CN1059014A - 将低温热量变换成电能的方法和设备 - Google Patents

将低温热量变换成电能的方法和设备 Download PDF

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CN1059014A
CN1059014A CN91105805A CN91105805A CN1059014A CN 1059014 A CN1059014 A CN 1059014A CN 91105805 A CN91105805 A CN 91105805A CN 91105805 A CN91105805 A CN 91105805A CN 1059014 A CN1059014 A CN 1059014A
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阿历山大·I·卡林纳
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F01MACHINES OR ENGINES IN GENERAL; ENGINE PLANTS IN GENERAL; STEAM ENGINES
    • F01KSTEAM ENGINE PLANTS; STEAM ACCUMULATORS; ENGINE PLANTS NOT OTHERWISE PROVIDED FOR; ENGINES USING SPECIAL WORKING FLUIDS OR CYCLES
    • F01K25/00Plants or engines characterised by use of special working fluids, not otherwise provided for; Plants operating in closed cycles and not otherwise provided for
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    • F01K25/065Plants or engines characterised by use of special working fluids, not otherwise provided for; Plants operating in closed cycles and not otherwise provided for using mixtures of different fluids with an absorption fluid remaining at least partly in the liquid state, e.g. water for ammonia
    • YGENERAL 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
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    • Y02E10/46Conversion of thermal power into mechanical power, e.g. Rankine, Stirling or solar thermal engines

