TW394814B - Thermal engine with improved efficiency - Google Patents

Thermal engine with improved efficiency Download PDF

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Publication number
TW394814B
TW394814B TW087118937A TW87118937A TW394814B TW 394814 B TW394814 B TW 394814B TW 087118937 A TW087118937 A TW 087118937A TW 87118937 A TW87118937 A TW 87118937A TW 394814 B TW394814 B TW 394814B
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Taiwan
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cycle
gas
water vapor
working medium
scope
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TW087118937A
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Chinese (zh)
Inventor
Martin Ziegler
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Martin Ziegler
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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
    • F01K21/00Steam engine plants not otherwise provided for
    • F01K21/04Steam engine plants not otherwise provided for using mixtures of steam and gas; Plants generating or heating steam by bringing water or steam into direct contact with hot gas
    • F01K21/042Steam engine plants not otherwise provided for using mixtures of steam and gas; Plants generating or heating steam by bringing water or steam into direct contact with hot gas pure steam being expanded in a motor somewhere in the plant
    • 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
    • F01K19/00Regenerating or otherwise treating steam exhausted from steam engine plant
    • F01K19/02Regenerating by compression
    • 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
    • F01K19/00Regenerating or otherwise treating steam exhausted from steam engine plant
    • F01K19/02Regenerating by compression
    • F01K19/04Regenerating by compression in combination with cooling or heating
    • 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
    • F01K25/06Plants 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
    • 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E20/00Combustion technologies with mitigation potential
    • Y02E20/16Combined cycle power plant [CCPP], or combined cycle gas turbine [CCGT]

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  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Combustion & Propulsion (AREA)
  • Mechanical Engineering (AREA)
  • General Engineering & Computer Science (AREA)
  • Engine Equipment That Uses Special Cycles (AREA)

Abstract

The invention concerns a method and a thermal engine for the conversion of thermal energy (Qextern) into mechanical energy (Wextern), the thermal engine comprising a first thermodynamic cyclic process (steam cyclic process) and a second cyclic process (gas cyclic process), the waste heat (QD) of the first cyclic process being supplied to the second cyclic process and the waste heat (QG) of the second cyclic process being supplied to the first cyclic process.

Description

Λ7 、--、--一 _____H? 五、發明説明(i ) ' — 本發明係關於一種於熱動力機將熱能轉成機械能之方 法,其中熱動力機之熱效率增高而無需改變循環過程溫度 上限及/或下限。此外,本發明係關於一種執行此種方法 之熱動力機。 熱動力機為能量轉換器,利用熱動力循環過程將供給 的熱能轉成軸功(=動能)»用於此項目的,熱能於高溫供 給動力機内部之工作介質,然後於通過循環過程後再度於 低溫部分提取。理想情況下,熱能之供給量與提取量之差 對應於動力機之軸功輸出。 此種動力機之循環過程之熱效率為達成的軸功與施加 的主熱能間之比。該比值隨著過程溫度上下限間之差異程 度增高,最大可達到理想卡諾動力機之數值。循環過程之 最大可達成之熱效率以卡諾定律表示: V =(T0-TU)/T0 其中C為循環過程之最大熱效能,T。為過程溫度上限,及 TU為過程溫度下限。 經濟部中央標準局員工消費合作社印裝 f ---------裝—— (請先閱讀背面之注意事^^填寫本頁) .線· 為了對各次施加單位主熱能達到儘可能高之軸功或動 月b產率,熱能必須具有最高可能熱效率。此種目標可藉由 提高循環過程效率達成。為了達到此目的,根據卡諾定律 ,需降低溫度下限及/或提高溫度上限。溫度上限的增高 受限於熱動力機使用物質之熱穩定性。溫度下限的降低也 受限制,原因為習知操作熱動力機之方法中,廢熱係散逸 至環境,對溫度下限下降的自然限度係由熱動力機之周圍 溫度界定(熱動力學第二基本定律)。新鮮水冷卻系統例如 本紙張尺度適财_ I:. ( CNS ) A4規格公釐)_ 4 ΓΓ: 發明説明(2 ) Λ7 B7 經濟部中央標準局員工消費合作社印製Λ7,-, --- _____H? 5. Description of the Invention (i) '— The present invention relates to a method for converting thermal energy into mechanical energy in a thermal power machine, in which the thermal efficiency of the thermal power machine is increased without changing the upper limit of the cycle process temperature And / or lower bound. In addition, the present invention relates to a thermal power machine performing such a method. The thermodynamic engine is an energy converter. It uses the thermodynamic cycle to convert the supplied thermal energy into shaft work (= kinetic energy). »For this project, the thermal energy is supplied to the working medium inside the power engine at high temperature, and then passed to low temperature after passing through the cycle process. Partial extraction. Ideally, the difference between the amount of heat energy supplied and the amount of extraction corresponds to the shaft work output of the power machine. The thermal efficiency of the cycle of such a power machine is the ratio between the achieved shaft work and the applied main thermal energy. The ratio increases with the difference between the upper and lower limits of the process temperature, and can reach the maximum value of the ideal Carnot power machine. The maximum achievable thermal efficiency of the cyclic process is expressed by Carnot's Law: V = (T0-TU) / T0 where C is the maximum thermal efficiency of the cyclic process, T. Is the upper process temperature limit, and TU is the lower process temperature limit. Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs f --------- Installation-(Please read the precautions on the back ^^ Fill this page first). Line · In order to apply the main heat of the unit to the maximum Possibly high shaft work or dynamic monthly b yield, the thermal energy must have the highest possible thermal efficiency. This goal can be achieved by increasing the efficiency of the cycle process. To achieve this, according to Carnot's Law, it is necessary to lower the lower temperature limit and / or increase the upper temperature limit. The increase in the upper temperature limit is limited by the thermal stability of the materials used in the heat engine. The lower limit of the temperature is also limited, because in the conventional method of operating a thermodynamic machine, waste heat is dissipated to the environment. The natural limit for the lower limit of the temperature is defined by the ambient temperature of the thermodynamic machine (the second basic law of thermodynamics). Fresh water cooling systems such as this paper are suitable for the size of the paper _ I:. (CNS) A4 size mm) _ 4 ΓΓ: Description of the invention (2) Λ7 B7 Printed by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs

