WO2016086495A1 - Gravity-driven two-phase fluid loop - Google Patents

Gravity-driven two-phase fluid loop Download PDF

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Publication number
WO2016086495A1
WO2016086495A1 PCT/CN2015/000301 CN2015000301W WO2016086495A1 WO 2016086495 A1 WO2016086495 A1 WO 2016086495A1 CN 2015000301 W CN2015000301 W CN 2015000301W WO 2016086495 A1 WO2016086495 A1 WO 2016086495A1
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Prior art keywords
liquid
evaporator
condenser
line
accumulator
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PCT/CN2015/000301
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French (fr)
Chinese (zh)
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苗建印
邵兴国
吕魏
张红星
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北京空间飞行器总体设计部
苗建印
邵兴国
吕魏
张红星
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Application filed by 北京空间飞行器总体设计部, 苗建印, 邵兴国, 吕魏, 张红星 filed Critical 北京空间飞行器总体设计部
Publication of WO2016086495A1 publication Critical patent/WO2016086495A1/en

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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F28HEAT EXCHANGE IN GENERAL
    • F28DHEAT-EXCHANGE APPARATUS, NOT PROVIDED FOR IN ANOTHER SUBCLASS, IN WHICH THE HEAT-EXCHANGE MEDIA DO NOT COME INTO DIRECT CONTACT
    • F28D15/00Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies
    • F28D15/02Heat-exchange apparatus with the intermediate heat-transfer medium in closed tubes passing into or through the conduit walls ; Heat-exchange apparatus employing intermediate heat-transfer medium or bodies in which the medium condenses and evaporates, e.g. heat pipes

Definitions

  • the invention relates to the technical field of spacecraft thermal control, and in particular to a gravity driven two-phase fluid circuit. Background technique
  • the temperature difference between day and night on the surface of the celestial body is very large, and the high and low temperature lasts for a long time.
  • the moon has a long lunar day (about 27.3 Earth days).
  • the surface temperature of the moon is very fast. Reduce it to around -180 °C.
  • the celestial body detector needs to survive at night in a long-term low temperature environment (such as the 340 hours of continuous low temperature of the moon) in an environment without solar energy (source of heat and electricity).
  • the celestial spacecraft experiencing the low temperature of the moon and night are mainly the US “Surveyor” series, the “Apollo” series and the Soviet “Lunokhod”. "Series.
  • the "Reviewer” series uses batteries as a heat source, and the heat transfer from the cabin equipment to the radiant panel is automatically controlled by a semi-active mechanical thermal switch. This solution requires a larger weight of the battery to meet the heater length of 340.
  • the hourly power supply requirement; "Apollo 11” uses a 30W isotope as a heat source, and the isotope is mounted on the detector to directly transfer heat to the device.
  • the isotope heat source has less heat and most of its heat is in the month.
  • Both ⁇ and moonlight are passed to the equipment, which solves the problem of moonlight insulation and brings about the high temperature problem of the moonlight.
  • "Apollo 12, 14-17" mainly uses electric energy converted from isothermal energy of the isotope source as a heat source. At the same time, it solves the problem of power supply during the day and night and the heating problem during the moon and night. The electricity is heated by the moon and night, and the heat is converted into electric energy through the process. The process of converting electrical energy into thermal energy.
  • thermoelectric conversion efficiency limitation of the thermoelectric battery Due to the thermoelectric conversion efficiency limitation of the thermoelectric battery, the thermal power demand for the nuclear source reaches 1480W, and the design cost is high; the "Lunar Rover” series uses the isotope nuclear heat source as the heat source and utilizes the active circuit.
  • the continuous operation of the system transfers heat to the inside of the detector, and the active loop system is powered by a large-capacity battery.
  • the design scheme of the moon and night insulation is complicated, and the active loop system needs to work continuously with low reliability.
  • the battery needs to be 340 hours. Active circuit during the moon and night System power supply, making the weight of the system increase
  • the present invention provides a gravity driven two-phase fluid circuit that can be used for spacecraft night warming, and that is lightweight and highly reliable.
  • the gravity driven two-phase fluid circuit of the present invention comprises an evaporator, a vapor line, a condenser, a liquid reservoir, a liquid line and a control valve; wherein the condenser is located above the gravity field of the liquid storage device and is required to be insulated Coupling; the evaporator is located below the gravity field of the accumulator and is coupled to the isotope heat source; the accumulator is connected to the evaporator inlet through the liquid line, and a control valve is arranged on the liquid line; the evaporator outlet passes through the steam tube in sequence
  • the pipeline and the condenser are connected to the accumulator to form a closed pipeline system; wherein the condenser is composed of a condensation pipeline and a condensation fin, the condensation pipeline is a V-shaped tube on the inlet side of the condensation pipeline The road is parallel to the lunar surface.
  • the line on the outlet side of the condensing line is on the same vertical surface as the outlet line, and is located below the inlet line and at an angle of 15° to the inlet line.
  • the inside of the circuit is filled at -70° ( : ⁇ Working medium in the gas-liquid two-phase state within the range of 120 °C.
  • the evaporator includes four screen evaporators, a vapor combiner, and a liquid splitter, wherein the screen evaporator is composed of an evaporator housing and a heat collecting seat that is sleeved on the evaporator housing,
  • the collector seat and the isotope nuclear heat source are thermally conductively mounted, the inner circumferential wall surface of the evaporator casing is provided with a thread groove, and the sintered stainless steel wire mesh is set inside the casing as a capillary core;
  • the inlet of the wire mesh evaporator is connected with the liquid flow divider, the wire mesh
  • the outlet of the evaporator is connected to the vapor manifold;
  • the liquid splitter is connected to the liquid line, and the vapor combiner is connected to the vapor line.
  • the vapor manifold is a 1/4 open annular structure, and the liquid splitter has a ring structure.
  • one end of the vapor line near the condenser is an inverted U-shaped, inverted U-shaped vapor line The bottom is higher than the inlet of the condenser.
  • control valve is a solenoid valve, and the sealing specific pressure is 4.51 MPa, and the pressure difference between the sealing surfaces of the control valve is 0.2 MPa.
  • the working fluid is ammonia.
  • the present invention has a simple structure, is light in weight, does not require an additional driving force, and can be applied to a spacecraft for nighttime insulation and has high reliability.
  • the vapor manifold is designed as a 1/4-open annular structure, which can better adapt to the thermal expansion and contraction of the evaporator due to the temperature change of the isotope source (changed between 110 ⁇ 240 °C). Thermal Stress.
  • the condensing line is designed to be V-shaped, so that the liquid working medium in the reservoir can be prevented from flowing back into the condenser when the lunar slope is not more than 15°.
