TW509786B - Micro-force measurement device with all coil magnetic-force balanced structure - Google Patents
Micro-force measurement device with all coil magnetic-force balanced structure Download PDFInfo
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509786 五、發明說明(l) 發明背景 本發明係有關於一種精密量測裝置,尤其是一種線圈 磁浮式微力量測裝置,其利用電路調整所需的量測範圍及 解析度’以校正及量測微力,其中,量測範圍及解析度是 與電路的電流呈正比關係。 整合微力技術與奈米計量(例如原子力顯微技術 (atomic force microscopic technique)),即可量測奈509786 V. Description of the invention (l) Background of the invention The present invention relates to a precision measurement device, especially a coil magnetic floating type micro-force measurement device, which uses a circuit to adjust the measurement range and resolution required to correct and measure Micro force measurement, in which the measurement range and resolution are directly proportional to the current of the circuit. Integrate micro-force technology with nanometer metrology (such as atomic force microscopic technique) to measure nanometers
米結構(narostructure)之表面特徵與機械性質,例如表 面原子分布、微硬度、微觀楊式係數等。其技術關鍵在方 1針(Pr〇be)之輸出力量、或微機電(MEMS)製程的微應變 計〇n1Crostrainometer)等量測儀器,必須是定量的、 控的’才能將微觀機械性質轉拖氧 在至i mN之間,必的數據’此力量多 但目前並無適當儀器來達成此依目賴/。他精密裝置來校正, 因此’本發明之一目的係 測裝置,其利用電路調整所:二—種線圈磁浮式微力I 正及量測微力’其中,量測;圍=範圍及解析度,以杉 呈正比關係。 及解析度是與電路的電济 本發明之另一目的係提佴一 置,其應用電磁學原理,在量測微力;磁浮式微力量測装The surface features and mechanical properties of the rice structure (narostructure), such as the surface atomic distribution, micro hardness, and micro Young's coefficient. The key to its technology lies in measuring instruments such as the output power of Pr0be, or microstrain gauges of the micro-electromechanical (MEMS) process, such as 0n1Crostrainometer, which must be quantitative and controlled in order to change the micromechanical properties. Oxygen is between 1 mN, and the necessary data is' there is more power, but currently there are no suitable instruments to achieve this. Other precision devices are used for calibration, so 'an object of the present invention is a measuring device, which uses a circuit to adjust the place: two kinds of coil magnetic levitation type micro force I positive and measuring micro force', where measurement; range = range and resolution, to Sugi is directly proportional. And the resolution is the power of the circuit. Another object of the present invention is to improve the application of electromagnetic principles in measuring micro-force;
本發明係提供一種線圈礙 ••一徑向磁場產生I f /式倣力量剛裝t 節阳•、丨Λ 义置’用以產生一你1置’該裳 械、溫度等壞境因素降至最低。 t 可將材料、機 包括 ——用以甚 %夏,’ 重線圈,用以在導電時配合屋生—徑向礤 口5亥徑向磁場,以:努’ μ產生 反饋The present invention provides a coil obstruction •• A radial magnetic field generates I f / type imitation force just installed t section Yang •, 丨 Λ is used to generate a “you 1 set”, such as clothing, temperature and other environmental factors. To the lowest. t can include materials and machines-for very high summer, ’heavy coils, used to match the housing when conducting-radial radial port 5H radial magnetic field, to: feedback