用於降低絲溫度下限至接近關溫度,但由於環保理由 故不佳’考慮河流及湖泊原先已存在有熱負荷。另外,熱 係透過滋及乾冷卻塔抽取至空中。 也已知為了提高熱動力機效率可藉由以來自輪機之水 蒸氣預熱進水,並提升熱輸入之平均溫度來減少過程廢熱 。此種方法之上限受下述事實所限,若進水之預熱溫度過 高’則锅爐I氣溫度儘管空氣經過預熱仍無法維持於其最 低值。此外,此種形式之廢熱反饋有其缺點,原因為進水 被預熱至廢熱之最高溫度。 也可藉助於近代主電腦使動力機之循環過程之變數最 適化’例如於發電廠之例,現場水蒸氣及中間超熱條件, 預熱器之數量、效率及洩放壓力,冷凝器之尺寸及設計, 冷卻塔之設計等。雖言如此,即使藉助於此等措施效率的 增高仍僅達有限程度。 最後,又一種提高熱動力機效率之方法包含利用儘可 能完整於循環過程連鎖之吸熱與供熱間可利用的溫度梯度 ’而減少熱能吸收與傳送之能量損失。供此目的之用,二 或多動力機串聯連結,前一週期過程之廢熱用作隨後週期 過程之加熱熱。此種方法,例如用於近代組合式電廠(氣 體及水蒸氣電廠),其中燃燒過程之高熱首先用於氣輪機 ’然後其廢氣另外用於加熱水蒸氣發電設備。藉此方式, 減少水蒸氣產生之能量損失,及於若干階段利用存在於燃 燒溫度與周圍溫度間之熱梯度。 串聯偶合循環過程之方法構成專利申請案US 本紙張尺度適用中國國家標準(CNS ) M規格(21〇 X 297公釐) 5 (請先閱讀背面之注意事^填寫本頁) 裝. -線- 五、發明説明(3 ) Λ7 »7 經濟部中央標準局員工消費合作社印製 5,437,157及US 4,428,190之主題,其各有二串聯循環過程 ,及AT 327,299共有三串聯循環過程。 US 5,437,157使用曾知水蒸氣電廠(工作介質水)之冷 凝熱用於氣化有機工作介質,其於第二水蒸氣循環過程產 生有用的功。第二循環過程之廢熱隨後排放至環境。類似 原理用於US 4,428,190,二水蒸氣循環過程(水及有機工作 介質)透過中間熱累加器偶合,意圖改良白晝電廠之負荷 分布。AT 327,299描述鉀及水蒸氣循環過程利用基於有機 工作介質之第三循環過程偶合,有機工作介質將廢熱由鉀 過程傳遞至水過程作為加熱熱。所述各例中,各循環過程 實質彼此分開,熱由一過程傳遞至另一過程係透過熱交換 器壁進行。 循%過程之串聯偶合缺點為各循環過程需要額外傳熱 及能量轉換設備。此外,能量轉換之能的損失隨著串聯偶 合之循環過程數目的增加而增高,原因為利用熱交換器傳 熱僅能維持有限溫差◊又其缺點為串聯連鎖之最末循環過 程之廢熱須排放至周園環境。 因此,本發明之目的係提供一種方法其中可提高熱動 力機之熱效率而無需改變熱循環過程之過程溫度上限及/ 或下限。本發明也有一目的係提供一種執行此種方法之熱 動力機。 此等目的可藉具有如申請專利範圍第丨項之特點之方 法及藉由具有如申請專利範圍第14項之特點之熱動力機 達成。關聯附屬項揭示根據本發明之方法及熱動力機之優It is used to reduce the lower limit of the wire temperature to close to the off temperature, but it is not good for environmental reasons. 'Consider that rivers and lakes already have heat loads. In addition, the heat is extracted into the air through the nourishing dry cooling tower. It is also known that in order to improve the efficiency of a thermodynamic engine, the waste heat of the process can be reduced by preheating the incoming water with steam from the turbine and increasing the average temperature of the heat input. The upper limit of this method is limited by the fact that if the preheating temperature of the inlet water is too high ', the temperature of the boiler I gas cannot be maintained at its lowest value despite the preheating of the air. In addition, this form of waste heat feedback has its disadvantages because the incoming water is preheated to the maximum temperature of the waste heat. It is also possible to optimize the variables of the cycle process of the power machine with the help of a modern host computer. For example, in the case of a power plant, on-site water vapor and intermediate superheating conditions, the number of preheaters, the efficiency and the release pressure, the size of the condenser and Design, cooling tower design, etc. Having said that, even with these measures, the increase in efficiency is only to a limited extent. Finally, another method for improving the efficiency of a thermodynamic machine includes reducing the energy loss in the absorption and transmission of thermal energy by utilizing a temperature gradient ′ available between the endothermic and heating chains that is as complete as possible in the cyclic process chain. For this purpose, two or more power machines are connected in series, and the waste heat from the previous cycle process is used as heating heat for the subsequent cycle process. This method is used, for example, in modern combined power plants (gas and steam power plants), where the high heat of the combustion process is first used for gas turbines' and then its exhaust gas is used to heat steam power plants. In this way, the energy loss generated by water vapor is reduced, and the thermal gradient existing between the combustion temperature and the surrounding temperature is utilized in several stages. The method of tandem coupling cycle constitutes a patent application US The paper size is applicable to the Chinese National Standard (CNS) M specification (21〇X 297 mm) 5 (Please read the notes on the back first ^ Fill this page) Packing.-线- V. Description of the invention (3) Λ7 »7 The theme of the printing of 5,437,157 and US 4,428,190 by the Consumer Cooperatives of the Central Bureau of Standards of the Ministry of Economic Affairs each has two serial circulation processes, and AT 327,299 has three serial circulation processes. US 5,437,157 uses the condensing heat of a known steam power plant (working medium water) for gasifying an organic working medium, which produces useful work during the second water vapor cycle. The waste heat of the second cycle process is then discharged to the environment. A similar principle is used in US 4,428,190. The two water vapor cycle process (water and organic working medium) is coupled through an intermediate heat accumulator, which is intended to improve the load distribution of the daytime power plant. AT 327,299 describes the potassium and water vapor cycle process coupling using a third cycle process based on an organic working medium that transfers waste heat from the potassium process to the water process as heating heat. In the examples described, the cyclic processes are substantially separated from each other, and heat is transferred from one process to another through the heat exchanger wall. The disadvantage of series coupling in% process is that each cycle process requires additional heat transfer and energy conversion equipment. In addition, the loss of energy conversion energy increases with the number of cyclic processes coupled in series, because the use of heat exchangers to transfer heat can only maintain a limited temperature difference, and its disadvantage is that the waste heat of the last cyclic process in series must be discharged. To the Zhouyuan environment. Therefore, an object of the present invention is to provide a method in which the thermal efficiency of a heat engine can be improved without changing the upper and / or lower limits of the process temperature of the thermal cycle process. The present invention also has an object to provide a heat engine for performing such a method. These objects can be achieved by a method having the characteristics as described in the scope of the patent application and by a heat power machine having the characteristics as described in the scope of the patent application. Related subsidiary items reveal the advantages of the method and heat engine according to the invention

(請先閱讀背面之注意事@填寫本頁) 裝. 訂 線· 經濟部中央標準局員工消費合作社印製 Λ7 ~-___»7 太、發明説明(4 ) ~ ~ 異及較佳發展。 為了 了解本發明,重要地需了解熱動力機之熱效率非 與於其内部進行的循環過程之熱效率完全相等。 循環過程之熱效率係由各循環過程週期之輸送功及施 加熱施之比疋義。相反地,熱動力機之熱效率係由循環過 程之全部週期之輸送功對施加熱能之比定義。 當且唯有當循環過程廢熱離開動力機且輸送超出其系 統邊界至其環境時,兩種效率才相等。於習知熱動力機之 例,由循環過程提取之較低溫熱於個別週期完成時排放至 環境。如此,習知熱動力機效率最高等於其熱動.力循環過 程效率。 當動力機内部之全部或部分循環過程廢熱可施加作為 主能量(廢熱循環)時,熱動力機之效率大於其關聯循環過 程效率。此種情況下,循環過程之廢熱所含能量無需由新 主能量替代,或僅部分被替代,而動力機之累進效率隨著 所執行之循環過程週期數目而增高。 此種方法顯示於第1圖。第丨圖顯示其中假設循環過程 係以35%熱效率操作之熱動力機之效率進展。排放廢熱於 〇%,20%,40%,60% ’ 80%及100%(廢熱循環)之若干週 期返回此循環過程。不含廢熱反饋(〇%曲線),熱動力機效 率等於循環過程效率。利用廢熱反饋,熱動力機效率隨著 循環過程週期數之增加而增高,且漸進地趨近於理論最大 值。 第2圖顧示具極低效率僅5%之循環過程之相同方法。 本紙張尺度適用) A4規格(210χ297公楚) 7 --------^II (請先閱讀背面之注意事_填寫本頁) 訂 -線· 經 濟 標 準 貝 X 消 費 合 作 社 印 製 五、發明説明( Μ H? 即使此種不良過程效率,熱動力機效率可大為增高超過若 干週期數目。使用充分有效廢熱反饋,此種熱動力機可使 用低溫加熱經濟操作。 根據先前技術之習知熱動力機使用單一内循環過程。 其具有水蒸氣循環過程时丄作介f之相過渡(水蒸氣輪 機,水蒸氣動力機)或氣體循環過程而不含工作介質之相 過渡(氣體輪機,0tto引擎,柴油引擎,f飢引擎,斯德 鈴引擎,史丹佐引擎)。 於習知熱動力機之例,廢熱的反饋受廢熱溫度顯著比 供給循環絲之要求熱溫度更低的事實所限。因此理由故 ,僅小部分廢熱所含能量可返回循環過程。習知動力機, 升高廢熱溫度至過程溫度上限需要熱果,使廢熱能量可返 回循環過程。但此種熱㈣消耗部分由第—動力機產生的 軸功’結果對根據先前技術之習知熱動力機而言,廢埶反 饋之經濟程度有限。 現在本發明方法可透過内部廢熱反饋提高熱動力機之 累進熱效率,而無需使用習知熱泵方法之軸功。 習知動力機有單-水蒸氣循環過程或單一氣體循環過 程,或二者之串聯偶合(氣體/水蒸氣輪機,燃燒動力機, 氣體及水蒸氣發電廠卜本發明之熱動力機具有-水蒸氣 循環過程及-氣體循環過程於各熱動力機,亦即二循環過 程同時進行,而其實質上於氣相彼此” 水蒸氣循環過程用來產生軸功。水蒸氣循環過^由外 部熱源抽取加熱熱,水蒸氣循環過程之廢熱作為偶合氣體 (請先閲讀背面之注意事@填寫本頁) .裝.(Please read the note on the back @Fill this page first) Binding. Ordering · Printed by the Consumers' Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs Λ7 ~ -___ »7 Tai, Invention Description (4) ~ ~ Different and better development. In order to understand the present invention, it is important to understand that the thermal efficiency of a thermal power machine is not completely equal to the thermal efficiency of a cyclic process performed inside it. The thermal efficiency of the cyclic process is defined by the ratio of the transfer work and the application of heat during each cycle. In contrast, the thermal efficiency of a thermodynamic engine is defined by the ratio of the transfer work to the applied heat energy over the entire cycle of the cycle. The two efficiencies are equal if and only if the waste heat from the cycle leaves the engine and is transported beyond its system boundaries to its environment. In the case of the conventional thermal power engine, the lower temperature extracted from the cyclic process is discharged to the environment when the individual cycle is completed. In this way, the efficiency of the conventional thermodynamic engine is at the highest equivalent to the efficiency of its thermodynamic force cycle. When all or part of the waste heat in the cycle of the power engine can be applied as the main energy (waste heat cycle), the efficiency of the heat engine is greater than the efficiency of its associated cycle process. In this case, the energy contained in the waste heat of the cyclic process need not be replaced by the new main energy, or only part of it, and the progressive efficiency of the power machine increases with the number of cyclic process cycles performed. This method is shown in Figure 1. Figure 丨 shows the efficiency progress of a thermodynamic machine in which the cyclic process is assumed to operate at 35% thermal efficiency. The exhaust heat is returned to this cycle in several cycles of 0%, 20%, 40%, 60% ′ 80% and 100% (waste heat cycle). Without the waste heat feedback (0% curve), the thermodynamic efficiency is equal to the cycle process efficiency. Using waste heat feedback, the efficiency of the thermodynamic engine increases with the number of cycles in the cycle, and gradually approaches the theoretical maximum. Figure 2 shows the same method with a very low efficiency cycle of only 5%. Applicable to this paper size) A4 size (210 × 297 gongchu) 7 -------- ^ II (Please read the note on the back first_fill in this page) Order-line · Economic Standard X Printed by Consumer Cooperatives DESCRIPTION OF THE INVENTION (MH) Even with such poor process efficiency, the efficiency of the heat engine can be greatly increased over a number of cycles. With sufficient effective waste heat feedback, this heat engine can be economically operated using low temperature heating. According to the conventional heat engine Uses a single internal circulation process. It has a phase transition (water vapor turbine, water vapor power engine) or a phase transition without working medium (gas turbine, 0tto engine, diesel engine) during the water vapor cycle. , F star engine, Stering engine, Stanza engine). In the case of conventional thermal power engines, the feedback of waste heat is limited by the fact that the temperature of waste heat is significantly lower than the required heat temperature for the supply of circulating wire. Therefore, Only a small part of the energy contained in the waste heat can be returned to the cyclic process. Knowing the power engine, raising the waste heat temperature to the upper limit of the process temperature requires hot fruit, so that the waste heat energy can be returned. Back to the cycle process. However, the result of the shaft work generated by the first power engine is part of the heat consumption. The economical degree of waste feedback is limited to the conventional thermal power machine according to the prior art. The method of the present invention can now pass internal waste heat feedback. Improve the progressive heat efficiency of the thermodynamic engine without using the shaft work of the conventional heat pump method. The conventional power engine has a single-water vapor cycle process or a single gas cycle process, or a series coupling of the two (gas / water vapor turbine, combustion power engine, Gas and Water Vapor Power Plants The thermal power machine of the present invention has a -water vapor cycle process and -a gas cycle process in each heat power engine, that is, the two cycle processes are performed simultaneously, and they are essentially in the gas phase with each other. The shaft work is generated. The water vapor is circulated ^ The heating heat is extracted by an external heat source, and the waste heat of the water vapor circulation process is used as the coupling gas (please read the precaution on the back first @ fill this page).

