrigerant vapor return to the original phase state under adiabatic expansion conditions in an environment whose temperature is lower than its original evaporation temperature, and realizes phase change to cool the refrigeration cycle; the heat generated by the first-stage refrigeration is The second-stage phase change absorbs the amount of cold provided by the cold refrigeration cycle, so that the difference between the cooling temperature of the first-stage refrigeration and the temperature of the exhaust heat environment is reduced to the normal cooling of the first-stage refrigeration; The temperature, the phase change vaporization temperature of any intermediate-stage refrigeration, and the phase change vaporization temperature of the final-stage refrigeration are gradually increased in accordance with the connection order of each level. The first-stage refrigeration production temperature is low, and the final-stage refrigeration phase-change vaporization temperature is high. In the phase-change refrigeration method and its circulation system, except for the external cooling and cooling part in the final refrigeration cycle, the other refrigeration cycles at all levels and other functional parts in the final refrigeration cycle are insulated from the external environment, so that each The phase change uses adiabatic expansion when the refrigerating working medium vapor in the cold refrigeration cycle flows from the higher pressure evaporation space to the lower pressure condensing space. When the refrigerating working medium vapor condenses in the adiabatic expansion, it only releases sensible heat and does not release Condensation heat.
本发明所述的相变以冷制冷方法及其循环系统是一种使制冷工质蒸气 在绝热膨胀工况下、 在温度低于其原蒸发温度的环境中恢复原有相态的新 的制冷方法, 制冷效率高, 不向外界排放热量, 供冷温度可以在常温至深 冷低温之间任意设定。 附图的简要说明 The phase change cold cooling method and its circulation system of the present invention are a new type of refrigeration that restores the original phase state of the refrigerating working medium vapor under an adiabatic expansion condition in an environment whose temperature is lower than its original evaporation temperature. The method has high refrigeration efficiency and does not emit heat to the outside, and the cooling temperature can be arbitrarily set between normal temperature and cryogenic low temperature. Brief description of the drawings
下面结合附图对本发明作详细描述: The present invention is described in detail below with reference to the drawings:
图 1是一种相变以冷制冷方法及其循环系统的流程示意图。 FIG. 1 is a schematic flow chart of a phase change cooling method and its circulation system.
图 2是上述系统由首级制冷与末级制冷循环组成的流程示意图。 Fig. 2 is a flow diagram of the above system consisting of a first-stage refrigeration and a last-stage refrigeration cycle.
图 3 是上述系统由首级制冷、 中间一 1 级制冷至中间一η级制冷以及 末级制冷循环组成的流程示意图。
实施本发明的最佳方式 FIG. 3 is a schematic flow chart of the above system consisting of first-stage refrigeration, intermediate first-stage refrigeration to intermediate first-n stage refrigeration, and last-stage refrigeration cycle. Best Mode for Carrying Out the Invention
参看图 1 , 图中所示的任意中间级制冷级数为 1, 系统由首级制冷、 中间― 1级制冷和末级制冷循环组成。 Referring to Figure 1, the number of any intermediate refrigeration stages shown in the figure is 1, and the system consists of a first-stage refrigeration, an intermediate-stage 1 refrigeration, and a final-stage refrigeration cycle.
参看图 2, 图中所示的任意中间级制冷级数为 0, 系统由首级制冷与 末级制冷循环组成。 Referring to Figure 2, the number of any intermediate cooling stages shown in the figure is 0, and the system consists of a first-stage refrigeration and a last-stage refrigeration cycle.
参看图 3, 图中所示的任意中间级制冷级数为 1 ~ n, 系统由首级制冷、 中间一 1级制冷至中间一 n级制冷以及末级制冷循环组成。 Referring to FIG. 3, the number of any intermediate cooling stages shown in the figure is 1 to n. The system is composed of a first stage cooling, a middle stage 1 cooling to a middle stage n cooling, and a final stage refrigeration cycle.