509786 五 、發明說明(2) 浮力;一承力機構,用以承受待測微力;一組電容式位移 感測器,用以量測該待測微力所產生之一相對於該承力機 構原點位置之位移及據以調整在該反饋磁浮力及該待測微 力相等時所具有之一反饋電流;一控制電路,用以根據該 反饋電流來量測及校正該待測微力。 戈口上返,利用置測範圍及解析度與在該控制電路内所 提供至該舉重線圈之電流呈正比關係,使用本發明可達到 以電路調整所需的量測範圍及解析度,以校正及量測微力 的目的。又,在量測微力時,利用本發明也能將材料、 ^、溫度等環境影響因素降至最低。例如,在原子力 楝針或微應變針中,可先利用本發明來校正其應變力逝1 力的關係,將微力的控制與量測傳遞至量測程序 ^二 得最佳的量測效果。 Μ獲 圖示之簡單說明 為讓本發明之上述及直夕 而易見,下文特兴一 ϊ ΐ二 與優點能更顯 、牛 車乂佳貫施例,並配合所附圖式, 細說明如下: 1 Ή 口八’作詳 圖顯示一本發明之微力量測裝置示意圖; 示Γ圖中之控制電路方塊圖;及 “圖顯不以圖中之徑向磁場產生裝置剖 [符號說明] 1〜徑向磁場產生裝置509786 V. Description of the invention (2) Buoyancy; a load-bearing mechanism to withstand the micro-force to be measured; a set of capacitive displacement sensors for measuring one of the micro-forces to be measured relative to the original of the force-bearing mechanism The displacement of the point position is used to adjust a feedback current when the feedback magnetic buoyancy and the micro force to be measured are equal; a control circuit is used to measure and correct the micro force to be measured according to the feedback current. Going back, using the measurement range and resolution is proportional to the current provided to the weight coil in the control circuit, the invention can achieve the measurement range and resolution required by the circuit adjustment to correct and The purpose of measuring micro force. In addition, when measuring micro-force, the present invention can also minimize environmental influence factors such as materials, temperature, and temperature. For example, in an atomic force pin or micro-strain needle, the present invention can be used to correct the relationship between the strain force and the force, and the control and measurement of the micro-force can be transferred to the measurement program. Second, the best measurement effect can be obtained. In order to make the above and the present invention easy to see, a simple illustration is shown below. Special features, advantages, and advantages can be more clearly shown below. : 1 Ή 口 八 'detailed drawing shows a schematic diagram of the micro-force measuring device of the present invention; shows the block diagram of the control circuit in the figure; and "the figure shows the radial magnetic field generating device in the figure [symbol description] 1 ~ Radial magnetic field generator
/«6/ «6
2〜舉重線圈 3〜支撐機構 4〜撓性彈片 5〜承力機構 6〜電容式位移感測器 7〜控制電路 8〜驅動電路 9〜類比/數位電路 1 0〜微處理器 11〜電流供應器 1 2〜精密串接電阻 1 3〜線圈支撐機構 1 4〜線圈組 車交佳實施例之詳細說明 第1圖係本發明之微力量測裝罟 本穿菩七紅 J表置不意圖。在第1圖中 支f 裝置⑴、-舉重線圈⑴、2 ~ weight lifting coil 3 ~ support mechanism 4 ~ flexible spring 5 ~ force bearing mechanism 6 ~ capacitive displacement sensor 7 ~ control circuit 8 ~ drive circuit 9 ~ analog / digital circuit 1 0 ~ microprocessor 11 ~ current supply Device 1 2 ~ precision series resistor 1 3 ~ coil supporting mechanism 1 4 ~ detailed description of the best embodiment of the coil assembly. Figure 1 is the micro-force measuring device of the present invention. In the first figure, the f-device-, -weight coil ⑴,
動電谷式位移感測器(6)及一控制電路(7)。如第i圖所 =,承力機構(5)經由撓性彈片(4)與支撐機構(3)連接, 撓性彈片(5 )組合具易撓性,使承力機構(5 )僅做上下 向直線位移,不致產生側向位移。承力機構(5)兩邊緣以 差動電容式位移感測器(6)監測其位置,下方則連接環狀 的舉重線圈(2 )。舉重線圈(2 )懸吊於徑向磁場產生裝置A dynamic valley-type displacement sensor (6) and a control circuit (7). As shown in Figure i, the load bearing mechanism (5) is connected to the support mechanism (3) via a flexible spring sheet (4). The combination of the flexible spring sheet (5) is easy to make the load bearing mechanism (5) only move up and down. Displace in a straight line without causing lateral displacement. The two sides of the load-bearing mechanism (5) monitor its position with a differential capacitive displacement sensor (6), and a ring-shaped weight lifting coil (2) is connected below. Weightlifting coils (2) are suspended from a radial magnetic field generating device