  • the solenoid valve can effectively realize multiple opening and closing of the fluid circuit, and realize the heat transfer of the moon shackle. The function of transferring heat on the moon night.
  • the solenoid valve with a sealing specific pressure of 4.51Mpa and a pressure difference of 0.2MPa on the sealing surface of the control valve can meet the sealing reliability of the control valve and can withstand the axial acceleration of the detector in the launching section and the power lowering section. The sealing reliability of the control valve during the flight of the detector.
  • Figure 1 is a schematic view of the structure of the present invention.
  • Figure 2 is a schematic view of the structure of the evaporator.
  • Figure 3 is a schematic view of the structure of the screen evaporator.
  • Figure 4 is a schematic view of the structure of the condenser.
  • Figure 5 is a schematic view of the structure of the accumulator.
  • Figure 6 is a schematic view of the structure of the control valve.
  • the present invention provides a gravity driven two-phase fluid circuit, as shown in FIG. 1, including an evaporator 1 (including a wire mesh evaporator 7, a liquid flow divider 8 and a vapor manifold 9), a vapor line 2, and a condenser 3 a reservoir 4, a liquid line 6 and a control valve 5, wherein the condenser 3 is located above the gravity field of the accumulator 4 and coupled to a device (heat sink) requiring heat preservation, the evaporator 1 is located at the accumulator 4 gravity Below the field, coupled with an isotope heat source, a gravity driven height difference is formed between the liquid level in the reservoir 4 and the bottom of the evaporator 1; the reservoir 4 is connected to the inlet of the evaporator 1 through the liquid line 6, in the liquid tube There is a control room 5 on the road 6.
  • an evaporator 1 including a wire mesh evaporator 7, a liquid flow divider 8 and a vapor manifold 9
  • a vapor line 2
  • the outlet of the evaporator 1 is connected to the accumulator 4 through the vapor line 2 and the condenser 3 in sequence to form a closed piping system.
  • the inside of the circuit is filled with a working fluid in a gas-liquid two-phase state, such as ammonia, in the range of -70 ° C to 120 ° C, and the heat transfer is performed by using the gas-liquid phase change.
  • a working fluid in a gas-liquid two-phase state such as ammonia
  • the control valve 5 is opened. Due to the certain height difference between the reservoir 4 and the bottom of the evaporator 1, the liquid ammonia working fluid in the accumulator 4 flows into the evaporator 1 along the liquid line 6 under the driving of gravity.
  • the ammonia working fluid in the evaporator 1 absorbs the heat of the isotope heat source and is transformed into a gas.
  • the gaseous ammonia working fluid flows along the vapor line 2 to the condenser 3 to condense into a liquid, and transfers the heat to the lunar surface detector device.
  • the condensed liquid ammonia working fluid flows into the accumulator 4 to form a heat conduction loop for keeping the celestial detector warm.
  • the control valve 5 is closed, and the gravity-driven two-phase fluid circuit stops running.
  • the heat transfer between the isotope heat source and the inside of the detector is conducted through the heat conduction of the vapor line.
  • the heat is small to achieve thermal isolation, at which point the heat of the isotope nuclear heat source is dissipated outward by its own thermal radiation.
  • the structure of the evaporator 1 is as shown in FIG. 2, and includes four wire mesh evaporators 7, a vapor manifold 9, a liquid flow divider 8, a liquid filling pipe 10, and a joint (two-way, three-way, four-way), and wire.
  • the structure of the net evaporator 7 is as shown in FIG. 3, and is composed of an evaporator casing 14 and a heat collecting seat 15.
  • the evaporator casing 14 is installed inside the heat collecting seat 15, and the heat collecting seat 15 is thermally connected to the isotope heat source to evaporate.
  • the inner circumferential wall surface of the casing 14 is provided with a threaded groove, and the interior of the evaporator casing 14 is provided with a sintered stainless steel wire mesh as a capillary core.
  • the vapor manifold 9 is a 1/4-open circular ring. As shown in Fig. 2, it consists of two two-way 12, one three-way 11, one four-way 13 and three elbows. There are four steam inlets. And a vapor outlet, wherein the four vapor inlets are respectively connected to the outlets of the four screen evaporators, and the vapor outlets are connected to the vapor line 2.
  • the vapor manifold 9 is also provided with a liquid filling tube 10 of a two-phase fluid circuit.
  • the liquid diverter is annular and consists of three tees 11, one four-way 13 and four elbows, one liquid inlet and four liquid outlets, wherein the liquid inlet is connected to the liquid line 6, 4
  • the liquid outlets are respectively connected to the inlets of the four screen evaporators 7.
  • the material of the evaporator casing 14, the liquid filling pipe 10 and the joint is 00Crl7Nil4Mo2
  • the material of the heat collecting seat is 3A21 aluminum.
  • the liquid ammonia working fluid in the liquid storage device 4 flows into the liquid flow divider 8 through the liquid pipeline 6, and flows into the screen evaporator 7 by gravity to absorb the heat of the isotope nuclear heat source into a gaseous state, and the gaseous ammonia working fluid passes through the vapor.
  • the combiner 9 merges and flows into the vapor line 2.
  • the material of the steam line 2 is 00Crl7Nil4Mo2, in order to avoid the liquid working medium in the condenser 3 and the accumulator 4 flowing back into the evaporator 1 due to the position of the accumulator 4 being higher than the evaporator 1 during the lunar period, the evaporator 1
  • the liquid working medium is turned into a vapor and sent back to the condenser line 5, so that the detector device is still in a heating state.
  • the present invention sets the vapor line 2 close to the condenser 3 end to an inverted U shape, thereby The bottom of the inverted U-shaped vapor line 2 is made higher than the condenser 3 and the accumulator 4, and the reflux of the liquid working medium is suppressed.
  • the condenser 3 is composed of a condensing line 16 and a condensing fin 17, as shown in Figure 4, the material of the condensing line 16 is 00Crl 7Nil4Mo2, and the material of the condensing fin 17 is 3A21 aluminum.
  • the present invention designs the condensing line to be V-shaped, wherein, the condensation
  • the pipeline on the inlet side of the pipeline is parallel to the lunar surface, and the pipeline on the outlet side of the condensing pipeline is located below the gravity field of the inlet pipeline and at an angle of 15° to the inlet pipeline, thereby avoiding the inclination of the lunar surface by 15 degrees.
  • the liquid working fluid in the reservoir does not flow back into the condenser.
  • the control valve 5 is a solenoid valve, and its structure is shown in FIG. 6.
  • the material of the control valve housing is 00Crl 7Nil4Mo2 stainless steel, and the sealing portion is made of rubber.
  • the utility model utilizes the permanent magnet suction force and the medium pressure to act on the sealing surface to generate the sealing specific pressure.