.IT 本紙張尺度適用中國國家標準(CNS ) Α4規格(21〇χ^^.IT This paper size applies Chinese National Standard (CNS) Α4 specification (21〇χ ^^

I Λ7 B7 五、發明説明(6 經濟部中央標準局員工消費合作社印製 循環過程之加熱熱。水蒸氣循環過程之工作介質A為物質 或物質混合物,其成分具有顯著較高之分子偶極矩,故工 作介質AB之成分B係於氣體循環過程,此種成分大致永久 於氣態。水蒸氣循環過程中,工作介質A大半如同習知水 蒸氣動力機或水蒸氣輪機介於液體與氣體間進行週期性相 改變。 氣體循環過程用於本發明之熱動力機内部之廢氣反饋 。供此項目的之用,膨脹工作介質八所含之水蒸氣循環過 程之廢熱實質供給氣體循環過程作為產生軸功之加熱熱。 氣體循環過程也將部分水蒸氣循環過程之廢熱轉成軸功。 其工作介質AB(=氣體循環過程之工作介質)為水蒸氣循環 過程之工作介質A氣體部分與氣體循環過程之工作介質之 連續氣體成分B之混合。成分B為物質或物質混合物,而 其組成分具有顯著比來自水蒸氣循環過程之工作介質八之 物質組成分顯著更低的分子偶極矩。於氣體循環過程, 作介質AB以來自水蒸氣猶環過程之工作介質a之氣體一 規則調節,其再度於液體形式提取。結果AB内部之八之 百分量成分定期於氣體循環過程之封閉週期改變。 於氣相兩種過程實質交織用於二循環過程之物質或物 質混合物A與A B間熱能的直接交換及工作介質A之冷凝。 熱月b交換係藉彈性物質探勘兩種工作介質之物質氣體分子 間之布勞恩分子運動進行(碰撞頻率每秒約1〇1〇)。於顯微 層面分子動能(專於溫度)根據麥斯威爾理論進行統計機率 分布。供說明之用,需注意氣體或液體原子或分子移動而 工 量 (請先閱讀背面之注意事1£;填寫本頁) 裝· -線· -9 Λ7 B7 經濟部中央標準局員工消費合作社印製 五、發明説明(7 ) 無暫停且連續彼此碰撞。由於碰撞過程,其連續改變運動 方向、能量’結果也改變速度。如此,氣體或液體之全部 原子或分子速度不相等,但遵循麥斯威爾速度分布。於分 子層面,溫度及動能透過波茲曼常數彼此偶合,因此粒子 之平均動能(與旋轉能及擺動能無關)為E=3kT/2。結果於 氣相’不僅某個溫度而且溫度範圍相當於分子速度之統計 分布。於氣相得自物質A組及B組分子之渾沌態運動產生 分子間以不同速度及偶極矩彼此彈性碰撞。具有高分子偶 極矩之工作介質A物質組之慢(=冷)分子間碰撞,由於分子 間力影響,結果導致碰撞伴侣凝結,因而導致較大分子晶 格’及最終形成小滴。物質組A與B之分子晶格及快單一 分子間之碰撞導致動能(=熱)由較重小滴淨傳遞至較輕碰 撞伴倍。結果,氣體循環過程之氣相AB被分成快(=熱)及 慢(=冷)量化成分》 於顯微鏡下檢視,工作介質A之相過渡係透過本發明 之熱動力機氣體循環過程來自物質混合物AB自動形成之 霧執行。然後霧滴利用來自氣體循環過程氣相之守恆力場 (例如重力場或離心力場)透過相分離由氣體循環過程之氣 相去除,而透過進水泵送返水蒸氣循環過程。藉此方式, 工作介質A之水蒸氣於氣相供給氣體循環過程,並再度於 液相提取。供給氣體循環過程之熱為供給之氣態量化成分 A之潛熱,相當於冷凝熱。熱由水蒸氣循環過程移轉至氣 體循環過程可藉氣體循環過程之工作介質A之冷凝進行。' 氣體循環過程之廢熱為以工作介質A之液相提取熱。供熱 -------裝--:--:---訂-------線 (請先閱讀背面之注意事@填寫本頁) Γ, 10 - Λ7 η 7 五、發明説明(8 ) 與提取熱間之差為介於水蒸氣猶環過程與氣體 交換的工作介質A量之物質流之A凝埶甘 程間 ㈣程所誠生之最大軸功。結果,輯本發明之熱^ 機之水減循環過程之冷凝熱可於氣體循環過程全、 軸功(減少輻射熱)。根據本發明之熱動力機不再有進一成 廢熱(輻射熱除外)。藉此方式與習知熱動力機比較,根^ 本發明之熱動力機之效率隨著㈣過程·數目的增高而 增加,即使水蒸氣循環過程之效率不佳亦如此。結^间根 據本發明之熱動力機也適合作為利用低溫熱之能量守恆器I Λ7 B7 V. Description of the invention (6 The heating heat of the printing process of the consumer cooperative of the Central Standard Bureau of the Ministry of Economic Affairs. The working medium A of the water vapor circulation process is a substance or a mixture of substances, the composition of which has a significantly higher molecular dipole moment Therefore, the component B of the working medium AB is in the gas circulation process, and this component is almost permanent in the gaseous state. During the water vapor cycle, the working medium A is mostly like the conventional water vapor power machine or water vapor turbine. Phase change. The gas circulation process is used for the exhaust gas feedback inside the thermal power machine of the present invention. For the purpose of this project, the waste heat of the water vapor circulation process contained in the expanded working medium eight is actually supplied to the gas circulation process as the heating for generating shaft work. Heat. The gas circulation process also converts part of the waste heat of the water vapor circulation process into shaft work. Its working medium AB (= working medium of the gas circulation process) is the working medium A of the water vapor circulation process and the working medium of the gas circulation process. Of continuous gas component B. Component B is a substance or a mixture of substances, and its composition is divided There is a significantly lower molecular dipole moment than the material composition of the working medium eight from the water vapor cycle process. In the gas circulation process, the working medium AB is regularly adjusted with the gas from the working medium a from the water vapor cycle process. It is extracted again in liquid form. As a result, eighty percent of the components inside AB are periodically changed during the closed cycle of the gas circulation process. The two processes in the gas phase are essentially intertwined for the thermal energy of the substance or substance mixture A and AB in the second cycle process. Direct exchange and condensation of the working medium A. The hot month b exchange is carried out by using elastic materials to explore the movement of Braun molecules between the gas molecules of the two working mediums (the collision frequency is about 1010 per second). At the microscopic level Molecular kinetic energy (specialized in temperature) is used to calculate the statistical probability distribution according to Maxwell's theory. For illustration, pay attention to the amount of gas or liquid atoms or molecules moving and the amount of work (please read the note on the back 1 £; fill out this page)装 ·-线 · -9 Λ7 B7 Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 5. Description of the invention (7) No suspension and continuous collision with each other. Due to the collision It continuously changes the direction of movement, and the energy also changes the speed. In this way, the speed of all atoms or molecules of a gas or liquid is not equal, but it follows the Maxwell velocity distribution. At the molecular level, temperature and kinetic energy pass through the Bozman constant They are coupled to each other, so the average kinetic energy of the particles (irrespective of rotational energy and swing energy) is E = 3kT / 2. As a result, in the gas phase, not only a certain temperature, but also a temperature range equivalent to the statistical distribution of molecular velocities. The chaotic motion of molecules in groups A and B results in elastic collisions between molecules at different speeds and dipole moments. The slow (= cold) intermolecular collisions in the working medium A with a high molecular dipole moment due to intermolecular forces The result is that the collision partner coagulates, which leads to the formation of larger molecular lattices and eventually droplets. The molecular lattices of substance groups A and B and the collision between fast single molecules cause kinetic energy (= heat) to be eliminated by the heavier droplets. Pass to lighter collision partner times. As a result, the gas phase AB of the gas circulation process is divided into fast (= hot) and slow (= cold) quantified components. "Viewed under a microscope, the phase transition of the working medium A is derived from the substance mixture AB through the gas cycle process of the thermodynamic engine of the present invention. Automatically formed fog is performed. The droplet is then removed from the gas phase of the gas cycle through phase separation using a conserved force field (such as a gravitational field or a centrifugal force field) from the gas phase of the gas cycle process, and is returned to the water vapor cycle process through the inlet pump. In this way, the water vapor of the working medium A is supplied to the gas circulation process in the gas phase, and extracted again in the liquid phase. The heat of the supply gas circulation process is the latent heat of the supplied gaseous quantified component A, which is equivalent to the heat of condensation. The transfer of heat from the water vapor cycle to the gas cycle can be performed by the condensation of the working medium A in the gas cycle. '' The waste heat of the gas circulation process is the heat of liquid phase extraction of the working medium A. Heating -------- install-:-: --- order ------ (please read the note on the back @fill this page first) Γ, 10-Λ7 η 7 V. Description of the invention (8) The difference between the heat extraction and the heat extraction is the maximum shaft work that is produced by the A-condensation process between the process of the water vapor and the gas exchange of the working medium A. As a result, the condensing heat of the water reduction cycle of the heat generator of the present invention can be used for the full and shaft work of the gas cycle (reducing radiant heat). The thermal power machine according to the present invention no longer has 10% waste heat (except radiant heat). Compared with the conventional thermal power machine in this way, the efficiency of the thermal power machine of the present invention increases with the increase in the number and the number of processes, even if the efficiency of the water vapor cycle is not good. According to the invention, the thermodynamic machine according to the present invention is also suitable as an energy conservator using low-temperature heat.