0729-7241TWF;07900013;Sue.p t d 第7頁 509786 、發明說明(4) (1)之凹槽内上方,徑向磁場產生梦 之移動範圍内,提供一徑向分布磁η:重線圈⑺ 電容式位移感測器⑹、舉重線圈^制電路⑺負責 置⑴之信號讀取與線路驅動(2)及編場產生裝 -第2圖係第1圖之控制電路⑺之示意圖。 。,處理器⑽須先發出信號給驅動電路⑻以輸出驅 巧至電容式位移感測器(6a、6b)來進行量測。如 ΐ 待量測之微力P由上往下施加於承力機構⑸時, 機構(5)與其舉重線圈(2) 一起向下位移’此位移被電 :式位移感測ll(6a、6b)量測得到,而輸出一非零正比電 I至控制電路(7)。此時,在控制電路(7)中, j 〇 ),由微處理器(1 〇)計算出一反饋電流值,再令電流源 〔la)輸出此反饋電流至舉重線圈(2)。另一電流源(iib) 則提供固定電流予徑向磁場產生裝置(1),使其產生固定 之獲向磁場,環繞於舉重線圈内的反饋電流與此固定磁場 產生電磁作用力(勞倫茲力),此作用力的方向向上,使得 ,力機構(5 )與舉重線圈(2 )被一起向上舉起,而減小位移 里。第二次的位移量又被電容式位移感測器(6a、6b)檢 知’而再次修正反饋電流量,如此一再反覆進行,直至位 移回復為零,此時撓性彈片(5 )回至未受p施加前的力學狀 $ ’因此微力P等於線圈間的磁力,即可藉由反饋電流值 $測微力。此電流值由精密串接電阻(丨2 )量得電壓,再經 由類比/數位電路(9)輸入微處理器(1〇),計算且顯示微力0729-7241TWF; 07900013; Sue.ptd Page 7 509786, Description of Invention (4) (1) Above the groove, the radial magnetic field produces a range of dream movement, providing a radially distributed magnetic η: heavy coil ⑺ capacitance Displacement sensor ⑹, weight lifting coil ^ control circuit ⑺ is responsible for the signal reading and line drive (2) and field generating device-Figure 2 is a schematic diagram of the control circuit of Figure 1. . The processor must first send a signal to the drive circuit to output the drive to the capacitive displacement sensor (6a, 6b) for measurement. For example, when the micro-force P to be measured is applied to the load bearing mechanism from top to bottom, the mechanism (5) and its weight lifting coil (2) are displaced downward together. This displacement is electrically: type displacement sensing 11 (6a, 6b) Measured, and output a non-zero proportional electric I to the control circuit (7). At this time, in the control circuit (7), j0), a microprocessor (10) calculates a feedback current value, and then causes the current source [la] to output the feedback current to the weight lifting coil (2). The other current source (iib) provides a fixed current to the radial magnetic field generating device (1), so that it generates a fixed directional magnetic field, and the feedback current that surrounds the weightlifting coil generates an electromagnetic force with this fixed magnetic field (Lorentz Force), the direction of the acting force is upward, so that the force mechanism (5) and the weight lifting coil (2) are lifted upward together to reduce the displacement. The second amount of displacement was detected by the capacitive displacement sensor (6a, 6b), and the feedback current was corrected again, and iteratively repeated until the displacement returned to zero. At this time, the flexible spring (5) returned to Before the application of p, the micro force P is equal to the magnetic force between the coils, and the micro force can be measured by the feedback current value $. This current value is measured by the precision series resistor (丨 2), and then the analog / digital circuit (9) is input to the microprocessor (10), and the micro force is calculated and displayed.