  • the sealing specific pressure of 4.51 MPa is adopted, and the rubber soft sealing structure can ensure the ⁇ . ⁇ ⁇ 4 Pa-m 3 / s leak rate, meet the technical index internal leakage rate does not exceed 1.0xl (T 3 Pa rnVs requirements.
  • control valve 5 is also subjected to acceleration in the detector launch section and the power down section, between the liquid ammonia working fluid and the control valve sealing structure In the squeeze state, the control valve 5 is in a sealed state and will not be opened, thereby ensuring the reliability of the two-phase fluid circuit during the acceleration and deceleration of the detector.
  • the pressure difference between the sealing surface of the control valve is 0.2 MPa, it can withstand the influence of the pressure between the detector and the power-down section of the detector on the sealing structure due to the acceleration or deceleration of the ammonia and the sealing structure of the control valve.
  • the matching design of the accumulator 4 and the filling amount of the working fluid is related to the safety and heat transfer performance of the two-phase fluid circuit.
  • the accumulator should be able to accommodate most of the working fluid in the circuit during the lunar period, thereby avoiding the liquid working.
  • the volume expands when the temperature rises, causing the circuit to rupture, ensuring the safety of the entire fluid circuit.
  • the liquid level of the working fluid in the reservoir should be as small as possible with the working temperature, so that the storage
  • the gravity driving force corresponding to the height difference between the liquid level of the liquid level and the bottom of the evaporator 1 is as small as possible with temperature, which on the one hand can reduce the influence of the liquid level fluctuation on the stability of the circuit operation, and on the other hand, can ensure Provides sufficient driving force when the liquid level is lowest.
  • the structure of the accumulator 4 is as shown in Fig. 5, which is a cylinder whose upper and lower end faces are ellipsoidal. In order to reduce the height change of the liquid level of the accumulator at different working temperatures, the accumulator satisfies the layout and weight.
  • the inner diameter should be as large as possible if required.
  • the material of the liquid line 6 is 00Crl7Nil4Mo2 stainless steel.

Abstract

Disclosed is a gravity-driven two-phase fluid loop, consisting of an evaporator (1), a vapour pipeline (2), a condenser (3), a liquid storage device (4), a liquid pipeline (6) and a control valve (5), wherein the gravity formed by the altitude difference between the liquid storage device (4) and the evaporator (1) is used as a driving force; an isotopic nuclear heat source is used as a heat source; the heat is transferred by way of the gas-liquid transformation of a gas-liquid two-phase working medium filled into the loop; and the condenser (3) is arranged to be V-shaped, such that the liquid working medium in the liquid storage device (4) can be prevented from flowing back into the condenser (3) due to the lunar surface inclination.

Description

一种重力驱动两相流体回路 技术领域  Gravity driven two-phase fluid circuit
本发明涉及航天器热控制技术领域, 具体涉及一种重力驱动两相流体回路。 背景技术  The invention relates to the technical field of spacecraft thermal control, and in particular to a gravity driven two-phase fluid circuit. Background technique
天体表面昼夜温差很大, 且高、 低温持续时间长, 如月球具有漫长的月球 日 (约 27.3个地球日), 月夜期间, 由于月球上没有大气且月壤导热系数小, 月 球表面温度很快降低至 -180 °C左右。 天体探测器需在长时间的低温环境中 (如 月球连续 340小时的低温), 在没有太阳能.(热能和电能来源) 的环境中实现夜 间生存。 在已成功发射的天体探测器中, 经历月夜低温的天体探測器航天器主 要有美国的"勘测者 (Surveyor) "系列、 "阿波罗" (Apollo) "系列和苏联的"月 球车 (Lunokhod) "系列。 其中, "勘測者"系列采用蓄电池作为热源, 舱内设备 向辐射板的热量传递通过半主动的机械热开关自动控制, 该方案需较大重量的 蓄电池, 以满足加热器长达 340小时的供电需求; "阿波罗 11号"采用 30W的同 位素作为热源, 同位素安装在探測器上, 直接将热量传递至设备。 该方案中, 同位素热源热功率较小, 其绝大部分热量在月昼和月夜期间均传递给设备, 致 使解决月夜保温问题的同时也带来了月昼高温问题; "阿波罗 12、 14-17 号"主 要将同位素核源热能转化的电能作为热源。 该方案可同时解决昼夜期间供电问 题和月夜期间供热问题, 月夜电加热供热过,程中, 需经过热能转化成电能、 电 能再转化成热能的过程。 由于温差电池的热电转化效率限制, 使得对核源的热 功率需求达到 1480W, 设计方案成本较高; "月球车"系列采用同位素核热源作 为热源, 并利用主动回路系统的连续工作将热量传递至探测器内部, 主动回路 系统由大容量蓄电池供电。 该方案月夜保温设计方案复杂, 且需主动回路系统 连续工作, 可靠性低; 同时, 因蓄电池需要在 340 小时的月夜期间为主动回路 系统供电, 使得系统的重量增大 发明内容 The temperature difference between day and night on the surface of the celestial body is very large, and the high and low temperature lasts for a long time. For example, the moon has a long lunar day (about 27.3 Earth days). During the moon and night, because there is no atmosphere on the moon and the thermal conductivity of the moon is small, the surface temperature of the moon is very fast. Reduce it to around -180 °C. The celestial body detector needs to survive at night in a long-term low temperature environment (such as the 340 hours of continuous low temperature of the moon) in an environment without solar energy (source of heat and electricity). Among the successfully launched celestial detectors, the celestial spacecraft experiencing the low temperature of the moon and night are mainly the US "Surveyor" series, the "Apollo" series and the Soviet "Lunokhod". "Series. Among them, the "Reviewer" series uses batteries as a heat source, and the heat transfer from the cabin equipment to the radiant panel is automatically controlled by a semi-active mechanical thermal switch. This solution requires a larger weight of the battery to meet the heater length of 340. The hourly power supply requirement; "Apollo 11" uses a 30W isotope as a heat source, and the isotope is mounted on the detector to directly transfer heat to the device. In this scheme, the isotope heat source has less heat and most of its heat is in the month. Both 昼 and moonlight are passed to the equipment, which solves the problem of moonlight insulation and brings about the high temperature problem of the moonlight. "Apollo 12, 14-17" mainly uses electric energy converted from isothermal energy of the isotope source as a heat source. At the same time, it solves the problem of power supply during the day and night and the heating problem during the moon and night. The electricity is heated by the moon and night, and the heat is converted into electric energy through the process. The process of converting electrical energy into thermal energy. Due to the thermoelectric conversion efficiency limitation of the thermoelectric battery, the thermal power demand for the nuclear source reaches 1480W, and the design cost is high; the "Lunar Rover" series uses the isotope nuclear heat source as the heat source and utilizes the active circuit. The continuous operation of the system transfers heat to the inside of the detector, and the active loop system is powered by a large-capacity battery. The design scheme of the moon and night insulation is complicated, and the active loop system needs to work continuously with low reliability. At the same time, the battery needs to be 340 hours. Active circuit during the moon and night System power supply, making the weight of the system increase
有鉴于此, 本发明提供了一种重力驱动两相流体回路, 能够用于航天器夜 间保温, 且重量轻, 可靠性高。  In view of the above, the present invention provides a gravity driven two-phase fluid circuit that can be used for spacecraft night warming, and that is lightweight and highly reliable.