下列物質組合例如為根據本發明 組合: 之熱動力機操作之可 水蒸氣週期ΜΛ 氣體週期m) 氣化溫廣商 水 空氣 70... 300°C -氧化碳 空氣,氮 -70... 20°C 氨 空氣,氮 -40 …70〇C 冰凍混合物 空氣,氮 -50... 0°C 氮 氫 -200... -150°C 氮 惰性氣體 -200…-150°C 經濟部中央標準局員工消費合作社印製 本發明方法及執行此種方法之本發明之熱動力機於後 文將參照附圖進行說明,附圖中: 第1圖顯示初效率為35 %之熱動力機累進20週期之效 率; 第2圖顯示初效率為5%之熱動力機累進200週期之效 率; 第3圖顯示根據本發明偶合氣體循環過程之水蒸氣循 11 本紙張尺度適用中國國家標準(CNS ) Α4規格(210X297公釐) Λ7 B7 經濟部中央標準局貝工消资合作社印製 五、發明説明(9The following combinations of substances are, for example, combinations according to the present invention: The water vapor cycle MΛ gas period m) of the operation of a thermodynamic engine The gasification temperature Guangshang water air 70 ... 300 ° C-carbon oxide air, nitrogen-70 ... 20 ° C ammonia air, nitrogen -40… 70 ° C frozen mixture air, nitrogen-50 ... 0 ° C nitrogen hydrogen -200 ... -150 ° C nitrogen inert gas -200 ...- 150 ° C central standard of the Ministry of Economy The employee's consumer cooperative of the Bureau printed the method of the present invention and the heat engine of the present invention which executes this method will be described later with reference to the accompanying drawings. In the drawing: Figure 1 shows that the heat engine with an initial efficiency of 35% progresses for 20 cycles. Efficiency; Figure 2 shows the 200-cycle efficiency of a thermodynamic machine with an initial efficiency of 5%; Figure 3 shows the water vapor cycle of the coupled gas cycle process according to the present invention. 11 This paper size applies Chinese National Standard (CNS) A4 specification (210X297 (Mm) Λ7 B7 Printed by the Shellfish Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs

環過程之PV圖J 第4圖顯示根據本發明之熱動力機之二循環過程間之 能量流代表圖; 第5圖顯示兩種工作介質a及AB之麥冑咸爾 冷凝之代表圖; 第6圖顯示根據本發明之熱動力機之個別功能組件之 細節代表圖;及 ' 第7圖顯示根據本發明之密實熱動力機之功能組件之 代表圖。 第1圖顯示假設熱動力機透過20週期之效率之不同進 展。熱動力機之循環過程具有理論效率35%。熱動力機具 相等效率但無廢熱饋送返回循環過程(〇%級數卜若由循環 過程放出之某一部分廢熱返回熱動力機,則熱動力機之效 率緩慢增高。例如80%廢熱反饋,則經2〇週期後熱動力機 可達約70%效率。 第2圖說明效率僅5%之循環過程之相同情況。如第2 圖所示,熱動力機效率提高至约2〇%,廢熱反饋為8〇%。 如此,利用廢熱反饋,熱動力機效率比循環過程效率增高 約4倍。 第3圖顯示實質偶合水蒸氣循環過程(左PV圖)與氣體 循環過程(右PV圖)之示意代表圖。此處說明之水蒸氣循環 過程為不含多次中間超熱之單一過程。該方法也應用至全 部其它水蒸氣循環過程。水蒸氣循環過程包括六個指示點 D1至D6。氣體循環過程包括四個指示點⑴至G4。各步驟 l·!-------裝--^--:---訂------丨線 (請先聞讀背面之注意事1®填寫本頁)The PV diagram of the ring process J. Fig. 4 shows a representative diagram of the energy flow between the two cycle processes of the thermodynamic machine according to the present invention. Fig. 5 shows a representative diagram of the melamine condensation of the two working media a and AB; The figure shows a detailed representative diagram of the individual functional components of the heat power machine according to the present invention; and FIG. 7 shows a representative diagram of the functional components of the compact heat power machine according to the present invention. Figure 1 shows a hypothetical thermodynamic engine that progresses through 20 cycles of efficiency. The thermal power cycle process has a theoretical efficiency of 35%. The thermal power equipment has the same efficiency but no waste heat is fed back to the circulation process (0% series. If a part of the waste heat released by the circulation process is returned to the thermal power machine, the efficiency of the thermal power machine will slowly increase. For example, 80% waste heat feedback, after 20 cycles The rear heat engine can reach an efficiency of about 70%. Figure 2 illustrates the same situation of a cycle process with an efficiency of only 5%. As shown in Figure 2, the efficiency of the heat engine is increased to about 20%, and the waste heat feedback is 80%. Using waste heat feedback, the efficiency of the thermodynamic engine is about 4 times higher than the efficiency of the cycle process. Figure 3 shows a schematic representation of the substantially coupled water vapor cycle process (left PV picture) and gas cycle process (right PV picture). The water vapor cycle process is a single process without multiple intermediate superheats. This method is also applied to all other water vapor cycle processes. The water vapor cycle process includes six indicator points D1 to D6. The gas cycle process includes four indicator points⑴ Go to G4. Each step l ·! ------- install-^-: --- order ------ 丨 line (please read the note 1 on the back first and fill in this page)