按图 1 所示, 在末级制冷循环中运行的相变制冷工质经工质输送过程 3输入对外制冷供冷的蒸发段 1 , 从用冷处吸热汽化, 相变制冷并对外供冷, 相变制冷所产饱和蒸汽, 不再按现有制冷技术所施加的机械压缩方法实行 蒸气压缩制冷循环, 而是采用相变以冷制冷循环方法, 即让饱和蒸气沿箭 头方向实行绝热膨胀进入比饱和蒸气温度更低的冷凝段 2„ 由于蒸发段 1 内气压大于冷凝段 2 内气压, 所以饱和蒸气自动沿箭头方向由蒸发段 1 至 冷凝段 2。 由上一级相变以冷制冷循环的蒸发段 4, 向末级制冷循环的冷凝 段 2提供更低温度的冷量。 饱和蒸气在绝热膨胀工况下遇冷凝结的过程, 是一个只释放显热、 不释放凝结热的过程, 是一个吸收并保存冷量的过程, 供冷方把冷量传导给饱和蒸气, 使之成为过冷液态或固态工质。 实现相变 以冷制冷循环的实际冷量损失远远小于本级相变以冷制冷循环中工质汽化 相变制冷所得的制冷量, 当在冷凝工况中, 重复利用过冷工质所携帶的比 饱和温度更低的冷量来与饱和蒸气充分进行热交换, 则其冷量损失更小。 由此可知, 相变以冷制冷循环是一个多倍和高倍扩增上一级所提供的冷量 的过程。 蒸气, 释放汽化潜热而制冷。 任意中间级和末级制冷的相变以冷制冷循环 是将固态工质吸热直接升华汽化成蒸气, 释放升华潜热而制冷。 As shown in Figure 1, the phase change refrigerant working in the final refrigeration cycle is input to the external cooling and cooling evaporation section 1 through the refrigerant transfer process 3, and the heat is evaporated from the cold place, and the phase change cooling and external cooling are performed. The saturated vapor produced by phase change refrigeration no longer implements the vapor compression refrigeration cycle according to the mechanical compression method applied by the existing refrigeration technology, but adopts the phase change to the cold refrigeration cycle method, that is, the saturated vapor is subjected to adiabatic expansion in the direction of the arrow. Condensation section 2 with a lower temperature than the saturated vapor „Since the pressure in the evaporation section 1 is greater than the pressure in the condensation section 2, the saturated vapor automatically moves from the evaporation section 1 to the condensation section 2 in the direction of the arrow. From the previous phase change to the cold refrigeration cycle The evaporation section 4 provides a lower-temperature cooling capacity to the condensation section 2 of the final refrigeration cycle. The process of saturated vapor encountering condensation under adiabatic expansion conditions is a process that only releases sensible heat and does not release condensation heat. It is a process of absorbing and preserving the cold energy, and the cold supply side transmits the cold energy to the saturated vapor, so that it becomes a supercooled liquid or solid working medium. The actual cooling capacity loss is much smaller than the refrigeration capacity obtained from the phase change refrigeration of the phase change cooling refrigerant in the refrigeration cycle. When in the condensing mode, the cold refrigerant carried by the subcooling refrigerant is reused at a lower temperature than the saturation temperature. If the amount of heat is fully exchanged with saturated steam, the loss of cooling capacity will be smaller. From this, it can be seen that the phase-change cold refrigeration cycle is a process of multiplying and multiplying the cooling capacity provided by the previous stage. Vapor, release Latent heat of vaporization and refrigeration. The phase change of any intermediate and final refrigeration is a cold refrigeration cycle. The solid working fluid absorbs heat directly and sublimates it into vapor, releasing the sublimation latent heat and refrigerating.
中间一 i 级相变以冷制冷循环, 其大部分工质经工质输送过程 6进入 主蒸发段 4 内, 从冷凝段 2吸热汽化形成饱和蒸气, 由图示箭头方向, 自
动实行绝热膨胀进入冷凝段 5, 由首级制冷的产冷段 9提供更低温度的冷 量冷凝; 其小部分工质经工质输送过程 7 进入副蒸发段 8, 从首级制冷的 产热段 10吸热汽化, 形成饱和蒸气, 沿箭头方向实行绝热膨胀进入冷凝段 5冷凝; 由此全部完成中间一 1级相变以冷制冷循环。 与前述末级相变以冷 制冷循环同理, 蒸发段 4 所制取的冷量, 从数量上多倍或高倍多于冷凝段 5所消耗的冷量。 The middle stage i phase change uses a cold refrigeration cycle. Most of its working fluid enters the main evaporation section 4 through the working fluid transport process 6, and absorbs heat from the condensation section 2 to vaporize to form saturated vapor. Adiabatic expansion is initiated to enter the condensing section 5, and the lower-temperature refrigeration output section 9 provides colder condensation at a lower temperature; a small part of the working fluid enters the sub-evaporation section 8 through the working fluid transport process 7, and the production from the first-stage refrigeration The hot section 10 absorbs heat and vaporizes to form saturated vapor, and performs adiabatic expansion in the direction of the arrow to enter the condensing section 5 to condense; thus all of the intermediate first-stage phase change and cold refrigeration cycles are completed. In the same way as in the previous stage phase change using the refrigeration cycle, the amount of cooling produced by the evaporation section 4 is multiple or higher than the amount of cooling consumed by the condensation section 5.