本发明的重力驱动两相流体回路, 包括蒸发器、 蒸气管路、 冷凝器、 储液 器、 液体管路和控制阀; 其中, 冷凝器位于储液器重力场上方、 并与需要保温 的设备耦合; 蒸发器位于储液器重力场的下方、 并与同位素热源耦合安装; 储 液器通过液体管路连接至蒸发器入口, 并在液体管路上设有控制阀; 蒸发器出 口依次通过蒸气管路、 冷凝器连接至储液器, 形成封闭的管路系统; 其中, 所 述冷凝器由冷凝管路和冷凝翅片组成, 所述冷凝管路为 V型, 冷凝管路入口一 侧的管路与月面平行, 冷凝管路出口一侧的管路与出口管路在同一垂面上, 并 位于入口管路下方且与入口管路成 15° 角; 回路内部充有在 -70° (:〜 120°C范围 内处于气液两相态的工质。  The gravity driven two-phase fluid circuit of the present invention comprises an evaporator, a vapor line, a condenser, a liquid reservoir, a liquid line and a control valve; wherein the condenser is located above the gravity field of the liquid storage device and is required to be insulated Coupling; the evaporator is located below the gravity field of the accumulator and is coupled to the isotope heat source; the accumulator is connected to the evaporator inlet through the liquid line, and a control valve is arranged on the liquid line; the evaporator outlet passes through the steam tube in sequence The pipeline and the condenser are connected to the accumulator to form a closed pipeline system; wherein the condenser is composed of a condensation pipeline and a condensation fin, the condensation pipeline is a V-shaped tube on the inlet side of the condensation pipeline The road is parallel to the lunar surface. The line on the outlet side of the condensing line is on the same vertical surface as the outlet line, and is located below the inlet line and at an angle of 15° to the inlet line. The inside of the circuit is filled at -70° ( : ~ Working medium in the gas-liquid two-phase state within the range of 120 °C.
进一步地, 所述蒸发器包括 4 个丝网蒸发器、 蒸气汇流器和液体分流器, 其中, 丝网蒸发器由蒸发器壳体和套装在蒸发器壳体上的集热座组成, 所述集 热座与同位素核热源导热安装, 蒸发器壳体内側周向壁面开设有螺纹槽, 壳体 内部套装烧结的不锈钢丝网作为毛细芯; 丝网蒸发器的入口与液体分流器连接, 丝网蒸发器的出口与蒸气汇流器连接; 液体分流器与液体管路连接, 蒸气汇流 器与蒸气管路连接。  Further, the evaporator includes four screen evaporators, a vapor combiner, and a liquid splitter, wherein the screen evaporator is composed of an evaporator housing and a heat collecting seat that is sleeved on the evaporator housing, The collector seat and the isotope nuclear heat source are thermally conductively mounted, the inner circumferential wall surface of the evaporator casing is provided with a thread groove, and the sintered stainless steel wire mesh is set inside the casing as a capillary core; the inlet of the wire mesh evaporator is connected with the liquid flow divider, the wire mesh The outlet of the evaporator is connected to the vapor manifold; the liquid splitter is connected to the liquid line, and the vapor combiner is connected to the vapor line.
进一步地,所述蒸气汇流器为 1/4开口的环形结构, 所述液体分流器为环形 结构。  Further, the vapor manifold is a 1/4 open annular structure, and the liquid splitter has a ring structure.
进一步地, 所述蒸气管路靠近冷凝器的一端为倒 U型, 倒 U型的蒸气管路 的底高于冷凝器的入口。 Further, one end of the vapor line near the condenser is an inverted U-shaped, inverted U-shaped vapor line The bottom is higher than the inlet of the condenser.
进一步地, 所述控制阀为电磁阀, 其密封比压为 4.51Mpa, 控制阀密封面上 下压差为 0.2MPa。  Further, the control valve is a solenoid valve, and the sealing specific pressure is 4.51 MPa, and the pressure difference between the sealing surfaces of the control valve is 0.2 MPa.
进一步地, 所迷工质为氨。  Further, the working fluid is ammonia.
进一步地, 所述工质的充装量计算方法为: 利用质量=密度 *体积, 联立最 高和最低储存温度下工质质量计算方程, 获得储液器体积与工质充装量; 其中, 最高储存温度下, 储液器内液体充满率为 100%, 外回路均为气体; 最低储存温 度下, 外回路充满液体, 储液器中含有体积分数为 10%的液态工质; 其中, 所 述外回路由流体回路中除去储液器的其余部分組成, 其体积已知。  Further, the method for calculating the filling amount of the working medium is: using the mass=density* volume, the working mass quality calculation equation of the highest and lowest storage temperatures, and obtaining the volume of the accumulator and the filling amount of the working medium; At the highest storage temperature, the liquid filling rate in the reservoir is 100%, and the outer circuit is gas; at the lowest storage temperature, the outer circuit is filled with liquid, and the liquid storage medium contains 10% by volume of liquid working medium; The outer circuit consists of the remainder of the fluid circuit that removes the reservoir, the volume of which is known.
有益效果:  Beneficial effects:
( 1 ) 本发明结构简单、 重量轻, 不需要额外的驱动力, 能够适用于航天器 夜间保温, 且可靠性高。  (1) The present invention has a simple structure, is light in weight, does not require an additional driving force, and can be applied to a spacecraft for nighttime insulation and has high reliability.
(2) 使用多个并联的丝网蒸发器与热源表面耦合, 这些丝网蒸发器可以均 匀的布置在热源表面, 使得热源温度更均匀; 且丝网蒸发器具有毛细结构, 便 于吸收液体分流器中的液态工质, 减小蒸发器的过热度, 能够传递更多的热量。  (2) Coupling with a plurality of parallel screen evaporators on the surface of the heat source, these screen evaporators can be evenly arranged on the surface of the heat source to make the temperature of the heat source more uniform; and the screen evaporator has a capillary structure for absorbing liquid shunts The liquid working medium reduces the superheat of the evaporator and can transfer more heat.