12 Λ7 B7 經濟部中央標準局員工消費合作社印製 五、發明説明(10 ) 詳述如後: D1-D2水蒸氣循環過程之液體透過泵由低壓輸送至 高壓,並於高壓供給氣化器。 D2-D3工作介質A於氣化器於高壓藉施熱(Qt。)氣化, 並由液相轉成氣相。 D3-D4水蒸氣被超熱,此種超熱並非必要。於動力 機設計成利用低溫熱之例可刪除超熱。 D4-D5水蒸氣以軸功輸出膨脹至其壓力相當於氣體 循環過程之混合物壓力為止。(註:該點顯示於熱水蒸氣 區,但也位於濕水蒸氣區)。 D5-D6習知水蒸氣循環過程中,此區段為水蒸氣完 全膨脹至濕水蒸氣區。但根據本發明之動力機,此種過程 發生於氣體循環過程。 D6-D1習知水蒸氣循環過程中,此段為水蒸氣循環 過程工作介質A由氣相轉成液相,由於熱被提取而被迫冷 凝。影線區Qfr()m相當於水蒸氣循環過程之廢熱。.於本發 明之方法之例,此過程也發生於氣體循環過程。 D5-G2水蒸氣循環過程之完全或部分脹大的氣態工 作介質A轉移入氣體循環過程,氣態工作介質a混合至氣 體循環過程之壓縮氣態工作介質A B。由於工作介質A混 合入氣體混合物AB,故氣體混合物AB之相對濕度比成分 A升高。 氣體循環過程將由第一階段開始解說如下: G1-G2氣體循環過程工作介質AB之絕熱壓縮。結果 (諳先閱讀背面之注意事@填寫本頁) -裝. 訂 « -線. 枣紙悵尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 13 鯉濟部中央標準局員工消費合作社印製 Λ7 ___R7 五、發明説明(11 ) 導致介質AB之壓力及溫度升高,及相對濕度比物質成分 A減少。於點G2,如對過渡£)5_(}2所述,混合來自水蒸氣 循環過程之介質A物質量。 G2-G3實際混合過程:此處存在於氣體循環過程之 氣體混合物AB之量,因而AB之容積由來自水蒸氣循環過 程之工作介質A之物質量增高,混合物ab之相對濕度比 物質成分A增高。混合過程係以恆壓說明,但非必要。如 此表示混合過程也可以改變壓力進行。混合係藉軸功輸出 執行。 G3-G4氣體混合物以軸功輸出絕熱脹大。此處工作 介質AB之壓力及溫度降低,氣體混合物AB之相對濕度超 過其物質成分A之飽和限度。具較高偶極矩之物質a分子 凝結形成小滴,其動能輸出點氣相剩餘粒子AB。形成霧 伴隨殘餘氣體量AB之壓力及容積下降〇氣相ab之相對濕 度相對於物質A增至1 〇〇%。冷凝為霧之物質a之冷凝潛熱 量保留於殘留氣體量AB。 G4-G1透過提取液體使容積減少:霧於守恆力場(較 佳為離心力場)透過相分離而由工作介質AB之殘氣量去除 ,並呈液體送返水蒸氣循環過程。點G4至G1實際位置極 為接近’故氣體循環過程於PV圖之輪廓接近三角形。 G4-D1此步驟就液體工作介質a敘述由氣體循環過程 至水蒸氣循環過程之物質交換。如此,由氣體循環過程提 取之具高分子偶極矩之物質A之液體量重新供給水蒸氣循 環過程》 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) (請先閱讀背面之注意事填寫本頁) 裝. 線 14 經濟部中央標準局員工消費合作社印製 Λ7 _________B7五、發明説明(12 ) . 由線D-1-2-3-4-5-6-1包圍區相當於水蒸氣循環過程可 產生之最大功。線G-1-2-3-4-1包圍區對應於氣體循環過程 可產生之最大功。水蒸氣循環過程之廢熱連同水蒸氣循環 過程工作介質A之廢氣由點D5送至點G2作為氣體循環過 程之輸入熱;而氣體循環過程之廢熱連同冷凝液體由點G4 送至點D1作為水蒸氣循環過程之輸入熱。兩種循環過程 皆產生來自供給熱之功友廢熱。兩種循環過程組合於單一 熱動力機’結果導致熱動力機未排放任何廢熱進入周圍環 境。 第4圖顯示於根據本發明之熱動力機,介於水蒸氣循 環過程與氣體循環過程間之能量流。動力機有二循環過程 ’各自由供給熱產生軸功(WD及WG)及之廢熱(QD及qg)。 如第4圖所示,熱QexternMQG供給水蒸氣循環過程,熱qd 供給氣體循環過程。由於事實上兩種循環過程可往復再度 使用其個別之廢熱流作為供熱,故動力機可將外部供熱流 Qextern完全轉成軸功wextern(但輻射熱除外)。 可能原因為經由利用於顯微層面於分子間作用的實際 氣體之偶極矩,可透過霧化冷凝以及導致守恆力場分離執 行快(=熱)及慢(=冷)粒子分離。 氣相分子間之能量移轉係藉彈性碰撞執行,而未受任 何方向限制所限。於分子層面,當彈性碰撞時動能(=熱) 可由重且慢(=冷)碰撞伴侣淨移轉給輕且快(=熱)碰撞伴侣 。由於根據麥斯威爾定律分子速度接受統計分布,故經常 有碰撞伴侣其比較巨觀測量溫度顯著更快或更慢。如此具 (請先聞讀背面之注意事!^填寫本頁) 裝· "·* -線_ 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公釐) 五、發明説明(l3 ) Λ7 H7 經濟部中央標準局員工消費合作社印製 有大及小偶極矩分子之氣體混合,於溫度降低時必然導致 高偶極矩分子凝結,其隨後作為與較小偶極矩分子之彈性 碰撞中的較重碰撞伴侣,損失較大動能(=熱卜溫度下降 係由於絕熱膨脹強迫進行(參考階段G3-G4),故具有大偶 極矩的慢分子必須保持彼此黏著,且釋放其動能給具有低 偶極矩之分子。事實上,由於氣相冷凝熱之移轉並未發生 於不同溫度實體間,反而利用於麥斯威爾速度分布範圍内 粒子間之彈性碰撞,而於分子層面發生移轉,故遵守熱力 學第二基本定律。 此種過程闡明於第5圖。第5圖左圖顯示兩種工作介質 A及B之氣態混合物之麥斯威爾速度分布,此處於各 例規定具有某種速度u之分子數目。冷卻時,霧之冷凝係 透過絕熱冷凝進行。工作介質八與8之混合物含工作介質 A濃度降低,持續保留氣態(第5圖之右上圖)。相反地,工 作介質A形成小滴,例如可藉助於離心機由氣相去徐(第5 圖之右下圖)。 物質交換僅發生於引擎内部之兩種循環過程而非與環 境物質交換。動力機可構造為密閉系統,系統邊界僅傳送 熱能及軸功。由於動力機無需輸送廢熱返回環境,故可利 用低溫熱能作為熱源。如此要求水蒸氣循環過程具有相過 渡溫度低於低溫熱源溫度。否則低溫熱無法用於氣化水蒸 氣循環工作介質。由於輻射損失小,故若熱能係於低溫供 給,則動力機之效率藉施加低溫熱甚至比施加高溫熱更佳 (請先閲讀背面之注意事^填离本頁) •裝· 訂 Φ 線.12 Λ7 B7 Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs 5. Description of the Invention (10) The details are as follows: The liquid in the D1-D2 water vapor circulation process is transported from the low pressure to the high pressure through the pump and supplied to the gasifier at high pressure. D2-D3 working medium A is gasified in the gasifier by applying heat (Qt.) At a high pressure, and is converted from a liquid phase to a gas phase. D3-D4 water vapor is superheated. Such superheating is not necessary. In the case where the engine is designed to use low temperature heat, superheat can be removed. D4-D5 water vapor expands with shaft work output until its pressure is equal to the pressure of the mixture during gas circulation. (Note: This point is shown in the hot water vapor zone, but also in the wet water vapor zone). D5-D6 It is known that during the water vapor cycle, this section is the area where the water vapor completely expands to the wet water vapor. However, according to the power machine of the present invention, such a process occurs in a gas circulation process. D6-D1 In the conventional water vapor cycle process, this section is the water vapor cycle. The working medium A changes from the gas phase to the liquid phase and is forced to condense because heat is extracted. The hatched area Qfr () m corresponds to the waste heat of the water vapor cycle. In the case of the method of the present invention, this process also occurs in the gas circulation process. D5-G2 The fully or partially swollen gaseous working medium A is transferred into the gas cycle, and the gaseous working medium a is mixed to the compressed gaseous working medium A B of the gas cycle. Since the working medium A is mixed with the gas mixture AB, the relative humidity of the gas mixture AB is higher than that of the component A. The gas circulation process will be explained from the first stage as follows: G1-G2 gas circulation process adiabatic compression of working medium AB. Results (Please read the note on the back @ Fill this page first) -Packing. Ordering «-Line. The date paper jujube scale is applicable to the Chinese National Standard (CNS) A4 specification (210X297 mm) 13 Employee Consumer Cooperative of the Central Standards Bureau of Liji Print Λ7 ___R7 V. Description of the invention (11) Causes the pressure and temperature of the medium AB to increase, and the relative humidity to be reduced compared to the substance component A. At point G2, as described in the transition £) 5 _ (} 2, mix the mass of medium A from the water vapor cycle process. G2-G3 Actual mixing process: The amount of gas mixture AB present in the gas cycle process here, so The volume of AB is increased by the mass of the working medium A from the water vapor cycle process, and the relative humidity of the mixture ab is higher than that of the material component A. The mixing process is described with constant pressure, but it is not necessary. This means that the mixing process can also be carried out by changing the pressure. .Mixing is performed by shaft work output. G3-G4 gas mixture is adiabaticly expanded by shaft work output. Here the pressure and temperature of the working medium AB are reduced, and the relative humidity of the gas mixture AB exceeds the saturation limit of its material component A. The molecules of substance a with a high dipole moment condense to form droplets, and the kinetic energy output point of the remaining particles in the gas phase AB. The formation of mist is accompanied by a decrease in the pressure and volume of the residual gas amount AB. The relative humidity of the gas phase ab is increased to 1 relative to the substance A. 〇%. The condensing latent heat of the substance a condensed into the mist is retained in the residual gas amount AB. G4-G1 reduces the volume by extracting the liquid: the mist is in a conserved force field (preferably centrifugal force) ) The residual gas content of the working medium AB is removed through phase separation, and the liquid is returned to the water vapor cycle process. The actual position of points G4 to G1 is very close to 'therefore, the outline of the gas cycle process in the PV diagram is close to a triangle. G4-D1 this step Regarding the liquid working medium a, the material exchange from the gas circulation process to the water vapor circulation process is described. In this way, the liquid amount of the substance A with a high molecular dipole moment extracted from the gas circulation process is supplied to the water vapor circulation process again. China National Standard (CNS) A4 specification (210X297 mm) (Please read the notes on the back first and fill in this page) Packing. Line 14 Printed by the Consumers Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs Λ7 _________ B7 V. Invention Description (12) The enclosed area of line D-1-2-3-4-5-6-1 is equivalent to the maximum work that can be generated by the water vapor cycle. The enclosed area of line G-1-2-3-4-1 corresponds to the The maximum work produced. Waste heat from the water vapor cycle together with waste gas from working medium A in the water vapor cycle is sent from point D5 to point G2 as the input heat of the gas cycle process; and waste heat of the gas cycle process with condensate It is sent from point G4 to point D1 as the input heat of the water vapor cycle process. Both cycle processes generate waste heat from the workers who supply heat. The combination of the two cycle processes in a single heat engine 'results in the heat engine not emitting any waste heat into the surroundings The environment. Figure 4 shows the energy flow between a steam cycle and a gas cycle in a thermal power machine according to the present invention. The power machine has a two-cycle process, each of which generates shaft work (WD and WG) and waste heat from the supplied heat. (QD and qg). As shown in Figure 4, the heat QexternMQG supplies the water vapor cycle process, and the heat qd supplies the gas cycle process. Due to the fact that the two cycle processes can re-use their individual waste heat streams as heat again, the power machine The external heat flow Qextern can be completely converted into shaft work wextern (except for radiant heat). The possible reason is that fast (= hot) and slow (= cold) particle separation can be performed through the atomic condensation and the conservation of the force field separation through the dipole moment of the actual gas that is used for intermolecular interaction at the microscopic level. Energy transfer between molecules in the gas phase is performed by elastic collisions and is not limited by any directional restrictions. At the molecular level, the kinetic energy (= heat) can be transferred from a heavy and slow (= cold) collision partner to a light and fast (= hot) collision partner during an elastic collision. Because molecular velocity is accepted as a statistical distribution according to Maxwell's law, there are often collision partners that measure temperatures significantly faster or slower than the macroscopic view. It ’s so (please read the notes on the back! ^ Fill in this page) Packing " · * -line_ This paper size is applicable to China National Standard (CNS) A4 specification (210X297mm) V. Description of invention (l3) Λ7 H7 Gas mixtures printed with large and small dipole moment molecules by the Consumer Cooperative of the Central Standards Bureau of the Ministry of Economic Affairs will inevitably cause high dipole moment molecules to condense when the temperature decreases, which then acts as an elastic collision with smaller dipole moment molecules The heavy collision partner in the medium loses a large amount of kinetic energy (= the temperature drop is forced due to adiabatic expansion (reference stage G3-G4), so slow molecules with large dipole moments must keep sticking to each other and release their kinetic energy to Molecules with a low dipole moment. In fact, the transfer of the condensation heat of the gas phase does not occur between entities at different temperatures, but is instead used for elastic collisions between particles in the Maxwell velocity distribution, and occurs at the molecular level. Transfer, so the second basic law of thermodynamics is observed. This process is illustrated in Figure 5. The left side of Figure 5 shows the Maxwell velocity distribution of a gaseous mixture of two working media A and B. Here Each example specifies the number of molecules with a certain speed u. When cooling, the condensation of the mist is carried out through adiabatic condensation. The mixture of working mediums 8 and 8 contains a decrease in the concentration of working medium A, which continues to retain the gaseous state (Figure 5, upper right). Conversely, the working medium A forms droplets, which can be removed from the gas phase by means of a centrifuge, for example (bottom right of Figure 5). Material exchange occurs only in the two internal circulation processes of the engine and not with the environmental material. Power machines Can be constructed as a closed system, the system boundary only transfers thermal energy and shaft work. Since the power machine does not need to transport waste heat back to the environment, it can use low-temperature thermal energy as a heat source. This requires that the water vapor cycle process have a phase transition temperature lower than the low-temperature heat source temperature. Otherwise, it is low temperature Heat cannot be used as the working medium for the vaporized water vapor cycle. Because the radiation loss is small, if the thermal energy is supplied at a low temperature, the efficiency of the power machine is even better than the application of low temperature heat (please read the precautions on the back first) ^ Fill this page) • Binding and binding Φ line.