Abstract

实施热力循环的一种方法和设备,能将低温热量 变换成电能。

Description

本发明总的说来涉及热能变换成机械能再变换成电能的技术领域。更具体地说,本发明涉及低温热源的低温热变换成电能的过程。
低温热源的热能变换成电能的方法是能量生产的一个重要领域。目前有这样一种需要,即要求提供提高这种低温热变换成电能的效率的方法和设备,使其超过标准兰金循环的效率。本发明就为提供这种方法和设备。
本发明提供一种实施热力循环的方法,该方法包括下列步骤:
令气态工(作介)质流膨胀,将其能量转变成有用的形式,并产生废流;
令废流冷凝,由此产生液态工质流;
从液态工质流形成富集流和贫流;和
加热富集流,由此形成气态工质流。
本发明还提供一种实施热力循环的设备,该设备包括:
膨胀装置,用以使气态工质流膨胀,将其能量转变成有用形式,并产生废流;
一第一料流混合器,用以混合废流与贫流,形成预冷凝流;
一冷凝器,用以冷凝所述预冷凝流,产生液态工质流;
一台泵,用以泵送该液态工质流,使其压力增高;
一重力分离器,用以从液态工质流形成蒸汽流和第一液态流;
一第一料流分离器,用以分离第一液态流,产生第二液态流和贫流;
一第二料流混合器,用以混合第二液态流与蒸汽流,产生富集流;和
一热交换器,用以用外热源传来的热量加热富集流,产生气态工质流。
虽然通常可用普通的外热源来与本发明的方法和设备配用,但本发明特别适宜变换来自低温地热海水或来自太阳池的低温热量。从下面对诸最佳实施例的说明可以看出,本发明的方法和设备能提高采用低温热源的能量循环中低温热变热成电能的效率。
图1是本发明方法和设备的一个实施例的原理图。
本发明是实施热力循环的一种新方法和设备。在本发明的方法中,气态工质流是经过膨胀的。此膨胀过程将工质流的能量转换成有用的形式并产生废流。最佳膨胀装置包括普通常用的涡轮机或涡轮机系。废流经冷凝产生液态工质流。冷凝器最好是现有技术中普通使用的那种。
从液态工质流形成富集流和贫流。富集流中的低沸点组分百分比含量最好高于液态工质流的。贫流的低沸点组分百分比含量最好低于液态工质流的。从液态工质流制造贫流和富集流可采用任何能从单种料流制造两种或多种具有不同组分的料流的普通设备。制备这些料流的装置最好是普通常用的重力分离器,例如普通的闪蒸箱。
富集流最好处于蒸汽状态或汽-液混合状态。贫流最好处于饱和状态或过冷液体状态。
富集流经加热形成气态工质流。该传热过程可经由普通的热交换器进行。加热源可采用任何传统形式的加热源,包括同流换热式热源或外热源。可用于本发明的外热源最好是那些温度低于大约400°F的外热源。特别理想的是那些温度低于250°F的外热源,例如低温地热海水或太阳池外热源。
本发明的方法最好加上这样一个步骤:废流在冷凝形成液态工质流之前先与贫流在第一料流混合器中混合。这种含贫流和废流的料流可以叫做预冷凝流。
本发明的方法最好加上这样一个步骤:用泵提高液态工质流的压力,并用废流和贫流传来的热量使液态工质流部分蒸发。为达到此目的可采用普通的泵和热交换器。
在本发明液态工质流被部分蒸发的实施例中,可以在闪蒸箱将部分蒸发了的液态工质流分离成汽流和液流来形成富集流和贫流-蒸汽产生富集流,富集流经加热形成气态工质流,和产生贫流的液体。不然也可以在闪蒸箱把这种部分蒸发了液态工质流分离成汽流和第一液流。第一液流又可在第一料流分离器分离成第二液流和贫流。然后将第二液流在第二料流混合器与汽流混合生成富集流。在本发明的这个实施例中,富集流应处于汽-液混合料的状态,这个混合料经加热形成气态工质流。
图1的原理图示出了可用于本发明的方法中较理想设备的一个实施例。具体地说,图1示出了系统100,该系统包括涡轮机101,热交换器104、105和102,冷凝器106,重力分离器103,泵108,料流分离器109和111,料流混合器110、112和114,以及外热源113。
冷凝器106可以是任何类型的已知热耗损设备。例如,冷凝器106可取热交换器的形式,如水冷系统或其它类型的冷凝设备。
驱动本发明的循环可采用各种形式的热源。在图1所示的实施例中,外热源113表示从点1经由热交换器102流至点9的低温地热流体流。
本发明实施例在系统100中所示的工质流最好是含有低沸点组分和高沸点组分的多组分工质流。这类较理想的工质流可以是氨-水混合料、两种或多种烃类、两种或多种氟利昂、烃和氟利昂的混合料等等。一般说来,工质流可以是任何数目热力学性能和溶解度都良好的化合物组成的混合料。在特别值得推荐的实施例中,采用了水与氨的混合料。
如图1所示,工质流在系统100中循环。该工质流包括从热交换器102流向涡轮机101的气态工质流。该工质流还包括从涡轮机101流向第一料流混合器114的废流、从第一料流混合器114流向冷凝器106的预冷凝流、从冷凝器106流向重力分离器103的液态工质流和从第二料流混合器112流向热交换器102的富集流。气态工质流、废流和富集流中所含的低沸点组分百分比最好比预冷凝流和液态工质流中所包含的高。
在系统100中流通的除工质流外还有从第一料流分离器111流向第一料流混合器114的贫流、从重力分离器103流向第一料流分离器111的第一液流、从第一料流分离器111流向第二料流混合器112的第二液流和从重力分离器103流向第二料流混合器112的汽流。贫流、第一液流和第二液流中各自的低沸点组分百分比含量最好低于液态工质流中的。汽流所含低沸点组分百分比最好要比液态工质流中的高。
在本发明图1所示的实施例中,液态工质流是经过彻底冷凝的,其温度最好接近环境温度,其参数如点14处所示,该液态工质流用泵108提高其压力之后,获得如点21所示参数。然后该液态工质流在料流分离器109经过分离之后产生分流,其参数分别如点61和62处所示。这些分流分别传送到同流换热式热交换器104和105。液态工质流的各分流流经热交换器104和105时经过加热,温度达到沸点,其参数分别如点7和4处所示,然后再经过部分蒸发。液态工质流经部分蒸发的分流从热交换器104和105出来之后,其参数分别如点63和64处所示。这些分流接着在料流混合器110中重新混合,重新组成其参数如点5处所示的液态工质流。
点5处的液态工质流最好处于双相状态,即,处于部分蒸发状态。该液态工质流传送到重力分离器103(例如闪蒸箱)中,在那里液体从蒸汽中分离出来。