按图 2 所示, 首级制冷与末级相变以冷制冷循环组成相变以冷制冷循 环系统, 其任意中间级级数为 0。 末级制冷负责将上一级制冷提供的冷量 扩增并负责对外制冷供冷, 其制冷工质大部分经工质输送过程 3, 进入主 蒸发段 1 , 从用冷处吸热汽化制冷并对外供冷, 然后沿箭头方向实行绝热 膨胀进入冷凝段 2, 利用首级制冷的产冷段 9所提供的更低温度冷量冷凝; 小部分制冷工质经工质输送过程 7, 进入副蒸气段 8, 从首级制冷的产热段 10吸热汽化, 然后沿箭头方向实行绝热膨胀进入冷凝段 2冷凝恢复相态, 由此完成末级变以冷制冷循环, 首级制冷负责提供原始冷量。 As shown in Fig. 2, the first-stage refrigeration and the last-stage phase change constitute a phase-change to cold-refrigeration cycle system with a cold refrigeration cycle, and the number of any intermediate stage is zero. The last stage refrigeration is responsible for amplifying the amount of cooling provided by the previous stage refrigeration and responsible for external refrigeration and cooling. Most of its refrigerants go through the process 3 of the refrigerant transport, enter the main evaporation section 1, and absorb heat from the cold place to vaporize the refrigeration and Provide external cooling, and then perform adiabatic expansion in the direction of the arrow to enter the condensing section 2, and use the lower-temperature cooling capacity provided by the first-stage refrigeration production section 9 to condense; a small part of the refrigerant working fluid passes through the working fluid conveying process 7 and enters the sub-steam. Stage 8, absorb heat and vaporize from the heat-generating stage 10 of the first stage refrigeration, and then perform adiabatic expansion in the direction of the arrow to enter the condensing stage 2 to condense and restore the phase state, thereby completing the final stage to cool the refrigeration cycle. The first stage refrigeration is responsible for providing the original cooling the amount.
按图 3所示, 首级制冷与中间一 1级至中间一 n级相变以冷制冷循环, 以及末级相变以冷制冷循环所组成的 N+2级相变以冷制冷循环系统。 首级 制冷提供原始冷量, 中间一 1级至中间一 n级制冷负责逐级扩增原始冷量, 末级制冷负责将上一级制冷提供的冷量扩增并负责对外供冷。 末级制冷工 质经工质输送过程 3, 进入蒸发段 1 汽化制冷, 沿箭头方向实行绝热膨胀 回到冷凝段 2冷凝。 中间一 n级制冷工质经输送过程 6n, 进入蒸发段 4n, 从冷凝段 2吸热汽化, 再按箭头方向实行绝热膨胀回到冷凝段 5n冷凝。 依 照上述末级制冷与中间一 n级制冷之间关系, 同理设定中间一 1级至中间一 n级之间任意相连两级关系, 即上一级相变以冷制冷循环的蒸发段为次一 级相变以冷制冷循环的冷凝段提供充足冷量。 中间一 1 级制冷与首级制冷 的关系与图 1完全相同。 As shown in Fig. 3, the first-stage refrigeration and the middle-stage 1 to the middle-stage n-phase change to the cold refrigeration cycle, and the last-stage phase change consists of the N + 2 phase change to the cold refrigeration cycle system. The first-stage refrigeration provides the original cooling capacity, and the middle-stage 1 to middle-stage n-stage refrigeration is responsible for expanding the original cooling capacity step by step, and the final-stage refrigeration is responsible for expanding the cooling capacity provided by the previous-stage refrigeration and responsible for external cooling. The final refrigerating refrigerant enters the evaporation section 1 through the refrigerant conveying process 3, enters the evaporation section 1 and performs adiabatic expansion in the direction of the arrow, and returns to the condensation section 2 for condensation. In the middle, the n-stage refrigerating refrigerant enters the evaporation section 4n through the transfer process 6n, absorbs heat and vaporizes from the condensation section 2, and then performs adiabatic expansion in the direction of the arrow to return to the condensation section 5n for condensation. According to the relationship between the last stage refrigeration and the middle stage n refrigeration, the same two-stage relationship is set between the middle stage 1 to the middle stage n stages, that is, the phase change of the previous stage is the evaporation section of the cold refrigeration cycle as The second-stage phase change provides sufficient cooling capacity in the condensation section of the cold refrigeration cycle. The relationship between the first-stage cooling and the first-stage cooling is exactly the same as in Figure 1.