(3) 将蒸气汇流器设计为 1/4开口的环形结构形式, 能够更好地适应由于 同位素核源温度变化(在 110〜240°C之间变换) 导致蒸发器热胀冷缩带来的热应 力。  (3) The vapor manifold is designed as a 1/4-open annular structure, which can better adapt to the thermal expansion and contraction of the evaporator due to the temperature change of the isotope source (changed between 110~240 °C). Thermal Stress.
(4) 将蒸气管路设置成倒 U型, 可以避免冷凝器中的液态工质回流至蒸气 管路中。  (4) Set the vapor line to an inverted U shape to prevent the liquid working fluid in the condenser from flowing back into the vapor line.
(5) 将冷凝管路设计为 V型, 使得月面倾斜不超过 15° 的情况下避免储 液器中的液态工质倒流入冷凝器中, 造成的不利影响。  (5) The condensing line is designed to be V-shaped, so that the liquid working medium in the reservoir can be prevented from flowing back into the condenser when the lunar slope is not more than 15°.
(6) 采用电磁阀可以有效实现流体回路的多次开闭, 实现月昼阻断传热, 月夜传递热量的功能。 采用密封比压为 4.51Mpa, 控制阀密封面上下压差为 0.2MPa的电磁阀可以满足控制阀的密闭可靠性, 并能承受探测器在发射段和动 力下降段带来的轴向加速度, 满足探测器飞行期间控制阀的密闭可靠性。 附图说明 (6) The solenoid valve can effectively realize multiple opening and closing of the fluid circuit, and realize the heat transfer of the moon shackle. The function of transferring heat on the moon night. The solenoid valve with a sealing specific pressure of 4.51Mpa and a pressure difference of 0.2MPa on the sealing surface of the control valve can meet the sealing reliability of the control valve and can withstand the axial acceleration of the detector in the launching section and the power lowering section. The sealing reliability of the control valve during the flight of the detector. DRAWINGS
图 1为本发明结构示意图。  Figure 1 is a schematic view of the structure of the present invention.
图 2为蒸发器结构示意图。  Figure 2 is a schematic view of the structure of the evaporator.
图 3为丝网蒸发器结构示意图。  Figure 3 is a schematic view of the structure of the screen evaporator.
图 4为冷凝器结构示意图。  Figure 4 is a schematic view of the structure of the condenser.
图 5为储液器结构示意图。  Figure 5 is a schematic view of the structure of the accumulator.
图 6为控制阀结构示意图。  Figure 6 is a schematic view of the structure of the control valve.
其中, 1-蒸发器, 2-蒸汽管路, 3-冷凝器, 4-储液器, 5-控制阀, 6-液体管 路, 7-丝网蒸发器, 8-液体分流器, 9-蒸汽汇流器, 10-充液管, 11-三通, 12-二 通, 13-四通, 14-蒸发器壳体, 15-集热座, 16-冷凝管路, 17-冷凝翅片。 具体实施方式  Of which, 1-evaporator, 2-vapor line, 3-condenser, 4-reservoir, 5-control valve, 6-liquid line, 7-wire evaporator, 8-liquid splitter, 9- Steam manifold, 10-filled pipe, 11-three-way, 12-two-way, 13-four-way, 14-evaporator housing, 15-collector, 16-condensing line, 17-condensing fin. detailed description
下面结合附图并举实施例, 对本发明进行详细描述。  The present invention will be described in detail below with reference to the drawings and embodiments.
本发明提供了一种重力驱动两相流体回路, 如图 1所示, 包括蒸发器 1 (包 括丝网蒸发器 7、 液体分流器 8和蒸气汇流器 9)、 蒸气管路 2、 冷凝器 3、 储液 器 4、 液体管路 6和控制阀 5, 其中, 冷凝器 3位于储液器 4重力场上方、 并与 需要保温的设备 (热沉) 耦合, 蒸发器 1位于储液器 4重力场的下方、 并与同 位素热源耦合安装, 储液器 4内液面和蒸发器 1底部之间形成重力驱动高度差; 储液器 4通过液体管路 6连接至蒸发器 1入口, 在液体管路 6上设有控制间 5, 蒸发器 1出口依次通过蒸气管路 2、 冷凝器 3连接至储液器 4, 形成封闭的管路 系统。 回路内部充有在 -70°C〜120°C范围内处于气液两相态的工质,如氨, 利用 其气液相变进行热量传递。 月夜期间, 控制阀 5打开, 由于储液器 4和蒸发器 1 底部存在一定的高度差, 在重力驱动下, 储液器 4 中的液态氨工质沿着液体管 路 6流入蒸发器 1 中, 蒸发器 1 中的氨工质吸收同位素热源的热量并相变成气 体, 气态的氨工质顺着蒸气管路 2流至冷凝器 3 冷凝为液体, 将热量传递至月 面探测器设备, 冷凝后的液态氨工质流入储液器 4 中, 形成导热回路, 对天体 探测器进行保温。 月昼期间, 需要阻断热量的传递, 此时关闭控制阀 5, 重力驱 动两相流体回路停止运行, 此时, 同位素热源与探测器内部之间的热量传递通 过蒸气管路的导热进行, 传热量很小, 从而实现热隔离, 此时, 同位素核热源 的热量通过自身的热辐射向外散失。 The present invention provides a gravity driven two-phase fluid circuit, as shown in FIG. 1, including an evaporator 1 (including a wire mesh evaporator 7, a liquid flow divider 8 and a vapor manifold 9), a vapor line 2, and a condenser 3 a reservoir 4, a liquid line 6 and a control valve 5, wherein the condenser 3 is located above the gravity field of the accumulator 4 and coupled to a device (heat sink) requiring heat preservation, the evaporator 1 is located at the accumulator 4 gravity Below the field, coupled with an isotope heat source, a gravity driven height difference is formed between the liquid level in the reservoir 4 and the bottom of the evaporator 1; the reservoir 4 is connected to the inlet of the evaporator 1 through the liquid line 6, in the liquid tube There is a control room 5 on the road 6. The outlet of the evaporator 1 is connected to the accumulator 4 through the vapor line 2 and the condenser 3 in sequence to form a closed piping system. The inside of the circuit is filled with a working fluid in a gas-liquid two-phase state, such as ammonia, in the range of -70 ° C to 120 ° C, and the heat transfer is performed by using the gas-liquid phase change. During the moonlight night, the control valve 5 is opened. Due to the certain height difference between the reservoir 4 and the bottom of the evaporator 1, the liquid ammonia working fluid in the accumulator 4 flows into the evaporator 1 along the liquid line 6 under the driving of gravity. The ammonia working fluid in the evaporator 1 absorbs the heat of the isotope heat source and is transformed into a gas. The gaseous ammonia working fluid flows along the vapor line 2 to the condenser 3 to condense into a liquid, and transfers the heat to the lunar surface detector device. The condensed liquid ammonia working fluid flows into the accumulator 4 to form a heat conduction loop for keeping the celestial detector warm. During the lunar period, it is necessary to block the transfer of heat. At this time, the control valve 5 is closed, and the gravity-driven two-phase fluid circuit stops running. At this time, the heat transfer between the isotope heat source and the inside of the detector is conducted through the heat conduction of the vapor line. The heat is small to achieve thermal isolation, at which point the heat of the isotope nuclear heat source is dissipated outward by its own thermal radiation.
