TWI734029B - Production capacity estimation method for geothermal well - Google Patents

Production capacity estimation method for geothermal well Download PDF

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TWI734029B
TWI734029B TW107133223A TW107133223A TWI734029B TW I734029 B TWI734029 B TW I734029B TW 107133223 A TW107133223 A TW 107133223A TW 107133223 A TW107133223 A TW 107133223A TW I734029 B TWI734029 B TW I734029B
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geothermal
heat extraction
heat
well
model
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TW202012780A (en
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林大偉
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國立臺南大學
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    • 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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    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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    • Y02E10/10Geothermal energy

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Abstract

Embodiments disclose a production capacity estimation method for a geothermal well. The method includes: A. building a terrestrial heat storage level experiment system and obtaining a heat-retrieval data resulting from a heat-retrieval experiment; B. fitting the heat-retrieval data to a pore space heat-retrieval model, generating simulated physical properties in the environment such as pore space and fracture, and creating a terrestrial-heat retrieval model; C. scaling up a pipe flow model by the terrestrial heat storage level experiment system to create a single-well heat-retrieval model, receiving terrestrial heat production capacity data sets at different points in time, creating a value of total heat resistance, and identifying the difference there between for modifications of the single-well heat-retrieval model; and D. optimizing heat-retrieval data computed based on the single-well heat-retrieval model by using an optimization method.

Description

地熱井產能預估方法 Method for predicting productivity of geothermal wells

本發明係有關於一種可以用於模擬單井之地熱產能,以建立一地熱井之總熱阻,藉以可計算出最佳化取熱量之預估方法。 The present invention relates to a method that can be used to simulate the geothermal productivity of a single well to establish the total thermal resistance of a geothermal well, so that the optimal heat extraction estimation method can be calculated.

由於目前地球上的能源日漸短缺,因此尋求再生能源係已成為一刻不容緩之首要課題。再生能源係為一種具有恢復性之能源,可不斷補充和重複使用,最具代表性的有太陽能、風力能、海洋能、生物質能、地熱能等。隨著開發技術愈來愈成熟,其中地熱能在成本回收、產電效率和儲電容量雖還不如其它能源,且須克服許多地形岩層的限制,但比其它能源更加能夠持續循環利用,同時也能夠減少碳排放量問題,更可創造許多地熱產業機會。 Due to the current shortage of energy on the earth, the search for a renewable energy system has become the most important issue without delay. Renewable energy is a kind of restorative energy that can be continuously supplemented and reused. The most representative ones are solar energy, wind energy, ocean energy, biomass energy, geothermal energy, etc. As the development technology matures, geothermal energy is not as good as other energy sources in terms of cost recovery, power generation efficiency, and electricity storage capacity, and it must overcome the limitations of many terrain and rock formations, but it is more sustainable than other energy sources and can be recycled and used at the same time. It can reduce carbon emissions and create many opportunities for the geothermal industry.

因此有中華民國103年1月16日所公開之發明第201402943號「用於開採能源的單井、自流地熱系統」專利案,其係揭露:提供一種再生性能源、單井、一次自流、地熱熱量/電力產生系統,該系統使用熱交換器或渦輪機/發電機獲取自然產生之地下地熱熱量以加熱水及/或產生機械力/電力。可(諸如)使用真空絕緣使界定工作流體流動路徑之地下結構絕緣,以增加系統效率且確保實質上自生之工作流體流動。 Therefore, there is the invention No. 201402943 "Single Well, Artesian Geothermal System for Energy Extraction" published by the Republic of China on January 16, 103, which discloses: Provide a renewable energy, single well, primary artesian, geothermal A heat/power generation system that uses heat exchangers or turbines/generators to obtain naturally generated underground geothermal heat to heat water and/or generate mechanical power/electricity. Vacuum insulation can be used, for example, to insulate the underground structure that defines the working fluid flow path to increase system efficiency and ensure a substantially self-generating working fluid flow.

由於目前進行現地的地熱發電效能預測時,地熱井之產能均是利用現地實際人工測試之產能測試,主要原因為缺乏有效可靠之模型以及對儲集層熱質傳特性所知太少。因此於地熱的運用中,仍然需要實際進行開採,才能 獲得地熱以供應用。往往開採地熱後的取熱效率不如預期,而無法充分的運用地熱。 At present, when performing on-site geothermal power generation performance predictions, the productivity of geothermal wells is tested using actual on-site manual tests. The main reason is the lack of effective and reliable models and the lack of knowledge about the thermal and mass transfer characteristics of the reservoir. Therefore, in the application of geothermal heat, it is still necessary to actually mine to Get geothermal heat for supply. Often, the heat extraction efficiency after geothermal extraction is not as good as expected, and the geothermal energy cannot be fully utilized.

因此本發明的申請人曾申請核准有中華民國107年6月1日所公告之發明第I625460「增強型地熱之最佳取熱系統及其建立方法」專利案,其係揭露:建立一數值模型進行模擬取熱。利用該數值模型經模擬取熱後取得一模擬數據。透過一取熱實驗以驗證該數值模型之正確性。利用該取熱實驗取得一實驗數據,而與該模擬數據進行比對,藉以驗證該數值模型之正確性。以一最佳化方法取得在該模擬數據中之一最佳操作條件。利用該最佳操作條件建立一增強型地熱之最佳取熱系統。藉以可供輸入地質孔隙條件之平均粒徑和壓力,而查詢得知相對應之該最大取熱量之質量流率。 Therefore, the applicant of the present invention has applied for the approval of the invention No. I625460 "Best heat extraction system and its establishment method for enhanced geothermal" announced on June 1, 2007, which discloses: the establishment of a numerical model Perform simulated heat extraction. Use the numerical model to obtain a simulation data after simulating the heat. A thermal experiment was performed to verify the correctness of the numerical model. The heat extraction experiment is used to obtain an experimental data, which is compared with the simulated data to verify the correctness of the numerical model. An optimization method is used to obtain one of the best operating conditions in the simulation data. Use the optimal operating conditions to establish an enhanced geothermal optimal heat extraction system. With the input of the average particle size and pressure of the geological pore conditions, the corresponding mass flow rate of the maximum heat extraction can be obtained by querying.

該專利前案雖然可以供查詢在地熱儲集層中之不同地層平均粒徑和壓力,相對應之最大取熱量之質量流率,以做為取得最大取熱量之質量流率參考之用。惟其無法針對各個單井建立其總熱阻,以對於最佳化取熱量進行預估,因此於使用上有其不足之處。 Although the previous patent case can be used to query the average particle size and pressure of different formations in the geothermal reservoir, the mass flow rate of the corresponding maximum heat extraction can be used as a reference for the mass flow rate to obtain the maximum heat extraction. However, it cannot establish the total thermal resistance for each single well in order to estimate the optimal heat extraction, so it has its shortcomings in use.