juy/δ〇 五 發明說明(5) 之量測值。 由電磁學原理推導’徑向磁場與舉重線圈 ^為匕=πΟηΙΒ,其中D為舉重線圈(2)平均直押 為舉重線圈(2)上之電流、B:徑向= 磁ίβΐΓ/(1)所產生之徑向平均磁場。如第3圖所示,彳^ 磁%B疋由四組環形線圈(丨4 )的磁場向量合成 二向 (";Μη:^ί〇η) ° (Λ '線圈於該徑向磁場產生裝置⑴之環形凹样 (未顯不)内。在環形線圈(14)的電流方向如圖槽 ΐ,;向磁場值可由公式B = 計算獲就所 侍’厂中丫是-比例常數(由理論精確計算,介於12蛊 :Λ’Λ:線圈設計有關)、n’是環形線圈(⑷之租數: m圈(⑷上的電流值、&是上下兩線圈中 二 =。代入B後,得磁力( Mnmw/ t 1 饋平衡後之磁力匕與待測外力p相等, 口反 ;r c= rWww:〇rV^ 吊數,/、早位為N/A。C只含有電流(I, 與材料性質無關,可直接由公十呌# /、负度里⑶及㈧, 旦沪進楂、腾石士壯班 式计异,或以標準砝碼將力 里‘旱傳遞至本叙置、再轉換得出C 〇 本裝置因為未使用磁性材料為磁場源有別於 電子天平,故無磁性材料之、、w _ 、 叙之 反饋使承力機構⑸之位m效應與遲緩效應;又因以 片(4)機械應變之影響可以勿 便行里』又撓[生弹 常數C與電流丨,成正比:本略梦。上上述公式可知,校正 故本裝置可因應待測微力之大小juy / δ〇 5 Invention description (5) Measured value. The principle of electromagnetic field is derived from the principle of radial magnetic field and weight lifting coil ^ = πΟηΙΒ, where D is the average weight of the weight lifting coil (2) and the current on the weight lifting coil (2), B: radial = magnetic ίβΐΓ / (1) The radial average magnetic field produced. As shown in Figure 3, 彳 ^ 磁 % B 疋 is synthesized from the magnetic field vectors of four sets of toroidal coils (丨 4) to form a two-way (" Μη: ^ ί〇η) ° (Λ 'coil is generated in the radial magnetic field Inside the ring-shaped concave sample (not shown) of the device 。. The direction of the current in the toroidal coil (14) is shown in Figure ΐ. The value of the magnetic field can be calculated by the formula B = Theoretical and accurate calculations are between 12 蛊: Λ'Λ: coil design related, n 'is a toroidal coil (the number of rents of 圈: m turns (the current value on ⑷, & is the second and upper two coils =. Substitute B) Then, the magnetic force (Mnmw / t 1 after the feed balance is equal to the external force p to be measured, the mouth is opposite; rc = rWww: 〇rV ^ hanging number, /, the early position is N / A. C only contains the current (I It has nothing to do with the nature of the material. It can be directly calculated from the public ten 呌 # /, negative degree ⑶ and ㈧, Danhu Jinha, Tengshi Shizhuang class calculation, or use standard weights to pass Lili drought to the present, Reconverted to C. This device is different from electronic balances because no magnetic material is used as the magnetic field source. Therefore, the feedback of the magnetic material, w_, and Syria makes the position of the load bearing mechanism m effective. It should be related to the retardation effect; and because of the influence of the mechanical strain of the sheet (4), you can do it again and again [the spring constant C is proportional to the current 丨, which is proportional to this dream. The above formula shows that the device can According to the magnitude of the micro force to be measured
509786 五 發明說明(6) 而改變I ,以調整裝置至最適宜量測範圍。本裂置之特性 為線性、可由電路調整量測範圍與解析度、無迴滯 (hysteresis)、不需溫度補償、可直接追溯至基本量(電 流、長度)。 以一個設計例說明本發明之效能,當丨.2 7、D二 5:5 cm、n 二 20、η’ = 20 0、I,:= 〇· i a、a = i cm,可 得C為70 //N/A,若舉重線圈(2)的電流供應以—常用之電 流源:輸出範圍二0〜2 A、解析度=〇 · ;[ m a,則可得本 校正範圍為0〜140#N、解析度為7 nN。若欲提高校 乾圍為10倍:〇〜1400/zN,可提高電流Γ至! Α,直解 :度則,成70 nN。惟此例僅為本發明之一較佳實施例而 =非用來限定本發明實施之範圍,若依 ^圍所作的均等變化與修飾1為本發明專利範= 下施力力平衡為基礎,待測力由上往 平衡。電磁力為勞倫兹☆,以二力由下往上 圈’通電流(I,)產生局部的徑向磁;:计:的環形線 通電流(I ),與徑向磁場作用每以一J固環形線圈 結構以撓性彈片纟 向上的勞倫茲力。承力 其位移,當Ui;時並::差動式電容位移感剛器二 電磁力與",成舆待,力達到平銜,此; 力量’而此力量隨㈣::;月二輸出10心下的磁浮 __ 的變化為線性、可調整解 509786 五、發明說明(7) 析度與範圍,故適用於精密校正。本發明未使用磁性材 料,避免了解析度不足、隨溫度變異等缺失,與電子天平 之原理與結構皆不同。 雖然本發明已以一較佳實施例揭露如上,然其並非用 以限定本發明,任何熟知此技術之人士,在不脫離本發明 之精神及範圍内,當可做更動與潤飾,因此本發明之保護 範圍當視後附之申請專利範圍所界定者為準。