其中, 蒸发器 1的结构如图 2所示, 包括 4个丝网蒸发器 7、 蒸气汇流器 9、 液体分流器 8、 充液管 10和接头 (二通、 三通、 四通), 丝网蒸发器 7的结构如 图 3所示, 由蒸发器壳体 14和集热座 15组成, 蒸发器壳体 14安装在集热座 15 的内部, 集热座 15与同位素热源导热安装, 蒸发器壳体 14 内側周向壁面开设 有螺纹槽, 蒸发器壳体 14内部套装烧结的不锈钢丝网作为毛细芯。 蒸气汇流器 9为 1/4开口的圆环形, 如图 2所示, 由 2个二通 12、 1个三通 11、 1个四通 13 和 3个弯管组成, 有 4个蒸气进口和 1个蒸气出口, 其中, 4个蒸气进口分别与 4个丝网蒸发器的出口连接, 蒸气出口与蒸气管路 2连接。 同时, 蒸气汇流器 9 上还设有两相流体回路的充液管 10。 液体分流器为圆环形, 由 3个三通 11、 1 个四通 13和 4个弯管组成, 有 1个液体进口、 4个液体出口, 其中, 液体进口 与液体管路 6连接, 4个液体出口分别与 4个丝网蒸发器 7的入口连接。 其中, 蒸发器壳体 14、 充液管 10和接头的材料为 00Crl7Nil4Mo2 , 集热座的材料为 3A21铝。 储液器 4中的液态氨工质经液体管路 6流入液体分流器 8, 在重力作 用下流入丝网蒸发器 7 中吸收同位素核热源的热量相变为气态, 气态的氨工质 经蒸气汇流器 9汇合后流入蒸气管路 2。 The structure of the evaporator 1 is as shown in FIG. 2, and includes four wire mesh evaporators 7, a vapor manifold 9, a liquid flow divider 8, a liquid filling pipe 10, and a joint (two-way, three-way, four-way), and wire. The structure of the net evaporator 7 is as shown in FIG. 3, and is composed of an evaporator casing 14 and a heat collecting seat 15. The evaporator casing 14 is installed inside the heat collecting seat 15, and the heat collecting seat 15 is thermally connected to the isotope heat source to evaporate. The inner circumferential wall surface of the casing 14 is provided with a threaded groove, and the interior of the evaporator casing 14 is provided with a sintered stainless steel wire mesh as a capillary core. The vapor manifold 9 is a 1/4-open circular ring. As shown in Fig. 2, it consists of two two-way 12, one three-way 11, one four-way 13 and three elbows. There are four steam inlets. And a vapor outlet, wherein the four vapor inlets are respectively connected to the outlets of the four screen evaporators, and the vapor outlets are connected to the vapor line 2. At the same time, the vapor manifold 9 is also provided with a liquid filling tube 10 of a two-phase fluid circuit. The liquid diverter is annular and consists of three tees 11, one four-way 13 and four elbows, one liquid inlet and four liquid outlets, wherein the liquid inlet is connected to the liquid line 6, 4 The liquid outlets are respectively connected to the inlets of the four screen evaporators 7. Wherein, the material of the evaporator casing 14, the liquid filling pipe 10 and the joint is 00Crl7Nil4Mo2, and the material of the heat collecting seat is 3A21 aluminum. The liquid ammonia working fluid in the liquid storage device 4 flows into the liquid flow divider 8 through the liquid pipeline 6, and flows into the screen evaporator 7 by gravity to absorb the heat of the isotope nuclear heat source into a gaseous state, and the gaseous ammonia working fluid passes through the vapor. The combiner 9 merges and flows into the vapor line 2.
蒸气管路 2的材料为 00Crl7Nil4Mo2, 为了避免月昼期间由于储液器 4的 位置高于蒸发器 1 , 导致冷凝器 3和储液器 4中的液态工质回流入蒸发器 1, 蒸 发器 1又将液态工质变成蒸气, 送回冷凝器管路 5, 从而使得探测器设备仍处于 供热状态的情况, 本发明将蒸气管路 2靠近冷凝器 3—端设置成倒 U型, 从而 使得倒 U型蒸气管路 2的底高于冷凝器 3和储液器 4, 抑制了液态工质的回流。  The material of the steam line 2 is 00Crl7Nil4Mo2, in order to avoid the liquid working medium in the condenser 3 and the accumulator 4 flowing back into the evaporator 1 due to the position of the accumulator 4 being higher than the evaporator 1 during the lunar period, the evaporator 1 The liquid working medium is turned into a vapor and sent back to the condenser line 5, so that the detector device is still in a heating state. The present invention sets the vapor line 2 close to the condenser 3 end to an inverted U shape, thereby The bottom of the inverted U-shaped vapor line 2 is made higher than the condenser 3 and the accumulator 4, and the reflux of the liquid working medium is suppressed.
冷凝器 3由冷凝管路 16和冷凝翅片 17组成, 如困 4所示, 冷凝管路 16的 材料为 00Crl 7Nil4Mo2, 冷凝翅片 17的材料为 3A21铝。 为了避免因月面倾斜 导致的储液器高度大于冷凝器高度, 从而使得储液器中的液态工质流入冷凝器 中, 造成不利影响, 本发明将冷凝管路设计为 V型, 其中, 冷凝管路入口一侧 的管路与月面平行, 冷凝管路出口一側的管路位于入口管路的重力场下方且与 入口管路成 15° 角, 从而可以避免月面倾斜 15度的情况下,储液器内的液态工 质不会倒流至冷凝器中。  The condenser 3 is composed of a condensing line 16 and a condensing fin 17, as shown in Figure 4, the material of the condensing line 16 is 00Crl 7Nil4Mo2, and the material of the condensing fin 17 is 3A21 aluminum. In order to avoid that the height of the reservoir due to the inclination of the lunar surface is greater than the height of the condenser, so that the liquid working medium in the accumulator flows into the condenser, causing adverse effects, the present invention designs the condensing line to be V-shaped, wherein, the condensation The pipeline on the inlet side of the pipeline is parallel to the lunar surface, and the pipeline on the outlet side of the condensing pipeline is located below the gravity field of the inlet pipeline and at an angle of 15° to the inlet pipeline, thereby avoiding the inclination of the lunar surface by 15 degrees. The liquid working fluid in the reservoir does not flow back into the condenser.