爰此,有鑑於目前地熱發電廠之建置必須先掌握地熱井之產能,而目前產能之掌握均來自現地產能測試。現地產能預測為發電廠經濟效益評估中一成熟之評估方式,相關之成本資料均不難獲得。惟此評估中最重要之一環為每次產能測試之成本及對地熱井之影響,在現地以注氣或注水之方式測試地熱井所能產出之最大焓值,每一次產能測試約需三至四週,經費預估約需三百萬,但僅能獲得四組不同井口試氣管徑之產能值。因此耗費時間久、成本高、經濟效益差。 In view of this, in view of the current construction of geothermal power plants, the production capacity of geothermal wells must be mastered first, and the current production capacity control comes from on-site production testing. On-site production capacity prediction is a mature evaluation method in the economic benefit evaluation of power plants, and relevant cost information is not difficult to obtain. However, one of the most important links in this assessment is the cost of each productivity test and its impact on geothermal wells. The maximum enthalpy value that can be produced by geothermal wells is tested by gas or water injection on site. Each productivity test requires about three Up to four weeks, the estimated expenditure is about 3 million yuan, but only four sets of production values of different wellhead gas test pipe diameters can be obtained. Therefore, it takes a long time, high cost, and poor economic efficiency.

故本發明提供一種地熱井產能預估方法,包含有:建立一地熱儲集層實驗系統,經由取熱實驗藉以獲得一取熱結果,該地熱儲集層實驗系統係 藉由一高壓測試管路所形成之一測試段,藉以模擬一工作流體流經一儲集層之該取熱結果;利用該取熱結果擬合一孔隙取熱模型,完成於孔隙及裂隙條件下之一模擬物理特性,建立一地熱取熱模型,係以該地熱儲集層實驗系統經由該取熱結果,再依照該測試段以等比例,利用一電腦以電腦模擬該工作流體於該儲集層內之取熱現象,並獲得一模擬結果,比較該模擬結果與該取熱結果之差異性;利用該地熱儲集層實驗系統放大尺度,並結合一管流模型模擬建立一單井取熱模型,輸入不同時間點的一地熱產能資料,建立一地熱井之總熱阻,並比較其差異性,藉以修正該單井取熱模型,於該電腦中以該地熱儲集層實驗系統,結合該管流模型放大至現地尺度模型,以形成該單井取熱模型,藉以供實際應用於現地之地熱系統進行評估;利用一最佳化方法使該單井取熱模型計算最佳化取熱量,利用該最佳化方法計算出在已知地熱井深度及岩層孔隙狀態下,及最適合之地熱井注入流量,以獲得流經地熱井後可擷取之最大取熱量。 Therefore, the present invention provides a method for predicting the productivity of geothermal wells, which includes: establishing a geothermal reservoir experimental system, and obtaining a heat extraction result through heat extraction experiments. The geothermal reservoir experimental system is A test section is formed by a high-pressure test pipeline to simulate the heat extraction result of a working fluid flowing through a reservoir; use the heat extraction result to fit a pore heat extraction model to complete the pore and fracture conditions The next one is to simulate physical characteristics to establish a geothermal heat extraction model. The geothermal reservoir experimental system uses the heat extraction results, and then uses a computer to simulate the working fluid in the reservoir in proportion to the test section. The heat extraction phenomenon in the reservoir is obtained, and a simulation result is obtained, and the difference between the simulation result and the heat extraction result is compared; the scale of the geothermal reservoir experimental system is used to enlarge the scale, combined with a pipe flow model to simulate the establishment of a single well Thermal model, input a geothermal productivity data at different time points, establish the total thermal resistance of a geothermal well, and compare its differences, so as to modify the single well heat extraction model, and use the geothermal reservoir experimental system in the computer, Combine the pipe flow model and enlarge it to the local scale model to form the single-well heat extraction model, which can be used to evaluate the geothermal system that is actually applied to the site; an optimization method is used to optimize the calculation of the single-well heat extraction model. Heat, using the optimization method to calculate the most suitable injection flow rate of the geothermal well under the known depth of the geothermal well and the state of the pores of the formation, so as to obtain the maximum heat extraction that can be extracted after flowing through the geothermal well.

上述取熱結果包含於不同之介質粒徑、壓力、流量、孔隙率、層流狀態或流速下,該工作流體的實驗物理特性之變化。 The above-mentioned heat extraction results include changes in the experimental physical characteristics of the working fluid under different medium particle diameters, pressures, flow rates, porosity, laminar flow conditions or flow rates.

上述實驗物理特性包含熱交換效率、熱對流係數、熱分散性、取熱量其中之一或其任意組合。 The above-mentioned experimental physical characteristics include one of heat exchange efficiency, heat convection coefficient, heat dispersion, heat extraction, or any combination thereof.

上述模擬物理特性係包含熱擴散性、有效熱傳導係數、有效比熱、縱向熱分散性、橫向熱分散性其中之一或其任意組合。 The aforementioned simulated physical properties include one or any combination of thermal diffusivity, effective thermal conductivity, effective specific heat, longitudinal thermal dispersibility, and lateral thermal dispersibility.

以上述取熱結果提供該電腦中之該孔隙取熱模型擬合出在各種不同壓力與流量條件下之該熱分散性,並與取熱實驗過程所量測的取熱量與入出口溫差進行比較其差異性。 Use the above heat extraction results to provide the pore heat extraction model in the computer to fit the heat dispersion under various pressure and flow conditions, and compare it with the heat extraction and the temperature difference between the inlet and outlet measured during the heat extraction experiment Its difference.

上述將時間在前的任一已知地熱井之該地熱產能資料輸入該單井取熱模型,而獲得該已知地熱井之一舊總熱阻,再將時間在後的該地熱產能資料輸入該單井取熱模型,而獲得該已知地熱井的一新總熱阻,比較該新、舊總 熱阻之差異性,藉以修正並更新該單井取熱模型,以獲得新的該單井取熱模型,並驗證該已知地熱井隨時間之流量衰減狀況。 As mentioned above, input the geothermal productivity data of any known geothermal well before the time into the single-well heat extraction model to obtain the old total thermal resistance of one of the known geothermal wells, and then input the geothermal productivity data later The single-well heat model is obtained, and a new total thermal resistance of the known geothermal well is obtained, and the new and old total thermal resistance are compared. The difference in thermal resistance is used to modify and update the single-well heat extraction model to obtain a new single-well heat extraction model, and to verify the flow attenuation of the known geothermal well over time.

上述地熱產能資料係包含有該地熱井之深度、直徑、井底溫度、出口溫度、出口壓力及流量之數據。 The above-mentioned geothermal productivity data includes data on the depth, diameter, bottom hole temperature, outlet temperature, outlet pressure and flow rate of the geothermal well.

藉由上述電腦擬合出以一布林克曼模型與一熱傳模組共同建立之該孔隙取熱模型做為基礎之該地熱取熱模型,又該最佳化方法係為簡易共軛梯度法。 The geothermal heat extraction model based on the pore heat extraction model jointly established by a Brinkman model and a heat transfer module is fitted by the above computer, and the optimization method is a simple conjugate gradient Law.

上述技術特徵具有下列之優點: The above technical features have the following advantages:

1.可發展出模擬地熱井產能測試之相似產能的單井取熱模型,藉以能降低實際產能測試之成本與時間之耗費。 1. A single well heat extraction model with similar productivity can be developed to simulate the productivity test of geothermal wells, so as to reduce the cost and time consumption of the actual productivity test.

2.利用單井取熱模型可以預測目前單井在不同模擬物理特性下的測試結果,並可進行最佳化以預測最佳之產能結果。 2. Using the single-well heat extraction model can predict the current test results of a single well under different simulated physical characteristics, and can be optimized to predict the best productivity results.