具有如点6处所示参数的汽流从重力分离器103的顶部出来,具有如点10处相同参数的第一液流则从重力分离器103的底部出来。第一液流在第一料流分离器111被分离成分别具有如点11和13处相同参数的贫流和第二液流。第二液流,其参数如点13处所示,在第二料流混合器112与汽流混合,产生具有如点69处相同参数的富集流(在本发明的本实施例中“富集”是指富集流在低沸点组分方面比液态工质流丰富)。该富集流最好处在汽-液混合状态。
富集流送入热交换器102中,在那里为外热源113所加热。图1中所示的外热源113是个地热海水流。这类热源一般温度低于大约400°F,还可能低于大约250°F。此外外热源113也可由一些其它类型的低温料流组成,例如流自太阳池的低温料流。在图1所示的实施例中,地热海水进入热交换器102中,这时具有如点1处参数,再从热交换器102中出来,这时其参数如点9处的一样。如表一所示,点1处的地热海水其温度可能达230°F。
进入热交换器102的富集流经过进一步加热和蒸发之后,作为气态工质流从热交换器102中出来。从热交换器102出来的气态工质流可以是部分蒸发,也可以是完全蒸发处于过热状态。
图1实施例中的气态工质流从热交换器102出来时其参数与点30处的一样。然后气态工质流进入涡轮机101中,在涡轮机101中膨胀作功。废流从涡轮机101中出来时其参数与点36处的一样。该废流送入热交换器105中冷却。废流通过热交换器105中时最好处于部分冷凝状态,以获取与点38处一样的参数。废流通过热交换器105时传递热量,用以加热而且最好部分蒸发液态工质流从点62流至点64的支流。
参数与点11处的一样的贫流通过热交换器104,在交换器104中冷却。贫流通过热交换器104时提供热量,供预热而且最好部分蒸发从点61流至点63的液态工质流的支流之用。贫流从热交换器104出来时其参数与点20处的一样。在图1所示的实施例中,贫流通过减压装置107,该装置可以是一个节流阀。从减压装置107出来之后,贫流获得如点19处相同的参数。
在第一料流混合器114处,贫流与废流混合,产生具有如点29处相同参数的预冷凝流。该预冷凝流送入冷凝器106中,在冷凝器106中为自点23流至点24的冷却剂流彻底冷凝。经此冷凝产生了参数与点14处的一样的液态工质流,于是就完成了整个循环。
具有含49.5重量%的氨的水-氨富集流的一个系统其对应于图1所设各点的合适参数如表一所示。表2列出了采用图1所示实施例中表一各参数的本发明系统的理论特性。从该表列出的数据可以看出,本发明提出的系统理论上应有10.34%的效率,这在相同的边界条件下应超过标准兰金循环之效率约1.67倍。采用图1所示实施例的热源,在各参数如表一所列的情况下,预期可使功率输出从3.3兆瓦增加到5.5兆瓦。
表一
点  压力  X  温度°F  热量  G
(磅/平方英寸)  (英热量单位/磅)
1  -  海水  230.00  -  9.6554
2  37.90  0.2651  138.56  30.93  7.4728
3  9.97  0.4950  138.56  467.66  1.0000
4  40.10  0.2922  134.56  20.82  2.9728
5  38.10  0.2922  142.00  58.54  8.4728
6  38.10  0.9408  142.00  634.62  .3403
7  40.10  0.2922  134.56  20.82  5.5000
9  -  BRINE  170.62  -  9.6554
10  38.10  0.2651  142.00  34.44  8.1325
11  38.10  0.2651  142.00  34.44  7.4728
13  38.10  0.2651  142.00  34.44  .6597
14  8.72  0.2922  62.00  -54.06  8.4728
19  9.22  0.2651  76.79  -24.12  7.4728
20  37.70  0.2651  85.03  -24.12  7.4728
21  42.10  0.2922  62.00  -53.99  8.4728
23  -  水  55.00  -  17.4588
24  -  水  84.96  -  17.4588
29  9.22  0.2922  78.76  7.68  8.4728
30  33.10  0.4950  217.50  823.45  1.0000
36  10.72  0.4950  165.00  761.36  1.0000
38  9.22  0.4950  94.37  245.29  1.0000
61  42.10  0.2922  62.00  -53.99  5.5000
62  42.10  0.2922  62.00  -53.99  2.9728
63  38.10  0.2922  133.58  25.53  5.5000
64  38.10  0.2922  158.00  119.61  2.9728
69  38.10  0.4950  142.00  238.67  1.0000
表二
涡轮机的总热函降=62.08英热量单位/磅
涡轮机作功=60.53英热量单位/磅
供热量=84.78英热量单位/磅
热损耗=523.04英热量单位/磅
泵功率消耗=.09英热量单位/磅
净功率输出=60.44英热量单位/磅
净热效率=10.34%
工质重量流量=310705.84
净输出  5502.59KWe
第二定律极限  20.90%
第二定律效率  49.45%
海水消耗率  545.20磅/KWe
单位功率输出  1.83瓦-小时/磅
虽然本发明是就一些最佳实施例进行说明的(这些实施例应用了单一较理想的外热源),但本技术领域的专业人士不难理解,对这些实施例是可以进行一系列变更的。例如,可以采用不同的外热源,可以增加或减少热交换器的数目,可以改变泵、涡轮机、冷凝装置、分离器等的数目,还可以改变流经整个循环通路的料流的数量和组成。因此,本发明书所附的权利要求书旨在包括所有属于本发明精神实质和范围的这类变更和改型。