經濟部中央標準局員工消費合作社印製 Λ7 二7^ ----H? 五、發明説明(14 ) ;… —------- 本發明之熱動力機可設計為活塞引擎(馬達)或流引擎 (輪機)由於離心力場用於霧之分離為較佳,故偏好使用 i 占 51 3Sc 原因為此種離心力場容易於輪機之旋轉部件產生 0 適η執行本發明方法之兩種流引擎將參照第6及7圖說 明。 第6圖顯示適合用於超熱水蒸氣循環過程之系統,第7 圖顯示緊密系統,其作為最小構造僅含絕對需要的系統元 件。 —圖僅含各引擎之功能組件而不含其構造設計,及各 組件間之物質流動表示。 如第6圖所示,根據本發明之熱動力機至少包括下列 力育b 且件.系,氣化器,水蒸氣輪機,混合腔室,氣體輪 機,冷凝器,離心機及壓縮機。水蒸氣循環過程含有下列 組件.泵,氣化器,水蒸氣輪機及冷凝器。氣體循環過程 包括下列組件:氣體輪機及壓縮機。二循環過程間之物質 乂換係利用混合腔室及離心機執行。軸功消耗者為壓縮機 、泵及離心機,其係由氣體輪機及/或水蒸氣輪機驅動。 同時’水蒸氣輪機及/或氣體輪機輸出軸功給外部消耗者 〇 軋化器透過泵供給液體工作介質A,其係透過加熱而 於高溫氣化,及於水蒸氣輪機連同軸功之輸出膨脹。水蒸 氣輪機之廢氣於混合腔室混合壓縮機壓縮的氣體循環過程 之工作氣體AB,且由氣體輪機藉軸功輸出膨脹。離開氣 本紙張尺度適用中國國家標準(CNS ) A4規格(210X297公ffY ---— l·—IIΊ—I—IIHI n 批衣 ~~ —7 11 訂^— I ~"線 (諸先閲讀背面之注意事@填寫本頁} ί Λ7 _______R7 -一一-------- 五、發明説明(15 ) . 體輪機後,冷凝器内產生霧。霧於離心機由氣體循環過程 之氣相去除,並透過泵再度呈液體供給水蒸氣循環過程。 第7圖包含功能組件水蒸氣輪機及氣體輪機,連同輪 機組件之混合腔室及冷凝離心機組件之功能組件冷凝器及 離心機。此處,二循環過程之氣體流共同被帶入輪機,其 廢氣於冷凝離心機分成二相。泵及壓縮機輸送各流體返回 電路。此種單元可具有極為緊密的構造。 根據本發明之熱動力機可用於高溫範圍及低溫範圍, 但水蒸氣循環過程之相過渡溫度係低於熱源溫度。由於熱 動力機無需與系統環境作任何物質交換,故全然為環境中 性。於低溫範圍,可使用由於缺乏熱穩定性無法用於高溫 範圍的物質。 結果’根據先前技術無法用於習知動力機之用途藉由 使用不與環境產生任何物質交換之低溫熱動力機變成可行 18 本紙張尺度適用中國國家標準(CNS ) Μ規格(2ΐ〇χ297公釐)Printed by the Consumer Cooperatives of the Central Standards Bureau of the Ministry of Economic Affairs Λ7 2 7 ^ ---- H? V. Description of the invention (14); ... ------ --- The heat engine of the present invention can be designed as a piston engine (motor) Or the flow engine (turbine), because the centrifugal force field is better for the separation of the fog, i prefer to use 51. 3Sc because this kind of centrifugal force field is easy to generate for the rotating parts of the turbine. Description will be made with reference to FIGS. 6 and 7. Figure 6 shows a system suitable for use in the super hot water vapor cycle process, and Figure 7 shows a compact system that contains only the system components that are absolutely required as a minimum construction. —The figure includes only the functional components of each engine, not its structural design, and the representation of the material flow between the components. As shown in Fig. 6, the thermal power machine according to the present invention includes at least the following components: a gasifier, a steam turbine, a mixing chamber, a gas turbine, a condenser, a centrifuge, and a compressor. The water vapor cycle contains the following components: pump, gasifier, water turbine and condenser. The gas circulation process includes the following components: a gas turbine and a compressor. The material exchange between the two cycles is performed using a mixing chamber and a centrifuge. The consumers of shaft work are compressors, pumps and centrifuges, which are driven by gas turbines and / or steam turbines. At the same time, the steam turbine and / or gas turbine output shaft work to an external consumer. The rolling mill supplies liquid working medium A through a pump, which is gasified at high temperature by heating, and expands in the output of the steam turbine with shaft work. . The exhaust gas of the steam turbine is mixed with the working gas AB in the gas circulation process compressed by the mixing compressor in the mixing chamber, and the gas turbine expands by the shaft work output. The paper size of the paper is applicable to the Chinese National Standard (CNS) A4 specification (210X297 male ffy ----- l · —IIΊ—I—IIHI n batch clothing ~~ —7 11 order ^ — I ~ " line (read first Note on the back @ fill this page} ί Λ7 _______R7-one one -------- V. Description of the invention (15). After the turbine, the fog is generated in the condenser. The mist is in the centrifuge by the gas circulation process. The gas phase is removed, and the liquid is supplied to the water vapor cycle through the pump again. Figure 7 contains the functional components of the steam and gas turbines, together with the mixing chamber of the turbine components and the condensers and centrifuges of the condensing centrifuge components. Here, the gas flow of the two-cycle process is taken together into the turbine, and its exhaust gas is separated into two phases in the condensing centrifuge. The pump and compressor transport each fluid back to the circuit. Such a unit can have an extremely compact structure. The heat according to the invention The power engine can be used in high temperature range and low temperature range, but the phase transition temperature of the water vapor cycle is lower than the temperature of the heat source. Since the thermal power machine does not need to exchange any substance with the system environment, it is completely environmentally neutral. At low temperature The range can use substances that cannot be used in the high temperature range due to lack of thermal stability. As a result, it cannot be used for conventional power machines according to the prior art. It becomes feasible by using low temperature heat power machines that do not exchange any substance with the environment. 18 papers Standards are applicable to China National Standard (CNS) M specifications (2 × 〇χ297 mm)