3.進一步可輸入不同時間點的一地熱產能資料,以建立一地熱井之總熱阻,並求出在設定地層條件下之最佳化取熱量,進而提昇取熱效率。 3. It is further possible to input a geothermal productivity data at different time points to establish the total thermal resistance of a geothermal well, and obtain the optimal heat extraction under the set formation conditions, thereby improving the heat extraction efficiency.

(1):測試段 (1): Test section

(11):正排量泵 (11): Positive displacement pump

(12):預熱水槽 (12): Preheating water tank

(13):流量計 (13): Flowmeter

(14):壓力調節閥 (14): Pressure regulating valve

(15):冷卻水槽 (15): Cooling water tank

(16):訊號線 (16): Signal line

(17):資料記錄器 (17): Data Logger

(18):電腦 (18): Computer

(19):熱電偶 (19): Thermocouple

(2):單井地熱系統 (2): Single well geothermal system

(2A):雙井地熱系統 (2A): Double-well geothermal system

(21):冷工作流體 (21): Cold working fluid

(22):熱工作流體 (22): Hot working fluid

(3):孔隙取熱模型 (3): Pore heat model

(31):入口 (31): Entrance

(32):出口 (32): Export

(4):圓柱管 (4): Cylindrical tube

(41):多孔隙介質 (41): Porous media

[第一圖]係為本發明實施例之地熱井產能預估方法的流程圖。 [The first figure] is a flowchart of a method for predicting productivity of geothermal wells according to an embodiment of the present invention.

[第二圖]係為本發明實施例地熱儲集層實驗系統之配置圖。 [The second figure] is the configuration diagram of the geothermal reservoir experimental system according to the embodiment of the present invention.

[第三圖]係為本發明實施例地熱取熱模型之示意圖。 [Third Figure] is a schematic diagram of a geothermal heat extraction model according to an embodiment of the present invention.

[第四圖]係為本發明實施例孔隙取熱模型之示意圖。 [Fourth Figure] is a schematic diagram of a pore heat model according to an embodiment of the present invention.

[第五圖]係為本發明實施例於10、30MPa下空管與粒徑1.54mm及2.03mm隨流量變化之出入口溫差的比較圖。 [Fifth Figure] is a comparison diagram of the temperature difference between the inlet and outlet of the empty tube and the diameter of 1.54mm and 2.03mm as the flow rate changes at 10, 30MPa in the embodiment of the present invention.

[第六圖]係為本發明實施例取熱結果與模擬結果之測試段於出入口溫差的比較圖。 [The sixth figure] is a comparison diagram of the temperature difference between the inlet and outlet of the test section of the heat-taking result and the simulation result of the embodiment of the present invention.

[第七圖]係為本發明實施例取熱結果與模擬結果之取熱量的比較圖。 [The seventh figure] is a comparison diagram of the heat extraction result of the embodiment of the present invention and the simulation result.

[第八圖]係為本發明實施例裂隙流與孔隙流在不同流量下之縱向與橫向熱分散性結果的比較圖。 [The eighth figure] is a comparison diagram of the longitudinal and transverse thermal dispersion results of fractured flow and pore flow under different flow rates in the embodiment of the present invention.

[第九圖]係為本發明實施例單井取熱模型之示意圖。 [Figure 9] is a schematic diagram of a single well heat extraction model according to an embodiment of the present invention.

請參閱第一圖所示,本發明實施例為一種地熱井產能預估方法,包含下列步驟: A.建立一地熱儲集層實驗系統,經由取熱實驗藉以獲得一取熱結果。如第二圖所示,係利用該地熱儲集層實驗系統進行取熱實驗,以獲得該取熱結果。該地熱儲集層實驗系統係藉由一高壓測試管路所形成之一測試段(1),於填充不同介質粒徑,並改變一工作流體相關壓力及流量等參數,藉以模擬該工作流體流經一儲集層之該取熱結果。本發明係以水做為該工作流體。利用一正排量泵(11)以定流定壓方式,將該工作流體通過一預熱水槽(12)及一流量計(13)後注入該測試段(1)內,然後該工作流量再通過一壓力調節閥(14)、一冷卻水槽(15)後,再循環回到該正排量泵(11)。同時將該測試段(1)所得到之該取熱效率,透過一訊號線(16)傳送到一資料記錄器(17)及一電腦(18)。利用該測試段(1)進行孔隙介質取熱試驗,藉以可獲得不同介質粒徑、流量、儲集層壓力等之實驗物理特性。並且可得知不同之孔隙率、層流狀態、流速及壓力等實驗物理特性於操作過程中的差異。於取熱實驗過程中進行水壓力、流量及岩層粒徑之測試,可獲得該工作流體的上述實驗物理特性,例如熱交換效率、熱對流係數、熱分散性及取熱量等。進一步可針對不同孔隙率之水熱交換效率、孔隙所造成的壓損及浮力等相關參數進行上述實驗物理特性之實驗。 Please refer to the first figure. The embodiment of the present invention is a method for predicting the productivity of a geothermal well, which includes the following steps: A. Establish a geothermal reservoir experimental system to obtain a heat extraction result through heat extraction experiments. As shown in the second figure, the geothermal reservoir experimental system is used to conduct heat extraction experiments to obtain the heat extraction results. The geothermal reservoir experimental system is a test section (1) formed by a high-pressure test pipeline, which is filled with different medium particle diameters and changes the relevant pressure and flow parameters of a working fluid to simulate the flow of the working fluid. The heat extraction result of a reservoir. The present invention uses water as the working fluid. Using a positive displacement pump (11) in a constant flow and constant pressure mode, the working fluid is injected into the test section (1) after passing through a preheating tank (12) and a flow meter (13), and then the working flow is then After passing through a pressure regulating valve (14) and a cooling water tank (15), it recirculates back to the positive displacement pump (11). At the same time, the heat extraction efficiency obtained in the test section (1) is transmitted to a data recorder (17) and a computer (18) through a signal line (16). Use this test section (1) to carry out the heat extraction test of the porous medium, so as to obtain the experimental physical characteristics of different medium particle size, flow rate, reservoir pressure and so on. And we can know the difference in the operation process of different porosity, laminar flow state, flow rate and pressure and other experimental physical characteristics. The water pressure, flow rate, and rock diameter are tested during the heat extraction experiment, and the above-mentioned experimental physical characteristics of the working fluid, such as heat exchange efficiency, heat convection coefficient, heat dispersion, and heat extraction, can be obtained. Furthermore, the above-mentioned experimental physical characteristics experiments can be carried out for related parameters such as the water-heat exchange efficiency of different porosities, the pressure loss caused by the pores, and the buoyancy.