Claims (14)

1、实施热力循环的一种方法,该方法包括下列步骤:
令一气态工质流膨胀,将其能量转换成有用的形式,并产生废热流;
将废热流冷凝,以产生液态工质流;
从液态工质流形成富集流和贫流;和
加热富集流,形成气态工质流。
2、如权利要求1的方法,其特征在于,它还包括这样一个步骤:在将废热流冷凝形成液态工质流之前将其与贫流进行混合。
3、如权利要求1的方法,其特征在于,它还包括这样一个步骤:用温度小于大约400°F的外热源传来的热量加热富集流。
4、如权利要求3的方法,其特征在于,它还包括这样一个步骤:用温度小于大约250°F的外热源传来的热量加热富集流。
5、如权利要求4的方法,其特征在于,所述外热源选自一组由低温地热海水和太阳池组成的热源。
6、如权利要求1的方法,其特征在于,该方法还包括下列步骤:用泵提高液态工质流的压力,然后再用废流和贫流传来的热量部分蒸发液态工质流。
7、实施热力循环的一种方法,该方法包括下列各步骤:
令一气态工质流膨胀,将其能量转变为有用的形式并产生废流;
将废流与贫流混合形成预冷凝流;
将预冷凝流冷凝,产生液态工质流;
用泵提高该液态工质流的压力;
用废流和贫流传来的热量部分蒸发液态工质流;
从液态工质流形成汽流和第一液流;
将第一液流分离成第二液流和贫流;
将第二液流与汽流混合起来,产生富集流;和
用外热源传来的热量加热富集流,产生气态工质流。
8、权利要求7的方法,其特征在于,所述气态工质流、废流、贫流、预冷凝流、液态工质流、第一液流、第二液流、汽流和富集流各含有一低沸点组分和一高沸点组分。
9、实施热力循环的一种设备,它包括:
膨胀装置,用以使一种气态工质流膨胀,将其能量转变成有用形式并产生废流;
一第一料流混合器,用以将废流与贫流混合成预冷凝流;
一冷凝器,用以冷凝预冷凝流,产生液态工质流;
一台泵,用以提高液态工质流的压力;
一重力分离器,用以从液态工质流形成汽流和第一液流;
一第一料流分离器,用以将第一液流分离成第二液流和贫流;
一第二料流混合器,用以将第二液流与汽流混合生成富集流;和
一热交换器,用以用外热源传来的热量加热富集流,产生气态工质流。
10、如权利要求9的设备,其特征在于,它还包括各包含低沸点组分和高沸点组分的气态工质流、废流、贫流、预冷凝流、液态工质流、第一液流、第二液流、汽流和富集流。
11、如权利要求9的设备,其特征在于,它还包括第二热交换器和第三热交换器,前者用以用贫流传来的热量加热液态工质流,后者用以用废流传来的热量加热液态工质流。
12、如权利要求9的设备,其特征在于,它还包括一外热源,其温度约小于400°F。
13、如权利要求12的设备,其特征在于,所述外热源的温度小于大约250°F。
14、如权利要求13的设备,其特征在于,所述外热源选自一组由低温地热海水和太阳池组成的热源。
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