Claims (1)

if “争月广 六、申請專利範園 第87118937號專利申請案申請專利範圍修正本 1 —鞴於且古妨 -修正日期·· 88年12月 ’程之二1 動力循環過程和至少-第二循環過 3=機中轉化熱能成機械能之方法,其中該第 ::過程之廢熱供給該第二循環過程,及該第二循 ^之廢熱供給該Ί環過程,特徵在於 氣一==為水蒸氣猶環過程,及該第二循環過程為 頁 帛且物質父換發生在該氣Μ環過程與 該水蒸氣循環過程之間。 2. 如申請專利範圍第1項之方法,其特徵為該第-及第二 循環過程係同時進行而未與環境作物質交換。 訂 3. 如申請專利範圍第以之方法,其特徵為於水蒸氣循環 牡使用工作介fA其含有具高分子偶極矩之物質或 物質混合物’及於氣體循環過程使用工作介質Μ,其 含有得自水蒸氣循環過程氣相介質A與第二成分b之混 合物’其含有具低分子偶極矩之物質或物質混合物。 4.如申請專利_第3項之方法,其特徵為由外部供給熱 動力機之熱能,較佳用於氣化液體水蒸氣過程工作介 質A 〇 5·,申請專利範圍第3或4項之方法,其特徵為水蒸氣循 裱過程工作介質A透過物質交換涉及兩種循環過程。 6· t申請專利範圍第3或4項之方法,其特徵為水蒸氣循 環過程工作介質A之氣相混合氣體循環過程工作介質 AB之氣相。 ’ -19- 本紙張適用中國國家標準(CNS )八4職(210X297公褒) if “争月广 六、申請專利範園 第87118937號專利申請案申請專利範圍修正本 1 —鞴於且古妨 -修正日期·· 88年12月 ’程之二1 動力循環過程和至少-第二循環過 3=機中轉化熱能成機械能之方法,其中該第 ::過程之廢熱供給該第二循環過程,及該第二循 ^之廢熱供給該Ί環過程,特徵在於 氣一==為水蒸氣猶環過程,及該第二循環過程為 頁 帛且物質父換發生在該氣Μ環過程與 該水蒸氣循環過程之間。 2. 如申請專利範圍第1項之方法,其特徵為該第-及第二 循環過程係同時進行而未與環境作物質交換。 訂 3. 如申請專利範圍第以之方法,其特徵為於水蒸氣循環 牡使用工作介fA其含有具高分子偶極矩之物質或 物質混合物’及於氣體循環過程使用工作介質Μ,其 含有得自水蒸氣循環過程氣相介質A與第二成分b之混 合物’其含有具低分子偶極矩之物質或物質混合物。 4.如申請專利_第3項之方法,其特徵為由外部供給熱 動力機之熱能,較佳用於氣化液體水蒸氣過程工作介 質A 〇 5·,申請專利範圍第3或4項之方法,其特徵為水蒸氣循 裱過程工作介質A透過物質交換涉及兩種循環過程。 6· t申請專利範圍第3或4項之方法,其特徵為水蒸氣循 環過程工作介質A之氣相混合氣體循環過程工作介質 AB之氣相。 ’ -19- 本紙張適用中國國家標準(CNS )八4職(210X297公褒) 、申請專利範圍 V如申請專利範圍第…項任—項之方法,其特徵為循 環液-氣·液相變化透過轴功之輸出發生於水蒸氣循環 過程。 8. 如申請專利範圍第3或4項之方法,其特徵為水蒸氣循 環過程之工作介質人相對於氣體循環過程工作介質Μ 之循環量或濃度變化藉軸功之輸出發生於氣體循 程。 9. 如申請專利範圍第3或4項之方法,其特徵為水篆 環過程工作介質入之冷凝主要發生於氣體循環過程工 作介質AB之膨脹期内部及期間。 H).如申請專利範圍第3或4項之方法,其特徵為水蒸 環過程工作介質A之相過渡產生的霧利用守怪力場, 較佳離心力場與氣體循環過程工作介質^分離,及再 度呈液體供給水蒸氣循環過程之工作介質A。 如申請專利範圍第3或4項之方法,其特徵為水蒸氣循 環過程工作介質A及氣體循環卫作介f ab之第二成分 B可存在於下列組合: n A=水及B=空氣; A=二氧化碳及b=空氣/氮; A=氨及B=空氣/氮; A_=冰束混合物及b =空氣/氮; A=氮及B=氫;或 A=氮及B =惰性氣體。 ^一種用來轉化熱能成機械能之熱動力機,其具有第— -20- 本紙張从適用中國國冢標準(CNS )从祕(210X29^^7 m —I— l 1__1 m i ·1*^11-1 ^^1 ml·— In. In. A -¾ 、1 f請先閲讀背面之注意事項再填寫本頁} [ 熱動力循環過程和至少一第二循環過程,該 W 儒環 過程之廢熱供給該第二循環過程,及該第二循環過程 之廢熱供給該第一循環過程,£特徵為,該 過程為水蒸氣循環過程,及該第二循環過程為氣體循 環過程,且物質交換發生在該氣體循環過程與該水蒸 氣循環過程之間。 Ά 13.如申請專利範圍第!2,/之熱動力機,其特徵為熱動力 機包含至少下列功能組件,果,氣化器,水蒸氣,輪 機’混合腔室,氣體輪機’冷凝器,離心機及壓縮機 M.如申請專利範圍第13項之熱動力機,其特徵為水蒸氣 循環過程之㈣工作介f A供給氣化器伴以壓力增高 ,於此處被供給熱能氣化,及於水蒸氣輪機 : 出膨脹。 ^ 15·如申請專利範圍第13或14項之熱動力機,其特徵為水 蒸氣輪機之廢氣於混合腔室混合氣體猶環過程之壓縮 工作介質ΑΒ,於氣體輪機以軸功之輸出膨脹,並透過 工:器之膨脹調整為霧化;及其特徵為水蒸氣過程工 介質Α之霧係於離心機分離,並藉泵呈液體供給氣 =器;&其特徵為剩餘氣體循環過程卫作介fAB透過 重縮機由離心機再度供給混合腔室。 Μ :申請專利範圍第13或14項之熱動力機,其特徵為壓 、、 泵及離心機係藉水蒸氣輪機及/或氣體輪機驅動 A8 B8 C8 D8 六'申請專利範圍 17.如申請專利範圍第13或14項之熱動力機’其特徵為水 蒸氣輪機及/或氣體輪機輸出軸功給外部消耗者。 18·如申請專利範圍第I3或14項之熱動力機,其特.徵為功 能組件亦即水蒸氣輪機,氣體輪機及混合腔室組合形 成一功能單元’亦即輪機;及功能組件,亦即冷凝器 '及離心機組合形成一功能單元,亦即冷凝離心機。 19.如申請專利範圍第13或I4項之熱動力機,其特徵為 蒸氣過程工作介質之相過渡溫度係低於熱動 m _ 刀機之周 圍溫度。 ί請先閎讀背面之注$項再填寫本頁j .裴. 訂· .丨竦, 經濟部中央標準局員工消費合作社印製 -22- 本紙張尺度適用中國國家標率(CNS ) A4規格(210X297公釐)if "continuing the month of the sixth, the patent application Fanyuan No. 87118937 patent application amendment scope of the patent application 1 鞴 古 古 妨 妨 · 88 修正 修正 修正 12 12 88 88 88 之 二 1 2 power cycle process and at least-the first The second cycle passes 3 = the method of converting thermal energy into mechanical energy in the machine, wherein the waste heat of the first: process is supplied to the second cycle process, and the waste heat of the second cycle is supplied to the loop process, which is characterized by gas one == It is a water vapour ring process, and the second cycle process is a sheet, and the material parent exchange occurs between the gas M ring process and the water vapour cycle process. 2. If the method of the scope of patent application No. 1 is characterized, The first and second cycle processes are performed simultaneously without material exchange with the environment. Order 3. If the method of the scope of the patent application is applied, it is characterized in that the working medium fA is used in the water vapor cycle, which contains a polymer couple. A substance or substance mixture of polar moment 'and a working medium M used in the gas circulation process, which contains a mixture of gaseous medium A and a second component b obtained from the water vapor cycle process, which contains a substance or substance with a low molecular dipole moment 4. The method according to the patent application_item 3, characterized in that the heat energy of the heat power machine is supplied from the outside, preferably used for the working medium A of the process of vaporizing liquid water vapour, and the scope of the patent application is 3 or 4 The method is characterized in that the permeation of the working medium A through the water vapor circulation process involves two types of cyclic processes. 6. The method of applying for item 3 or 4 of the patent scope is characterized by the gas phase of the working medium A in the water vapor circulation process. The gas phase of the working medium AB in the mixed gas circulation process. '-19- This paper is applicable to the Chinese National Standard (CNS) 1984 (210X297) 褒 if "Zhengyue Guangli, Patent Application Park No. 87118937 patent application Patent Scope Amendment 1-鞴 在 古 古-Date of Amendment ·· December 88 'Cheng No. 1 Power cycle process and at least-Second cycle pass 3 = Method of converting thermal energy into mechanical energy in the machine, where the first :: The waste heat of the process is supplied to the second cycle process, and the waste heat of the second cycle is supplied to the loop process, which is characterized by the fact that the gas one == is the water vapor still loop process, and the second cycle process is the sheet and the substance Exchange occurs between the air and the water vapor Μ loop process cycle. 2. If the method of the first scope of patent application is applied, it is characterized in that the first and second cycle processes are performed simultaneously without material exchange with the environment. Article 3. If the method according to the scope of the patent application is applied, it is characterized by using a working medium fA in a water vapor cycle, which contains a substance or a mixture of substances with a high molecular dipole moment, and using a working medium M in a gas circulation process, which contains Obtained from the mixture of the gas phase medium A and the second component b from the water vapor cycle process, which contains a substance or a mixture of substances having a low molecular dipole moment. 4. If the method of claiming patent _ item 3 is characterized in that the heat energy of the heat power machine is supplied from the outside, it is preferably used for the working medium A of the vaporized liquid water vapor process. It is characterized in that the working medium A permeates through two types of cyclic processes through the water vapor cycle mounting process. 