上述該測試段(1)的入口端連接該預熱水槽(12),可控制該工作流體注入時的溫度,再於該測試段(1)的出口端連接該冷卻水槽(15),藉以使其出口水溫下降以方便系統循環。該預熱水槽(12)及該冷卻水槽(15)的目的為使該正排量泵(11)及該壓力調節閥(14)能在操作溫度內運作,而該測試段(1)並以加熱器輸入固定電壓以加溫該測試段(1)達到熱平衡,該測試段(1)內填充不同的孔隙介質,並於其外壁裝設10組熱電偶(19),以環狀方式環繞於該測試段(1)的外壁凹槽內,再以保溫棉及絕熱材料包覆,降低熱損失的影響,其目的是要量測穩態及暫態時之外壁溫度反應,進而帶入下列計算公式(一)得到壁內溫度的變化。該取熱實驗為測試該工作流體於孔隙介質的熱傳特性,其取熱結果透過定流量、壓力及熱通量的設定,以計算其熱對流係數和熱交換量,觀察其溫度分布。並利用取熱實驗之溫度記錄,推算該測試段(1)之內壁溫度分布,並提供後續模型以擬合出模型之熱分散性設定。該計算公式(一)如下所示:

Figure 107133223-A0305-02-0008-1
The inlet end of the above-mentioned test section (1) is connected to the preheating water tank (12), which can control the temperature of the working fluid when it is injected, and then the cooling water tank (15) is connected to the outlet end of the test section (1), so that The outlet water temperature drops to facilitate system circulation. The purpose of the preheating water tank (12) and the cooling water tank (15) is to enable the positive displacement pump (11) and the pressure regulating valve (14) to operate within the operating temperature, and the test section (1) is The heater inputs a fixed voltage to heat the test section (1) to achieve thermal equilibrium. The test section (1) is filled with different porous media, and 10 sets of thermocouples (19) are installed on the outer wall of the test section (1), which surrounds the test section (1) in a ring The outer wall groove of the test section (1) is then covered with thermal insulation cotton and thermal insulation material to reduce the influence of heat loss. The purpose is to measure the temperature response of the outer wall in steady state and transient state, and then bring the following calculations Formula (1) obtains the temperature change in the wall. The heat extraction experiment is to test the heat transfer characteristics of the working fluid in the pore medium. The heat extraction results are used to calculate the heat convection coefficient and heat exchange amount through the setting of constant flow, pressure and heat flux, and observe its temperature distribution. And use the temperature record of the heat extraction experiment to calculate the temperature distribution of the inner wall of the test section (1), and provide a follow-up model to fit the thermal dispersion setting of the model. The calculation formula (1) is as follows:
Figure 107133223-A0305-02-0008-1

TIW:內壁溫度(K); TOW:外壁溫度(K); Qr:管表面之輸入的熱通量(W/m2); d1:測試段內徑(m); d2:測試段外徑(m); λ sus :不銹鋼之熱傳導率(W/mk)。 T IW : inner wall temperature (K); T OW : outer wall temperature (K); Q r : input heat flux on the surface of the tube (W/m 2 ); d 1 : inner diameter of the test section (m); d 2 :The outer diameter of the test section (m); λ s u s :The thermal conductivity of stainless steel (W/mk).

本發明的取熱實驗已完成7.5MPa下空管(裂隙流)、石英砂粒徑1.54mm及2.03mm條件下,流量為0.33g/s、0.66g/s、0.99g/s及1.32g/s之取熱實驗。 預計還需持續建立在8MPa、9MPa、10MPa、11MPa及12.5MPa各項壓力下之不 同的取熱結果,以獲得在不同壓力、流量及孔隙條件下完整之該實驗物理特性。 而針對於裂隙條件之實驗方法相同於上述孔隙條件之實驗方法。 The heat extraction experiment of the present invention has been completed under the 7.5MPa hollow tube (fracture flow), under the conditions of the quartz sand particle size of 1.54mm and 2.03mm, the flow rate is 0.33g/s, 0.66g/s, 0.99g/s and 1.32g/ s of heat extraction experiment. It is expected that it will continue to be established under the various pressures of 8MPa, 9MPa, 10MPa, 11MPa and 12.5MPa. The same heat extraction results to obtain the complete physical characteristics of the experiment under different pressure, flow and pore conditions. The experimental method for the fracture conditions is the same as the experimental method for the above-mentioned pore conditions.

B.利用該取熱結果擬合一孔隙取熱模型,完成於孔隙及裂隙條件下之一模擬物理特性,建立一地熱取熱模型。其係以該地熱儲集層實驗系統經由取熱實驗獲得之該取熱結果,再依照該測試段(1)以等比例,藉由該電腦(18)擬合出以布林克曼〔Brinkman〕模型與熱傳模組之該孔隙取熱模型做為基礎之該地熱取熱模型,以供利用該電腦(18)以電腦模擬該工作流體於地熱儲集層內之取熱現象的各種模擬物理特性。該模擬物理特性係包含以該取熱結果提供該電腦(18)中之該孔隙取熱模型以擬合出在各種不同壓力與流量條件下之熱分散性,藉由與取熱實驗過程所量測的取熱量與入出口溫差之熱分散性進行比較其差異性,並進行修改,以擬合出更準確的該孔隙取熱模型,藉以建立該地熱取熱模型。 B. Use the heat extraction results to fit a pore heat extraction model, complete a physical characteristic simulation under the conditions of pores and cracks, and establish a geothermal heat extraction model. It is based on the heat extraction result obtained by the geothermal reservoir experimental system through the heat extraction experiment, and then according to the test section (1) in equal proportions, the computer (18) is used to fit the Brinkman (Brinkman) ] The geothermal heat extraction model based on the model and the pore heat extraction model of the heat transfer module is used for various simulations using the computer (18) to simulate the heat extraction phenomenon of the working fluid in the geothermal reservoir Physical characteristics. The simulated physical properties include providing the pore heat model in the computer (18) with the heat extraction result to fit the heat dispersion under various pressure and flow conditions, which is measured by the heat extraction experiment process The difference between the measured heat extraction and the heat dispersion of the temperature difference between the inlet and outlet is compared and modified to fit a more accurate pore heat extraction model to establish the geothermal heat extraction model.

請參考第三圖所示,不論是同時可供冷工作流體(21)輸入,而熱工作流體(22)輸出的單井地熱系統(2);或是其中一井可供一冷工作流體(21)輸入,而另一井可供熱工作流體(22)輸出的雙井地熱系統(2A)。以水做為工作流體的取熱模式均與孔隙熱傳相關,故以該孔隙取熱模型(3)做為合理之該地熱取熱模型。該孔隙取熱模型(3)係於該電腦(18)中以電腦模擬方式,探討該工作流體於多孔介質中熱傳之關係,其所建構的該地熱取熱模型設定為流場與溫度場兩種模型之耦合類型,其數學模型包含連續方程式、動量平衡方程式、介質能量平衡方程式及流體能量平衡方程式等。 Please refer to the third figure, whether it is a single-well geothermal system (2) that simultaneously provides cold working fluid (21) input and hot working fluid (22) output; or one of the wells can provide a cold working fluid ( 21) A dual-well geothermal system (2A) with input and another well available for output of thermal working fluid (22). The heat extraction modes using water as the working fluid are all related to pore heat transfer, so the pore heat extraction model (3) is used as a reasonable geothermal heat extraction model. The pore heat extraction model (3) is used in the computer (18) to explore the relationship between the heat transfer of the working fluid in the porous medium, and the geothermal heat extraction model constructed by it is set as the flow field and the temperature field The coupling type of the two models, its mathematical models include continuous equation, momentum balance equation, medium energy balance equation and fluid energy balance equation, etc.