控制阀 5为电磁阀,其结构如图 6所示,控制阀壳体材料为 00Crl 7Nil4Mo2 不锈钢, 密封部分材料为橡胶。 其利用永磁铁吸力和介质压力共同作用在密封 面上, 产生密封比压, 本发明中, 采用 4.51MPa密封比压, 在橡胶软密封结构 上可以确保 Ι .Οχ ΙΟ·4 Pa-m3/s漏率, 满足技术指标内漏率不超过 1.0x l(T3 Pa rnVs 要求。 此外, 控制阀 5 在探测器发射段和动力下降段还承受着加速度, 液态氨 工质与控制阀密封结构间处于挤压状态, 控制阀 5处于密封状态, 不会被打开, 从而保证了两相流体回路在探测器加速、 减速飞行过程中的可靠性。 同时, 根 据挤压产生的压强公式 Ρ=/^/ζ可知, 当液态氨工质密度最大、 加速度最大、 储 液器中液态氨的液面与控制阀密封结构高度差最大时, 产生的压强最大。 当控 制阀密封面上下压差为 0.2MPa时,可以承受探测器在发射段和动力下降段因加 速或减速氨与控制阀密封结构间的压力对密封结构的影响。 The control valve 5 is a solenoid valve, and its structure is shown in FIG. 6. The material of the control valve housing is 00Crl 7Nil4Mo2 stainless steel, and the sealing portion is made of rubber. The utility model utilizes the permanent magnet suction force and the medium pressure to act on the sealing surface to generate the sealing specific pressure. In the present invention, the sealing specific pressure of 4.51 MPa is adopted, and the rubber soft sealing structure can ensure the Ι.Οχ ΙΟ· 4 Pa-m 3 / s leak rate, meet the technical index internal leakage rate does not exceed 1.0xl (T 3 Pa rnVs requirements. In addition, the control valve 5 is also subjected to acceleration in the detector launch section and the power down section, between the liquid ammonia working fluid and the control valve sealing structure In the squeeze state, the control valve 5 is in a sealed state and will not be opened, thereby ensuring the reliability of the two-phase fluid circuit during the acceleration and deceleration of the detector. Meanwhile, the pressure formula according to the extrusion Ρ=/^ /ζ knows that when liquid ammonia has the highest density, maximum acceleration, and storage When the height difference between the liquid level of the liquid ammonia and the control valve sealing structure is the largest, the generated pressure is the largest. When the pressure difference between the sealing surface of the control valve is 0.2 MPa, it can withstand the influence of the pressure between the detector and the power-down section of the detector on the sealing structure due to the acceleration or deceleration of the ammonia and the sealing structure of the control valve.
储液器 4 和工质充装量的匹配设计关系到两相流体回路的安全性和传热性 能, 储液器在月昼期间应能容纳回路内的绝大部分工质, 从而避免液态工质在 温度升高时体积膨胀, 导致回路破裂, 确保整个流体回路的安全; 同时, 在流 体回路工作时, 储液器内工质液面高度随工作温度的变化应尽可能小, 从而使 储液器液面高度距蒸发器 1 底部的高度差所对应的重力驱动力随温度变化尽可 能小, 一方面可以减弱由于液面波动对回路工作稳定性造成的影响, 另一方面 也可以确保在液面最低时仍能提供足够的驱动力。 储液器 4的结构如图 5所示, 为圆柱体, 其上下端面为椭球形, 其中, 为了减小不同工作温度时储液器液面 的高度变化量, 储液器在满足布局和重量要求的情况下, 内径应尽可能大。  The matching design of the accumulator 4 and the filling amount of the working fluid is related to the safety and heat transfer performance of the two-phase fluid circuit. The accumulator should be able to accommodate most of the working fluid in the circuit during the lunar period, thereby avoiding the liquid working. The volume expands when the temperature rises, causing the circuit to rupture, ensuring the safety of the entire fluid circuit. At the same time, when the fluid circuit is working, the liquid level of the working fluid in the reservoir should be as small as possible with the working temperature, so that the storage The gravity driving force corresponding to the height difference between the liquid level of the liquid level and the bottom of the evaporator 1 is as small as possible with temperature, which on the one hand can reduce the influence of the liquid level fluctuation on the stability of the circuit operation, and on the other hand, can ensure Provides sufficient driving force when the liquid level is lowest. The structure of the accumulator 4 is as shown in Fig. 5, which is a cylinder whose upper and lower end faces are ellipsoidal. In order to reduce the height change of the liquid level of the accumulator at different working temperatures, the accumulator satisfies the layout and weight. The inner diameter should be as large as possible if required.
工质充装量与储液器体积之间进行匹配设计: 利用质量=密度'体积,联立最 高和最低储存温度下工质质量计算方程, 获得储液器体积与工质充装量; 其中, 最高储存温度下, 储液器内液体充满率为 100%, 外回路均为气体; 最低储存温 度下, 外回路充满液体, 储液器中含有体积分数为 10%的液态工质; 其中, 所 述外回路由流体回路中除去储液器的其余部分組成, 其体积已知。  Matching design between the filling amount of the working fluid and the volume of the accumulator: Using the mass = density 'volume, the equation for calculating the mass of the working medium at the highest and lowest storage temperatures, the volume of the accumulator and the filling amount of the working fluid are obtained; At the highest storage temperature, the liquid filling rate in the liquid reservoir is 100%, and the outer circuit is gas; at the lowest storage temperature, the outer circuit is filled with liquid, and the liquid storage medium contains a liquid working medium having a volume fraction of 10%; The outer circuit consists of the remainder of the fluid circuit that removes the reservoir, the volume of which is known.
液体管路 6的材料为 00Crl7Nil4Mo2不锈钢。  The material of the liquid line 6 is 00Crl7Nil4Mo2 stainless steel.
综上所述, 以上仅为本发明的较佳实施例而已, 并非用于限定本发明的保 护范围。 凡在本发明的精神和原则之内, 所作的任何修改、 等同替换、 改进等, 均应包含在本发明的保护范围之内。  In conclusion, the above is only a preferred embodiment of the present invention and is not intended to limit the scope of the present invention. Any modifications, equivalent substitutions, improvements, etc. made within the spirit and scope of the present invention are intended to be included within the scope of the present invention.