首级制冷所产生的热量由次一级相变以冷制冷循环所提供的冷量吸 收, 是直接将首级制冷所产生的热量排放到次一级制冷工质中, 使之吸收 热量产生相变。
首级制冷所产生的热量由次一级相变以冷制冷循环所提供的冷量吸 收, 是间接将首级制冷所产生的热量排放到次一级制冷工质中, 使次一级 制冷工质通过中间媒体, 吸收首级制冷所排放的热量产生相变。 The heat generated by the first-stage refrigeration is absorbed by the second-stage phase change and the cooling capacity provided by the cold refrigeration cycle. The heat generated by the first-stage refrigeration is directly discharged to the second-stage refrigeration working medium, so that it absorbs the heat and generates a phase. change. The heat generated by the first-stage refrigeration is absorbed by the second-stage phase change and the cooling capacity provided by the cold refrigeration cycle, which indirectly discharges the heat generated by the first-stage refrigeration to the second-stage refrigeration refrigerant, so that the second-stage refrigeration workers The mass passes through the intermediate medium and absorbs the heat emitted by the first-stage refrigeration to produce a phase change.
首级制冷为现有制冷技术, 电能或机械能进入首级制冷电器装置 1 1 , 使产冷段 9产冷, 产热段 10产热。 由于次一级以以冷制冷循环副蒸发段 8 全部了吸收了产热段 10的热量, 致使首级制冷的产冷段与产热段之间的温 差, 可以减小到符合实现首级制冷最佳工况的温差要求, 由此实现首级制 低, 甚至无法制冷的实际技术障碍。 The first-stage refrigeration is the existing refrigeration technology, and electric or mechanical energy enters the first-stage refrigeration electrical device 1 1 to generate 9 in the cold section and 10 in the heat section. Since the secondary stage has completely absorbed the heat of the heat-generating section 10 by the sub-evaporation section 8 of the refrigeration cycle, the temperature difference between the cold-generating section and the heat-generating section of the first-stage refrigeration can be reduced to meet the requirements of the first-stage refrigeration. The temperature difference requirements of the best working conditions, thereby realizing the first technical system low, even the actual technical obstacle of refrigerating.
任意中间级和末级相变以冷制冷循环均利用上一级制冷所提供的更低 温度的冷量来冷凝本级相变制冷所产生的蒸气, 即利用上一级制冷所提供 的更低温度的冷量将本级蒸气在绝热膨胀的工况下直接冷凝成过冷工质。 Any intermediate-stage and final-stage phase-change cooling refrigeration cycle uses the lower-temperature cooling capacity provided by the previous-stage refrigeration to condense the vapor generated by this phase-change refrigeration, that is, the lower-stage cooling provided by the previous-stage refrigeration is used. The cooling capacity of the temperature directly condenses the supercooled working fluid under adiabatic expansion conditions.
任意中间级和末级相变以冷制冷循环均利用上一级制冷所提供的更低 温度的冷量来冷凝本级相变制冷所产生的蒸气, 即利用上一级制冷所提供 的更低温度的冷量将本级蒸气在绝热膨胀工况下首先冷凝成过冷工质, 然 后利用过冷工质所携带的显冷再去冷凝绝热膨胀中的蒸气, 并多次重复利 用上一级制冷所提供的更低温度的冷量。 Any intermediate-stage and final-stage phase-change cooling refrigeration cycle uses the lower-temperature cooling capacity provided by the previous-stage refrigeration to condense the vapor generated by this phase-change refrigeration, that is, the lower-stage cooling provided by the previous-stage refrigeration is used. The cooling capacity of the temperature will first condense the steam in the adiabatic expansion into a supercooled working medium, then use the sensible cooling carried by the supercooled working medium to decondensate the steam in the adiabatic expansion, and reuse the previous stage multiple times. The cooler cooling capacity provided by refrigeration.