該連續方程式之計算公式(二)如下所示:

Figure 107133223-A0305-02-0009-2
The calculation formula (2) of the continuous equation is as follows:
Figure 107133223-A0305-02-0009-2

該動量平衡方程式之計算公式(三)如下所示:

Figure 107133223-A0305-02-0010-3
The calculation formula (3) of the momentum balance equation is as follows:
Figure 107133223-A0305-02-0010-3

多孔介質熱傳之統御方程式係由平均體積法求得,使孔隙和介質之間能個別獲得固有的平均性值,在介質與流體之間的熱傳平衡方程式已被廣泛的用於分析多孔介質之熱傳。因此以傅立葉定律(Fourier's Law)描述在多孔介質中完全飽和之介質與流體。該介質能量平衡方程式之計算公式(四)如下所示:

Figure 107133223-A0305-02-0010-4
The governing equation of heat transfer in porous media is obtained by the average volume method, so that the pores and the media can individually obtain the inherent average value. The heat transfer balance equation between the medium and the fluid has been widely used in the analysis of porous media The heat transfer. Therefore, Fourier's Law is used to describe media and fluids that are completely saturated in porous media. The calculation formula (4) of the medium energy balance equation is as follows:
Figure 107133223-A0305-02-0010-4

該流體能量平衡方程式之計算公式(五)如下所示:

Figure 107133223-A0305-02-0010-5
The calculation formula (5) of the fluid energy balance equation is as follows:
Figure 107133223-A0305-02-0010-5

方程式中ρ為密度、u為流體的流速、Qbr為質量力、ε為孔隙率、μ為流體的動力黏度、K為滲透率、F為強制力項、Cp為常壓比熱及k為熱傳導係數。如第四圖所示,於該地熱取熱模型中,該孔隙取熱模型(3)表面設定為一恆定熱源對其內部加熱,且一端設有一入口(31),以供冷工作流體(21)輸入,另一端設有一出口(32),以供加後後成為熱工作流體(22)輸出。分別改變入口流速、系統壓力與內部介質粒徑,觀察出口溫度及內壁溫度的變化。藉由該孔隙取熱模型(3),將可電腦模擬一封閉區域中之流體注入儲集層後,經由該孔隙取熱模型(3)計算取熱之現象,並獲得一模擬結果。所要比較之模擬結果為流體之取熱量,並將取熱實驗記錄之溫度,用以計算沿著儲集層之整體溫度分布,並與該孔隙取熱模型(3)模擬結果比較之。計算公式如下所示:

Figure 107133223-A0305-02-0010-15
In the equation, ρ is the density, u is the flow velocity of the fluid, Q br is the mass force, ε is the porosity, μ is the dynamic viscosity of the fluid, K is the permeability, F is the force term, C p is the atmospheric specific heat, and k is Thermal conductivity. As shown in the fourth figure, in the geothermal heat extraction model, the surface of the pore heat extraction model (3) is set as a constant heat source to heat its interior, and one end is provided with an inlet (31) for cooling the working fluid (21) ) Input, the other end is provided with an outlet (32) for the output of the hot working fluid (22) after being added. Change the inlet flow rate, system pressure and internal medium particle size respectively, and observe the changes of outlet temperature and inner wall temperature. Using the pore heat extraction model (3), after injecting fluid in a closed area that can be computer-simulated into the reservoir, the pore heat extraction model (3) calculates the heat extraction phenomenon and obtains a simulation result. The simulation result to be compared is the calorific value of the fluid, and the temperature recorded by the thermal experiment is used to calculate the overall temperature distribution along the reservoir, and compare it with the simulation result of the pore thermal model (3). The calculation formula is as follows:
Figure 107133223-A0305-02-0010-15

經由測試不同壓力下之模擬結果,係已確定該地熱儲集層實驗系統足以模擬2-3千公尺深之地底儲集層之現象。如第五圖所示,係為10、30MPa 下空管與粒徑1.54mm及2.03mm隨流量變化之出入口溫差。先利用內建之水性質做為該地熱取熱模型探討10MPa及30MPa下之狀況。模擬結果可以觀察到壓力對取熱之影響極微,由此可以證明,以該地熱儲集層實驗系統在100大氣壓左右建立的該測試段(1),已足以模擬地底儲集層之狀況。亦觀察到孔隙的變化影響亦小,但空管(裂隙流)與孔隙條件之影響則有顯著之差異。而流量對取熱為最主要之影響,由此可知,未來可進一步針對在取熱實驗與電腦模擬上將進行10MPa附近不同壓力下空管與不同孔隙率條件之不同流量之取熱分析。 After testing the simulation results under different pressures, it has been determined that the geothermal reservoir experimental system is sufficient to simulate the phenomenon of underground reservoirs at a depth of 2-3 thousand meters. As shown in the fifth figure, the system is 10, 30MPa The temperature difference between the inlet and outlet of the lower hollow tube and the diameter of 1.54mm and 2.03mm with flow changes. First use the built-in water properties as the geothermal heat extraction model to explore the conditions under 10MPa and 30MPa. The simulation results show that the pressure has minimal effect on heat extraction, which proves that the test section (1) established with the geothermal reservoir experimental system at about 100 atmospheres is sufficient to simulate the condition of the underground reservoir. It has also been observed that the influence of pore changes is also small, but there are significant differences in the influence of empty pipes (fracture flow) and pore conditions. The flow rate is the most important influence on heat extraction. It can be seen that in the future, heat extraction experiments and computer simulations will be carried out in the heat extraction experiments and computer simulations to conduct further heat extraction analysis for empty pipes at different pressures around 10MPa and different porosity conditions.

該地熱取熱模型之熱擴散性質為一經驗值,類似熱對流係數必須依賴實驗獲得。故本發明以取熱實驗之取熱結果擬合該孔隙取熱模型建立合理之該地熱取熱模型即為此緣故。孔隙熱傳中之模擬物理特性之定義如下。 The thermal diffusion property of the geothermal heat extraction model is an empirical value, and the similar thermal convection coefficient must be obtained by experiment. Therefore, the present invention uses the heat extraction results of the heat extraction experiment to fit the pore heat extraction model to establish a reasonable geothermal heat extraction model for this reason. The definition of simulated physical properties in pore heat transfer is as follows.

熱擴散性:

Figure 107133223-A0305-02-0011-16
。 Thermal diffusivity:
Figure 107133223-A0305-02-0011-16
.

有效熱傳導係數:

Figure 107133223-A0305-02-0011-8
Effective thermal conductivity:
Figure 107133223-A0305-02-0011-8

有效比熱:C peff =ε.ρ f .C p,f +(1-ε).ρ p .C p,p Effective specific heat: C peff = ε. ρ f . C p,f +(1- ε ) . ρ p . C p,p .

縱向熱分散性:

Figure 107133223-A0305-02-0011-17
。 Longitudinal thermal dispersion:
Figure 107133223-A0305-02-0011-17
.

橫向熱分散性:

Figure 107133223-A0305-02-0011-18
。 Transverse thermal dispersion:
Figure 107133223-A0305-02-0011-18
.