509786 V Description of the invention (6) and change I to adjust the device to the most suitable measurement range. The characteristics of this split are linear, the measurement range and resolution can be adjusted by the circuit, no hysteresis, no temperature compensation is required, and it can be directly traced back to the basic quantity (current, length). A design example is used to illustrate the effectiveness of the present invention. When .7, D2 5: 5 cm, n2 20, η '= 20 0, I ,: = 〇 · ia, a = i cm, we can get C as 70 // N / A, if the current supply of weightlifting coil (2) is-commonly used current source: output range 2 0 ~ 2 A, resolution = 0 ·; [ma, then the correction range is 0 ~ 140 #N, resolution is 7 nN. If you want to increase the school circumference by 10 times: 0 ~ 1400 / zN, you can increase the current Γ to! Α, direct solution: the rule is 70 nN. However, this example is only a preferred embodiment of the present invention and is not intended to limit the scope of implementation of the present invention. If equal changes and modifications are made in accordance with the present invention, 1 is the patent scope of the present invention. The forces are balanced from top to bottom. The electromagnetic force is Lorentz ☆, the current (I,) is generated by two forces from the bottom to the upper circle to generate local radial magnetism; The J-fixed toroidal coil structure uses a flexible spring to force the Lorentz force upward. Bearing force and its displacement, when Ui; and :: the electromagnetic force of the differential capacitive displacement rigidity device II and ", become public opinion, the force reaches the same level, this; the force ', and this force follows ::; The change of the magnetic levitation __ under the output of 10 cores is linear and adjustable. 509786 V. Description of the invention (7) The resolution and range are suitable for precision correction. The present invention does not use magnetic materials, avoids insufficient resolution, lack of variation with temperature, etc., and is different from the principle and structure of electronic balances. Although the present invention has been disclosed as above with a preferred embodiment, it is not intended to limit the present invention. Anyone who is familiar with this technology can make changes and decorations without departing from the spirit and scope of the present invention. The scope of protection shall be determined by the scope of the attached patent application.
0729-7241TWF;07900013;Sue.ptd 第11頁0729-7241TWF; 07900013; Sue.ptd Page 11
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Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI510768B (en) * | 2011-06-21 | 2015-12-01 | Ind Tech Res Inst | Force sensing device and force sensing system |
CN116839780A (en) * | 2023-07-06 | 2023-10-03 | 西安电子科技大学 | Weak electromagnetic force measuring device and method for wireless power transmission coupler |
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
TWI510768B (en) * | 2011-06-21 | 2015-12-01 | Ind Tech Res Inst | Force sensing device and force sensing system |
CN116839780A (en) * | 2023-07-06 | 2023-10-03 | 西安电子科技大学 | Weak electromagnetic force measuring device and method for wireless power transmission coupler |
CN116839780B (en) * | 2023-07-06 | 2024-04-23 | 西安电子科技大学 | Weak electromagnetic force measuring device and method for wireless power transmission coupler |
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