6. The method for applying item 3 or 4 of the scope of patent application is characterized by the vapor phase of the working phase A of the working medium A of the water vapor cycle process and the gas phase of the working medium AB of the cycle gas working process. '-19- This paper applies Chinese National Standards (CNS), 84th position (210X297 gong), the method of applying for the patent scope V, such as the scope of the patent scope of the application of any of ..., which is characterized by circulating liquid-gas · liquid phase changes The output of shaft work occurs during the water vapor cycle. 8. If the method of claim 3 or 4 is applied, it is characterized by the change in the circulation volume or concentration of the working medium of the water vapor cycle process with respect to the working medium M of the gas cycle process. The output of the shaft work occurs in the gas process. 9. If the method of claim 3 or 4 is applied for patent, it is characterized in that the condensation of the working medium of the water loop process mainly occurs inside and during the expansion period of the working medium AB of the gas circulation process. H). The method according to item 3 or 4 of the scope of the patent application, characterized in that the mist generated by the phase transition of the working medium A in the water evaporation ring process uses a strange force field, preferably the centrifugal force field is separated from the working medium in the gas circulation process, and Once again, the working medium A is supplied with liquid water vapor cycle. For example, the method of claim 3 or 4 in the scope of patent application is characterized in that the working medium A of the water vapor cycle process and the second component B of the gas cycle health agent f ab may exist in the following combinations: n A = water and B = air; A = carbon dioxide and b = air / nitrogen; A = ammonia and B = air / nitrogen; A_ = ice bundle mixture and b = air / nitrogen; A = nitrogen and B = hydrogen; or A = nitrogen and B = inert gas. ^ A thermal power machine for converting thermal energy into mechanical energy, which has a number of -20th paper which is applicable from the Chinese National Tomb Standard (CNS) Congmi (210X29 ^^ 7 m —I— l 1__1 mi · 1 * ^ 11 -1 ^^ 1 ml · — In. In. A -¾, 1 f Please read the notes on the back before filling out this page} [Thermodynamic cycle process and at least one second cycle process, the waste heat of the W circle process The second cycle process is supplied, and the waste heat of the second cycle process is supplied to the first cycle process, which is characterized in that the process is a water vapor cycle process, and the second cycle process is a gas cycle process, and the material exchange occurs at Between the gas circulation process and the water vapor circulation process. Ά 13. According to the scope of the patent application! 2, the thermal power machine is characterized in that the thermal power machine contains at least the following functional components, fruit, gasifier, water vapor, turbine 'Mixing chamber, gas turbine' Condenser, centrifuge and compressor M. For example, the thermal power machine in the scope of patent application No. 13 is characterized by the working medium f A of the water vapor circulation process, which is supplied to the gasifier with increased pressure. , Supplied here Thermal energy gasification and expansion in steam turbines: ^ 15 · If the thermal power engine in the scope of patent application No. 13 or 14, is characterized by the compressed working medium of the exhaust gas of the steam turbine in the mixing chamber and the gas mixture ΑB, the expansion of the shaft work in the gas turbine, and through the work: the expansion of the device is adjusted to atomization; and its feature is that the water vapor process medium A is separated by the centrifuge, and is pumped to provide liquid gas = &Amp; is characterized in that the residual gas circulation process of Hyakusuke fAB is re-supplied to the mixing chamber from the centrifuge through the re-shrinking machine. Μ: The thermodynamic machine with the scope of patent application No. 13 or 14, which is characterized by pressure, pump, and Centrifuge is driven by water steam turbine and / or gas turbine A8 B8 C8 D8 Six 'application patent scope 17. If the patent application scope of the thermal power engine of item 13 or 14' is characterized by steam turbine and / or gas turbine output shaft To the external consumer. 18. If the thermal power engine in the scope of patent application No. I3 or 14 is used, it is characterized by a functional component, that is, a steam turbine, a gas turbine and a mixing chamber. 'I.e. turbine; and functional components, i.e. condensers' and the centrifuge combine to form a functional unit, i.e., a condensing centrifuge. 19. For a thermal power machine with a scope of patent application No. 13 or I4, it is characterized by steam process work The phase transition temperature of the medium is lower than the ambient temperature of the thermodynamic m _ knife machine. ΊPlease read the note on the back before filling in this page. J.Pei. Order ·. 丨 竦, Staff Consumer Cooperative, Central Standards Bureau, Ministry of Economic Affairs Printing-22- This paper size applies to China National Standards (CNS) A4 specifications (210X297 mm)
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PL2232019T3 (en) * 2007-12-17 2017-01-31 Klaus Wolter Method, device, and system for injecting energy into a medium
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US20120006024A1 (en) * 2010-07-09 2012-01-12 Energent Corporation Multi-component two-phase power cycle
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US2140254A (en) * 1936-10-21 1938-12-13 Ammonia Casale Societa Anonima Device for operating internal combustion engines with mixtures of ammonia, hydrogen, and nitrogen prepared from ammonia
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US4267692A (en) * 1979-05-07 1981-05-19 Hydragon Corporation Combined gas turbine-rankine turbine power plant
US4439988A (en) * 1980-11-06 1984-04-03 University Of Dayton Rankine cycle ejector augmented turbine engine
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US5437157A (en) * 1989-07-01 1995-08-01 Ormat Industries Ltd. Method of and apparatus for cooling hot fluids

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