由於本發明已完成在空管、粒徑為1.54mm及2.03mm情況下,建立該地熱取熱模型。已建立之該地熱儲集層實驗系統亦已完成在7.5MPa空管條件時,流量為0.33g/s、0.66g/s、0.99g/s與1.32g/s之取熱實驗,繼而將該取熱結果擬合該地熱取熱模型之模擬結果,以獲得此條件下之熱擴散係數。藉由調整該地 熱取熱模型中的縱向與橫向熱分散性(λ lo 與λ tr ),使該地熱取熱模型之電腦模擬情況可擬合取熱實驗之取熱結果,並與取熱實驗比較出入口溫差及取熱量,以確認電腦模擬之正確性。經校驗後發現,取熱實驗之取熱結果與電腦模擬之模擬結果,該測試段於出入口溫差比較結果如第六圖所示,其平均誤差值皆小於0.001%。而取熱結果與模擬結果之取熱量比較結果如第七圖所示,其平均誤差值皆小於0.72%。由上述比較結果可看出模擬結果與取熱結果吻合,故可建立正確之熱分散性。 Because the present invention has completed the establishment of the geothermal heat extraction model in the case of an empty tube with a particle size of 1.54mm and 2.03mm. The established experimental system for the geothermal reservoir has also completed the heat extraction experiments with flow rates of 0.33g/s, 0.66g/s, 0.99g/s and 1.32g/s under 7.5MPa empty pipe conditions. The thermal result is fitted to the simulation result of the geothermal thermal model to obtain the thermal diffusivity under this condition. By adjusting the longitudinal and lateral heat dispersion (λ lo and λ tr ) in the geothermal heat extraction model, the computer simulation of the geothermal heat extraction model can be fitted to the heat extraction results of the heat extraction experiment, and be combined with the heat extraction experiment Compare the temperature difference between the entrance and exit and the amount of heat to confirm the correctness of the computer simulation. After verification, it was found that the temperature difference between the entrance and exit of the test section was compared with the simulation result of the computer simulation, and the average error value was less than 0.001%. The comparison between the heat extraction result and the simulation result is shown in the seventh figure, and the average error value is less than 0.72%. From the above comparison results, it can be seen that the simulation results are consistent with the heat extraction results, so the correct heat dispersion can be established.

如第六圖及第七圖所示,係顯示質量流率增大,使取熱量增大,但造成該測試段之出入口溫差減小。因此隨著質量流率之增加,取熱量有一可預測之趨近值。因此,於實際的地熱單井中將存在一適當之出口流量可獲得一最大之取熱量。並且發現在熱分散性上,如第八圖所示,根據熱分散性(kdisp)定義而言,流速、比熱與分散性均會對熱擴散係數產生影響。但流速為平方項,因此在低流速時孔隙熱傳之分散性為一有影響力之因子,此時孔隙熱傳效果大於裂隙流(空管)之熱傳效果。但流速上升時,分散性之影響迅速降低,故流率上升後,造成空管之熱傳較孔隙熱傳之流動為佳。亦即,低流速在孔隙條件下取熱效果較好,但高流速時則是裂隙條件較好。 As shown in the sixth and seventh graphs, it is shown that the mass flow rate increases, which increases the heat extraction, but causes the temperature difference between the inlet and outlet of the test section to decrease. Therefore, as the mass flow rate increases, the heat extraction has a predictable approach value. Therefore, in the actual geothermal single well, there will be an appropriate outlet flow rate to obtain a maximum heat extraction. And found that in terms of thermal dispersibility, as shown in Figure 8, according to the definition of thermal dispersibility (k disp ), flow velocity, specific heat, and dispersibility all affect the thermal diffusivity. But the flow velocity is a square term, so the dispersion of pore heat transfer at low flow velocity is an influential factor. At this time, the pore heat transfer effect is greater than the heat transfer effect of the fractured flow (empty pipe). However, when the flow rate increases, the influence of dispersion decreases rapidly, so when the flow rate increases, the heat transfer of the empty tube is better than the flow of the pore heat transfer. In other words, low flow rates have better heat extraction effects under pore conditions, but high flow rates have better fracture conditions.

C.利用該地熱儲集層實驗系統放大尺度,並結合一管流模型模擬建立一單井取熱模型,輸入不同時間點的一地熱產能資料,建立一地熱井之總熱阻,並比較其差異性,藉以修正該單井取熱模型。於該電腦中係以上述取熱實驗擬合之地熱儲集層實驗系統,結合該管流模型放大至現地尺度模型,以供實際應用於現地之地熱系統進行評估。由於各個地點的地質構造、特性、物理與化學條件之複雜,位於不同地熱場址之地熱儲集層結構均不相同。建立合理的現地數值之該單井取熱模型,將有助於了解地底熱流現象與各種操作參數設定,進一步預測總地熱發電產能、最佳化地熱井之熱量取得。本發明結合的該 管流模型,係以宜蘭縣的清水地區之單井尺寸為基準,做成為現地的該單井取熱模型。現地取熱的該單井取熱模型之尺度放大,為依照目前清水現地鑿井之尺寸、深度及2008年前後之產能測試,以建立該單井取熱模型。繼而調整注入之流量以取熱最大化。由放大之數值模型結果,可預期現地取熱之取熱規模,藉此於評估成本時有一參考依據。該單井取熱模型之幾何設計,如第九圖所示,係以一中空的圓柱管(4)形成該管流模型,並於其底部部分填入一多孔隙介質(41),該多孔隙介質(41)係模擬儲集層之狀態,調整注入之流量將以取熱最大化規劃,以銜接下一步的取熱評估。 C. Use the geothermal reservoir experimental system to enlarge the scale and combine a pipe flow model to establish a single well heat extraction model, input a geothermal productivity data at different time points, establish the total thermal resistance of a geothermal well, and compare it The difference is used to modify the single-well heat extraction model. The computer is a geothermal reservoir experimental system fitted with the above-mentioned heat extraction experiment, combined with the pipe flow model to enlarge it to an on-site scale model, for the actual application of the on-site geothermal system for evaluation. Due to the complex geological structure, characteristics, physical and chemical conditions of each site, the geothermal reservoir structure at different geothermal sites is different. The establishment of a reasonable in-situ value of the single-well heat extraction model will help to understand the underground heat flow phenomenon and various operating parameter settings, further predict the total geothermal power generation capacity, and optimize the heat extraction of geothermal wells. The combination of the present invention The pipe flow model is based on the size of a single well in the Qingshui area of Yilan County, and is used as an on-site heat extraction model for the single well. The scale-up of the single-well heat extraction model for in-situ heat extraction is to establish the single-well heat extraction model in accordance with the current size and depth of the clean-water in-situ sinking well and the productivity test around 2008. Then adjust the injected flow rate to maximize heat extraction. Based on the results of the enlarged numerical model, the scale of the on-site heat extraction can be predicted, so as to have a reference basis when evaluating the cost. The geometric design of the single-well heat extraction model, as shown in the ninth figure, is to form the tube flow model with a hollow cylindrical tube (4), and fill the bottom part with a porous medium (41). The porous medium (41) simulates the state of the reservoir, and adjusts the injection flow rate to maximize the heat extraction plan to connect to the next heat extraction evaluation.