如图所示, 产冷段 9的温度低于蒸发段 4的温度, 蒸发段 4的温度低 于蒸发段 1 的温度。 蒸发段 9、 4、 1之间的温度差值, 按所需冷凝饱和蒸 气工况的要求设定。 对外制冷供冷的末级蒸发段 1 的温度按用冷要求, 可 在常温至深冷低温之间任意设定。 As shown in the figure, the temperature of the cooling section 9 is lower than the temperature of the evaporation section 4, and the temperature of the evaporation section 4 is lower than the temperature of the evaporation section 1. The temperature difference between the evaporation sections 9, 4, and 1 should be set according to the requirements of the required condensing saturated steam working conditions. The temperature of the last-stage evaporation section 1 for external cooling and cooling can be arbitrarily set between normal temperature and cryogenic low temperature according to the cooling requirements.
由于首级制冷中产热段 10 所产生的微量的热量全部被次一级相变以 冷制冷循环之副蒸发段 8 吸收, 并为其相变潜热消耗, 首级制冷以下各级 制冷循环均为消耗热量的工况, 所以图示相变以冷制冷方法及其循环系统 无任何热量向外界环境排放, 它只产冷, 不产热。 Since the trace heat generated in the heat-generating section 10 of the first-stage refrigeration is completely absorbed by the secondary evaporation section 8 of the second-stage phase change to the cold refrigeration cycle, and is consumed by its phase-change latent heat, the refrigeration cycles of the following stages of the first-stage refrigeration are Working conditions that consume heat, so the phase change shown in the figure shows that the cooling method and its circulation system do not emit any heat to the external environment. It only produces cold and does not produce heat.
由于制冷工质蒸气在绝热膨胀工况下遇冷凝结的过程, 是一个只释放 显热、 不释放凝结热的过程, 是一个吸收并保存冷量的过程, 相变以冷制 冷循环是一个多倍和高倍扩增上一级制冷所提供的冷量的过程。
首级制冷在本发明所提供的最佳冷凝环境工况条件下, 实现按正常效 率制冷, 甚至实现超出正常效率水准制冷, 其制冷量经由中间级相变以冷 制冷循环逐级从数量上多倍和高倍扩增, 为实现任意规模对外供冷的末级 相变以冷制冷循环提供了足够的冷凝冷量。 在图示整个相冷制冷方法及其 循环系统中, 除首级制冷必须耗费电能或机械动能之外, 其余各级相变以 冷制冷循环, 除工质输送过程还需要微量能耗之外, 无需其他能耗。 如前 所述, 首级制冷所消耗的能量已经取得正常制冷效率, 其效率经多级扩增, 使得本发明可以具有极高的制冷效率。 Since the refrigerant refrigerant vapor condenses and condenses under adiabatic expansion conditions, it is a process that only releases sensible heat and does not release condensation heat. It is a process that absorbs and preserves the amount of cold energy. The process of multiplying and doubling the amount of cooling provided by the previous stage of refrigeration. Under the optimal condensing environment working conditions provided by the present invention, the first-stage refrigeration achieves cooling at normal efficiency, or even exceeds the level of normal efficiency. Its refrigeration capacity is gradually increased by the number of stages in the cold refrigeration cycle through the intermediate phase change. Multiplier and high-amplification, in order to achieve the final stage phase change of external cooling of any scale to provide sufficient condensing cooling capacity. In the illustrated phase-cooling refrigeration method and its circulation system, in addition to the first-stage refrigeration, which must consume electrical energy or mechanical kinetic energy, the other stages of phase-change use a cold-refrigeration cycle. In addition to the working fluid transportation process, a small amount of energy is required. No additional energy consumption is required. As mentioned above, the energy consumed by the first-stage refrigeration has achieved normal refrigeration efficiency, and its efficiency has been multi-stage expanded, so that the present invention can have extremely high refrigeration efficiency.
本发明所述相变以冷制冷方法及其循环系统节省了制冷电能, 降低了 制冷供冷成本, 为扩充制冷供冷的生产规模和能力提供了技术条件。 本发 明在原理、 工业和商业上的应用都包含在本发明的权利要求范围内, 任何 在此基础上的改进技术都取自本发明的权利要求。
The phase change cooling method and its circulation system of the present invention save refrigeration electric energy, reduce the cost of refrigeration and cooling, and provide technical conditions for expanding the production scale and capacity of refrigeration and cooling. The principle, industry and commercial application of the present invention are all included in the scope of the claims of the present invention, and any improved technology based on this is taken from the claims of the present invention.