Claims

权 利 要 求 书 Claim
1、 一种重力驱动两相流体回路, 其特征在于, 包括蒸发器 (1 )、 蒸气管路1. A gravity driven two-phase fluid circuit, characterized in that it comprises an evaporator (1), a vapor line
(2)、 冷凝器 (3)、 储液器 (4)、 液体管路 (6) 和控制阀 (5) ; 其中, 冷凝器(2), condenser (3), accumulator (4), liquid line (6) and control valve (5); wherein, condenser
(3) 位于储液器 (4) 重力场上方、 并与需要保温的设备耦合; 蒸发器 (1 ) 位 于储液器 (4) 重力场的下方、 并与同位素热源耦合安装; 储液器 (4) 通过液 体管路 (6) 连接至蒸发器 (1 ) 入口, 并在液体管路 (6) 上设有控制阀 (5) ; 蒸发器 (1 ) 出口依次通过蒸气管路 (2)、 冷凝器 (3) 连接至储液器 (4) , 形 成封闭的管路系统; 其中, 所述冷凝器 (3) 由冷凝管路(16) 和冷凝翅片 (17) 组成, 所述冷凝管路 (16) 为 V型, 冷凝管路入口一側的管路与月面平行, 冷 凝管路出口一側的管路与出口管路在同一垂面上, 并位于入口管路下方且与入 口管路成 15° 角; 回路内部充有在 -70°C〜120°C范围内处于气液两相态的工质。 (3) Located above the gravity field of the accumulator (4) and coupled to the equipment to be insulated; the evaporator (1) is located below the gravity field of the accumulator (4) and is coupled to the isotope heat source; the accumulator ( 4) Connect to the evaporator (1) inlet through the liquid line (6) and set the control valve (5) on the liquid line (6); the evaporator (1) outlet passes through the vapor line (2) in turn, The condenser (3) is connected to the accumulator (4) to form a closed piping system; wherein the condenser (3) is composed of a condensation line (16) and a condensation fin (17), the condensation tube The road (16) is V-shaped, the pipeline on the inlet side of the condensing pipeline is parallel to the lunar surface, and the pipeline on the outlet side of the condensing pipeline is on the same vertical plane as the outlet pipeline, and is located below the inlet pipeline and with the inlet The pipeline is at an angle of 15°; the inside of the circuit is filled with a working fluid in a gas-liquid two-phase state in the range of -70 ° C to 120 ° C.
2、 如权利要求 1所述的重力驱动两相流体回路, 其特征在于, 所述蒸发器 ( 1 ) 包括 4 个丝网蒸发器 (7)、 蒸气汇流器 (9) 和液体分流器 (8), 其中, 丝网蒸发器 (7) 由蒸发器壳体 (14) 和套装在蒸发器壳体上的集热座 (15) 組 成, 所述集热座 (15) 与同位素核热源导热安装, 蒸发器壳体 (14) 内侧周向 壁面开设有螺纹槽, 壳体内部套装烧结的不锈钢丝网作为毛细芯; 丝网蒸发器 (7) 的入口与液体分流器(8) 连接, 丝网蒸发器(7) 的出口与蒸气汇流器(9) 连接; 液体分流器(8) 与液体管路(6) 连接, 蒸气汇流器(9) 与蒸气管路(2) 连接。  2. A gravity driven two-phase fluid circuit according to claim 1, characterized in that said evaporator (1) comprises four wire mesh evaporators (7), a vapor manifold (9) and a liquid splitter (8). Wherein, the wire mesh evaporator (7) is composed of an evaporator casing (14) and a heat collecting seat (15) fitted on the evaporator casing, and the heat collecting seat (15) is thermally insulated from the isotope nuclear heat source. The inner side wall surface of the evaporator casing (14) is provided with a thread groove, and the inside of the casing is provided with a sintered stainless steel wire mesh as a capillary core; the inlet of the wire mesh evaporator (7) is connected with the liquid flow divider (8), the wire mesh The outlet of the evaporator (7) is connected to the vapor manifold (9); the liquid splitter (8) is connected to the liquid line (6), and the vapor manifold (9) is connected to the vapor line (2).
3、 如权利要求 2所述的重力驱动两相流体回路, 其特征在于, 所述蒸气汇 流器 (9) 为 1/4开口的环形结构, 所述液体分流器 (8) 为环形结构。  3. A gravity driven two-phase fluid circuit according to claim 2, wherein said vapor manifold (9) is a 1/4 open annular structure and said liquid flow divider (8) is annular.
4、 如权利要求 1所述的重力驱动两相流体回路, 其特征在于, 所述蒸气管 路 (2) 靠近冷凝器 (3) 的一端为倒 U型, 倒 U型的蒸气管路的底高于冷凝器 (3) 的入口。 4. The gravity driven two-phase fluid circuit according to claim 1, wherein one end of the vapor line (2) adjacent to the condenser (3) is inverted U-shaped, and the bottom of the U-shaped vapor line is inverted. Above the condenser (3) The entrance.
5、 如权利要求 1所述的重力驱动两相流体回路, 其特征在于, 所述控制阀 (5) 为电磁阀, 其密封比压为 4.51Mpa, 控制阀密封面上下压差为 0.2MPa。  The gravity-driven two-phase fluid circuit according to claim 1, wherein the control valve (5) is a solenoid valve having a sealing specific pressure of 4.51 MPa and a pressure difference of 0.2 MPa on the sealing surface of the control valve.
6、 如权利要求 1所述的重力驱动两相流体回路, 其特征在于, 所述工质为 氨。  6. The gravity driven two phase fluid circuit of claim 1 wherein said working fluid is ammonia.
7、 如权利要求 1所述的重力驱动两相流体回路, 其特征在于, 所述工质的 充装量计算方法为: 利用质量=密度 *体积, 联立最高和最低储存温度下工质质 量计算方程, 获得储液器体积与工质充装量; 其中, 最高储存温度下, 储液器 内液体充满率为 100%, 外回路均为气体; 最低储存温度下, 外回路充满液体, 睹液器中含有体积分数为 10%的液态工质; 其中, 所述外回路由流体回路中除 ^储液器的其余部分组成, 其体积已知。  7. The gravity driven two-phase fluid circuit according to claim 1, wherein the filling amount of the working fluid is calculated by: using mass=density* volume, and working medium quality at maximum and minimum storage temperatures. Calculate the equation to obtain the volume of the accumulator and the filling amount of the working fluid; wherein, at the highest storage temperature, the liquid filling rate in the accumulator is 100%, the outer loop is gas; at the lowest storage temperature, the outer loop is filled with liquid, 睹The liquid reservoir contains a liquid working medium having a volume fraction of 10%; wherein the outer circuit is composed of the remaining portion of the fluid circuit except the liquid storage device, and the volume thereof is known.
PCT/CN2015/000301 2014-12-02 2015-05-04 Gravity-driven two-phase fluid loop WO2016086495A1 (en)

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