再透過該電腦,將西元2008年至2009年清水地區現地一地熱井的地熱產能資料輸入該單井取熱模型,從而獲得該地熱井之一舊總熱阻(以整體單井視為一系統)。繼而,將西元2017年清水地區該地熱井某一筆現地的地熱產能資料輸該入單井取熱模型而獲得一新總熱阻。該新、舊總熱阻之計算係分別以該地熱井的熱散失除以(井溫與環境溫度之差值)即可求得。比較該新、舊總熱阻之差異(新、舊總熱阻相減後除以2008至2009數值之百分比),藉以修正並更新該單井取熱模型,即可獲得新的該單井取熱模型,並驗證該地熱井隨時間之流量衰減狀況。不同時間點的該地熱產能資料係包含有該地熱井之深度、直徑、井底溫度、出口溫度、出口壓力及流量之數據。經由修正該單井取熱模型,藉以可預測未來不同管徑之產能測試結果,並可於該單井取熱模型中預測最佳之產能結果。利用該單井取熱模型之表面設定為一以現地產能測試擬合出之散熱面。分別改變入口流速、系統壓力,繼而觀察出口溫度及內壁溫度的變化,與已知之產能測試擬合,進一步獲得推估之井壁熱量損失,以獲得該地熱井之總熱阻,以求出在設定地層條件下之取熱量及效率。 Then through the computer, input the geothermal productivity data of an on-site geothermal well in Qingshui area from 2008 to 2009 into the single-well heat extraction model to obtain the old total thermal resistance of one of the geothermal wells (the entire single well is regarded as a system ). Then, input the on-site geothermal productivity data of the geothermal well in Qingshui area in 2017 into the single-well heat extraction model to obtain a new total thermal resistance. The calculation of the new and old total thermal resistance is obtained by dividing the heat loss of the geothermal well by (the difference between the well temperature and the ambient temperature). Compare the difference between the new and old total thermal resistances (the new and old total thermal resistances are subtracted and divided by the percentage of the value from 2008 to 2009) to modify and update the single-well heat extraction model to obtain the new single-well extraction model. Thermal model and verify the flow attenuation of the geothermal well over time. The geothermal productivity data at different time points includes data on the depth, diameter, bottom hole temperature, outlet temperature, outlet pressure and flow rate of the geothermal well. By modifying the single-well heat extraction model, the future productivity test results of different pipe diameters can be predicted, and the best productivity results can be predicted in the single-well heat extraction model. The surface of the single-well heat extraction model is set as a heat dissipation surface fitted by the on-site productivity test. Respectively change the inlet flow rate and system pressure, and then observe the outlet temperature and inner wall temperature changes to fit the known productivity test, and further obtain the estimated heat loss of the well wall to obtain the total thermal resistance of the geothermal well to obtain Heat extraction and efficiency under set formation conditions.

D.利用一最佳化方法使該單井取熱模型計算最佳化取熱量。係以該最佳化方法計算出在已知一地熱井深度及岩層孔隙狀態下,最適合之該地熱 井注入流量,以獲得流經該地熱井後可擷取之最大取熱量,同時達到最佳之出口溫度範圍。僅需針對初始模組進行最佳化設計,即可獲得一最佳化之模組,同時獲得相對之最佳化操作參數。所使用之該最佳化方法,透過最佳化過程重複以一相似產能測試模型模擬以求出最佳之設計。以最佳化模型工作條件及設計參數。所使用之最佳化方法係為簡易共軛梯度法(Simplified Conjugated Gradient Method,SCGM),該簡易共軛梯度法於計算目標函數時,將有助敏感性分析。先對每個設計參數進行初始猜測,其次在疊代過程中的共軛梯度係數和搜尋方向進行評估,依此過程不斷更新設計參數。當目標函數達到設計要求,最佳化過程完成。其主要計算公式如下所示:

Figure 107133223-A0305-02-0014-11
D. Use an optimization method to calculate the optimal heat extraction of the single well heat extraction model. The optimization method is used to calculate the most suitable injection flow rate of a geothermal well under the known depth and pore state of the formation, so as to obtain the maximum heat extraction that can be extracted after flowing through the geothermal well, and at the same time achieve the maximum The best outlet temperature range. Only need to optimize the design for the initial module, you can obtain an optimized module, and at the same time obtain relatively optimized operating parameters. The optimization method used repetitively simulates with a similar capacity test model through the optimization process to find the best design. To optimize model working conditions and design parameters. The optimization method used is the Simplified Conjugated Gradient Method (SCGM), which will help sensitivity analysis when calculating the objective function. First, make an initial guess for each design parameter, and then evaluate the conjugate gradient coefficient and search direction in the iterative process, and continuously update the design parameters according to this process. When the objective function meets the design requirements, the optimization process is completed. The main calculation formula is as follows:
Figure 107133223-A0305-02-0014-11

其中a k 是設計參數,β k 是疊代搜尋的步距,ξ k 是疊代搜尋的方向。 疊代搜尋的方向為線性組合的最速下降方向,與目標函數的梯度有關,其計算公式如下所示:

Figure 107133223-A0305-02-0014-12
Where a k is the design parameter, β k is the step distance of the iterative search, and ξ k is the direction of the iterative search. The direction of the iterative search is the fastest descent direction of the linear combination, which is related to the gradient of the objective function. The calculation formula is as follows:
Figure 107133223-A0305-02-0014-12

其中J是目標函數,r是共軛梯度係數。 Where J is the objective function and r is the conjugate gradient coefficient.

共軛梯度係數計算公式如下:

Figure 107133223-A0305-02-0014-13
The formula for calculating the conjugate gradient coefficient is as follows:
Figure 107133223-A0305-02-0014-13

其中,該步距β k 可以假設為一個固定值,β k =C,k=1,2...,nAmong them, the step distance β k can be assumed to be a fixed value, β k =C, k =1, 2..., n .

其中,C值的大小係根據所設定之最佳化問題而決定。簡易共軛梯度法的步驟如下。 Among them, the size of the C value is determined according to the optimization problem set. The steps of the simple conjugate gradient method are as follows.

a.定義設計參數a k k=1,2...,na. Define the design parameters a k , k =1, 2..., n .

b.使用多重物理量軟體計算目標函數J,當目標函數達到設計要求,該求解過程將終止,否則跳到步驟c。 b. Use multiple physical quantity software to calculate the objective function J. When the objective function meets the design requirements, the solution process will be terminated, otherwise skip to step c.

c.執行數值敏感度分析,首先給一個△a k 擾動值。然後計算目標函數的改變所得到的比值△J,接下來可以直接計算梯度函數在各個設計參數的數值微分如下所示:

Figure 107133223-A0305-02-0015-14
c. Perform numerical sensitivity analysis, first give a perturbation value of △ a k. Then calculate the ratio △ J obtained by the change of the objective function, and then directly calculate the numerical differentiation of the gradient function in each design parameter as shown below:
Figure 107133223-A0305-02-0015-14

利用上述計算公式(六)、(七)及(八)計算各個設計參數a k k=1,2,…,n之共軛梯度係數r和共軛梯度搜尋方向ξ k Use the above calculation formulas (6), (7) and (8) to calculate the conjugate gradient coefficient r and the conjugate gradient search direction ξ k of each design parameter a k , k =1, 2, ..., n.

d.對於所有設計參數給予步距β k k=1,2,…,nd. Give steps β k for all design parameters, k =1, 2, ..., n .

e.使用計算公式(六)更新下一個疊代時的所有設計參數,然後回到步驟b。 e. Use the calculation formula (6) to update all the design parameters of the next iteration, and then return to step b.

待數值結果得到最佳化後,利用數值模擬建立新的該單井取熱模型,再根據新的該單井取熱模型進行最佳化操作條件之熱交換分析,以計算出最佳化取熱量。 After the numerical results are optimized, use numerical simulation to establish a new single-well heat extraction model, and then perform heat exchange analysis of optimized operating conditions based on the new single-well heat extraction model to calculate the optimal Heat.

綜合上述實施例之說明,當可充分瞭解本發明之操作、使用及本發明產生之功效,惟以上所述實施例僅係為本發明之較佳實施例,當不能以此限定本發明實施之範圍,即依本發明申請專利範圍及發明說明內容所作簡單的等效變化與修飾,皆屬本發明涵蓋之範圍內。 Based on the description of the above embodiments, when one can fully understand the operation and use of the present invention and the effects of the present invention, but the above embodiments are only the preferred embodiments of the present invention, and the implementation of the present invention cannot be limited by this. The scope, that is, simple equivalent changes and modifications made according to the scope of the patent application of the present invention and the content of the description of the invention, are all within the scope of the present invention.

Claims (8)

一種地熱井產能預估方法,包含有:建立一地熱儲集層實驗系統,經由取熱實驗藉以獲得一取熱結果,該地熱儲集層實驗系統係藉由一高壓測試管路所形成之一測試段,藉以模擬一工作流體流經一儲集層之該取熱結果;利用該取熱結果擬合一孔隙取熱模型,完成於孔隙及裂隙條件下之一模擬物理特性,建立一地熱取熱模型,係以該地熱儲集層實驗系統經由該取熱結果,再依照該測試段以等比例,利用一電腦以電腦模擬該工作流體於該儲集層內之取熱現象,並獲得一模擬結果,比較該模擬結果與該取熱結果之差異性;利用該地熱儲集層實驗系統放大尺度,並結合一管流模型模擬建立一單井取熱模型,輸入不同時間點的一地熱產能資料,建立一地熱井之總熱阻,並比較其差異性,藉以修正該單井取熱模型,於該電腦中以該地熱儲集層實驗系統,結合該管流模型放大至現地尺度模型,以形成該單井取熱模型,藉以供實際應用於現地之地熱系統進行評估;利用一最佳化方法使該單井取熱模型計算最佳化取熱量,利用該最佳化方法計算出在已知地熱井深度及岩層孔隙狀態下,及最適合之地熱井注入流量,以獲得流經地熱井後可擷取之最大取熱量。 A method for predicting the productivity of geothermal wells, including: establishing a geothermal reservoir experimental system, and obtaining a heat extraction result through heat extraction experiments. The geothermal reservoir experimental system is formed by a high-pressure test pipeline. The test section is used to simulate the heat extraction result of a working fluid flowing through a reservoir; use the heat extraction result to fit a pore heat extraction model to complete a simulated physical characteristic under pore and fracture conditions, and establish a geothermal extraction The thermal model is based on the geothermal reservoir experimental system through the heat extraction results, and then according to the test section in equal proportions, using a computer to simulate the heat extraction phenomenon of the working fluid in the reservoir, and obtain a Simulation results, compare the difference between the simulation results and the heat extraction results; use the geothermal reservoir experimental system to enlarge the scale, and combine a pipe flow model to simulate a single well heat extraction model, and input a geothermal productivity at different time points Data, establish the total thermal resistance of a geothermal well, and compare its differences, so as to modify the single-well heat extraction model, use the geothermal reservoir experimental system in the computer, and combine the pipe flow model to enlarge it to a local scale model. In order to form the single-well heat extraction model, it can be used to evaluate the geothermal system that is actually applied in the field; an optimization method is used to optimize the single-well heat extraction model to calculate the optimal heat extraction, and the optimization method is used to calculate the Knowing the depth of the geothermal well and the pore state of the formation, and the most suitable injection flow rate of the geothermal well, to obtain the maximum heat extraction that can be extracted after flowing through the geothermal well. 如申請專利範圍第1項所述地熱井產能預估方法,其中,該取熱結果包含於不同之介質粒徑、壓力、流量、孔隙率、層流狀態或流速下,該工作流體的實驗物理特性之變化。 For example, the method for predicting the productivity of geothermal wells described in the scope of the patent application, wherein the heat extraction results include the experimental physics of the working fluid under different medium particle size, pressure, flow rate, porosity, laminar flow state or flow velocity. Changes in characteristics. 如申請專利範圍第2項所述地熱井產能預估方法,其中,該實驗物理特性包含熱交換效率、熱對流係數、熱分散性、取熱量其中之一或其任意組合。 For example, the method for predicting the productivity of geothermal wells described in item 2 of the scope of patent application, wherein the experimental physical characteristics include one of heat exchange efficiency, heat convection coefficient, heat dispersion, heat extraction, or any combination thereof. 如申請專利範圍第1項所述地熱井產能預估方法,其中,該模擬物理特性係包含熱分散性、熱擴散性、有效熱傳導係數、有效比熱、縱向熱分散性、橫向熱分散性其中之一或其任意組合。 For example, the method for predicting the productivity of geothermal wells described in the scope of the patent application, wherein the simulated physical properties include thermal dispersibility, thermal diffusivity, effective thermal conductivity, effective specific heat, vertical thermal dispersibility, and lateral thermal dispersibility. One or any combination thereof. 如申請專利範圍第1項所述地熱井產能預估方法,其中,以該取熱結果提供該電腦中之該孔隙取熱模型擬合出在各種不同壓力與流量條件下之該熱分散性,並與取熱實驗過程所量測的取熱量與入出口溫差進行比較其差異性。 For example, the method for predicting the productivity of geothermal wells described in the scope of the patent application, wherein the heat extraction result is used to provide the pore heat extraction model in the computer to fit the heat dispersion under various pressure and flow conditions, And compare the difference with the heat extraction and the temperature difference between the inlet and outlet measured during the heat extraction experiment. 如申請專利範圍第1項所述地熱井產能預估方法,其中,將時間在前的任一已知地熱井之該地熱產能資料輸入該單井取熱模型,而獲得該已知地熱井之一舊總熱阻,再將時間在後的該地熱產能資料輸入該單井取熱模型,而獲得該已知地熱井的一新總熱阻,比較該新、舊總熱阻之差異性,藉以修正並更新該單井取熱模型,以獲得新的該單井取熱模型,並驗證該已知地熱井隨時間之流量衰減狀況。 For example, the method for predicting the productivity of geothermal wells described in the scope of the patent application, wherein the geothermal productivity data of any known geothermal well before the time is input into the single-well heat extraction model to obtain the known geothermal well An old total thermal resistance, and then input the time later the geothermal productivity data into the single-well heat extraction model to obtain a new total thermal resistance of the known geothermal well, and compare the difference between the new and the old total thermal resistance, In this way, the single-well heat extraction model is revised and updated to obtain a new single-well heat extraction model and to verify the flow attenuation of the known geothermal well over time. 如申請專利範圍第6項所述地熱井產能預估方法,其中,該地熱產能資料係包含有地熱井之深度、直徑、井底溫度、出口溫度、出口壓力及流量之數據。 For example, the geothermal well productivity estimation method described in item 6 of the scope of patent application, wherein the geothermal productivity data includes data on the depth, diameter, bottom hole temperature, outlet temperature, outlet pressure and flow rate of the geothermal well. 如申請專利範圍第1項所述地熱井產能預估方法,其中,藉由該電腦擬合出以一布林克曼模型與一熱傳模組共同建立之該孔隙取熱模型做為基礎之該地熱取熱模型,又該最佳化方法係為簡易共軛梯度法。 For example, the method for predicting the productivity of geothermal wells described in the scope of the patent application, wherein the computer is used to fit the pore heat extraction model jointly established by a Brinkman model and a heat transfer module as the basis The geothermal heat extraction model, and the optimization method is a simple conjugate gradient method.
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