TWI703338B - Electric current sensor - Google Patents
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本發明是有關於一種感測器,且特別是有關於一種電流感測器。The present invention relates to a sensor, and particularly relates to a current sensor.
電流感測是工業自動化中不可或缺的元素之一。近年來,電流感測的需求從工業用途擴展至智能居家與智慧城市領域的消費者產品與應用。高準確度、快速反應、小體積、低功耗及可靠的品質成為新一代電流感測器所追求的目標。Current sensing is one of the indispensable elements in industrial automation. In recent years, the demand for current sensing has expanded from industrial use to consumer products and applications in the field of smart homes and smart cities. High accuracy, fast response, small size, low power consumption and reliable quality have become the goals pursued by the new generation of current sensors.
目前有多種方法可以量測導體中的電流。舉例而言,可利用分路電阻器(shunt resistor)藉由量測橫跨其之電壓差來推算出電流。然而,此電阻相量小,因此電流消耗高,而不適用於小型或可攜式裝置。此外,高電流會產生熱,而造成其他問題。There are many ways to measure the current in a conductor. For example, a shunt resistor can be used to calculate the current by measuring the voltage difference across it. However, this resistance has a small phasor and therefore high current consumption, which is not suitable for small or portable devices. In addition, high currents can generate heat and cause other problems.
本發明提供一種電流感測器,具有高敏感度、高準確度及低功耗。The invention provides a current sensor with high sensitivity, high accuracy and low power consumption.
本發明的一實施例提出一種電流感測器,包括一基板、一導線、一第一異向性磁電阻(anisotropic magnetoresistor, AMR)單元、一第二異向性磁電阻單元、一第三異向性磁電阻單元、一第四異向性磁電阻單元、一第一磁化方向設定元件及一第二磁化方向設定元件。導線具有一第一導電段與一第二導電段,其中第一導電段與第二導電段排列於一第一方向上,各自沿著一第二方向延伸,且分別配置於基板之相對的一第一端與一第二端下方。第一異向性磁電阻單元與第二異向性磁電阻單元配置於基板的第一端上方,且沿著第一方向排列。第三異向性磁電阻單元與第四異向性磁電阻單元配置於基板的第二端上方,且沿著第一方向的反方向排列。第一磁化方向設定元件用以設定第一異向性磁電阻單元與第二異向性磁電阻單元的磁化方向。第二磁化方向設定元件用以設定第三異向性磁電阻單元與第四異向性磁電阻單元的磁化方向。當一電流流經導線時,因感應於電流所產生的磁場,第一異向性磁電阻單元所產生的電阻值變化相反於第二異向性磁電阻單元所產生的電阻值變化,且第三異向性磁電阻單元所產生的電阻值變化相反於第四異向性磁電阻單元所產生的電阻值變化,且第一、第二、第三及第四異向性磁電阻單元電性連接成一惠斯登電橋,以輸出對應於第一、第二、第三及第四異向性磁電阻單元所產生的電阻值變化的電壓訊號。An embodiment of the present invention provides a current sensor that includes a substrate, a wire, a first anisotropic magnetoresistor (AMR) unit, a second anisotropic magnetoresistor, and a third anisotropic magnetoresistor. The directional magnetic resistance unit, a fourth anisotropic magnetic resistance unit, a first magnetization direction setting element, and a second magnetization direction setting element. The wire has a first conductive segment and a second conductive segment, wherein the first conductive segment and the second conductive segment are arranged in a first direction, each extend along a second direction, and are respectively disposed on an opposite side of the substrate Below the first end and a second end. The first anisotropic magnetic resistance unit and the second anisotropic magnetic resistance unit are disposed above the first end of the substrate and arranged along the first direction. The third anisotropic magnetoresistive unit and the fourth anisotropic magnetoresistive unit are disposed above the second end of the substrate and are arranged along the opposite direction of the first direction. The first magnetization direction setting element is used for setting the magnetization directions of the first anisotropic magnetoresistive unit and the second anisotropic magnetoresistive unit. The second magnetization direction setting element is used for setting the magnetization directions of the third anisotropic magnetic resistance unit and the fourth anisotropic magnetic resistance unit. When a current flows through the wire, due to the magnetic field generated by the current, the resistance change generated by the first anisotropic magnetoresistive unit is opposite to the resistance change generated by the second anisotropic magnetoresistive unit, and the first The resistance change produced by the three anisotropic magnetoresistive unit is opposite to the resistance change produced by the fourth anisotropic magnetoresistive unit, and the first, second, third and fourth anisotropic magnetoresistive units are electrically It is connected as a Wheatstone bridge to output a voltage signal corresponding to the resistance change generated by the first, second, third and fourth anisotropic magnetoresistive units.
在本發明的一實施例中,電流感測器更包括一運算器,電性連接至惠斯登電橋的一輸出端,其中第一磁化方向設定元件與第二磁化方向設定元件將第一、第二、第三及第四異向性磁電阻單元的磁化方向組合設定為一第一組合,以使惠斯登電橋之後輸出一第一電壓訊號,且第一磁化方向設定元件與第二磁化方向設定元件再將第一、第二、第三及第四異向性磁電阻單元的磁化方向組合設定為相反於第一組合的一第二組合,以使惠斯登電橋之後輸出一第二電壓訊號。運算器用以將第一電壓訊號與第二電壓訊號相減,以輸出一對應於電流所產生的磁場的大小的輸出電壓訊號。In an embodiment of the present invention, the current sensor further includes an arithmetic unit electrically connected to an output terminal of the Wheatstone bridge, wherein the first magnetization direction setting element and the second magnetization direction setting element connect the first The magnetization direction combination of the second, third, and fourth anisotropic magnetoresistive units is set to a first combination, so that the Wheatstone bridge outputs a first voltage signal, and the first magnetization direction setting element and the first combination The second magnetization direction setting element then sets the magnetization direction combination of the first, second, third and fourth anisotropic magnetoresistive units to a second combination opposite to the first combination, so that the Wheatstone bridge outputs A second voltage signal. The arithmetic unit is used for subtracting the first voltage signal and the second voltage signal to output an output voltage signal corresponding to the magnitude of the magnetic field generated by the current.
在本發明的一實施例中,運算器用以將第一電壓訊號與第二電壓訊號相加,以輸出一偏移電壓訊號。In an embodiment of the present invention, the arithmetic unit is used to add the first voltage signal and the second voltage signal to output an offset voltage signal.
在本發明的一實施例中,當電流流經導線時,電流在第一導電段中的流向相反於在第二導電段中的流向。In an embodiment of the present invention, when current flows through the wire, the direction of current flow in the first conductive section is opposite to the direction of current flow in the second conductive section.
在本發明的一實施例中,第一方向垂直於第二方向。In an embodiment of the present invention, the first direction is perpendicular to the second direction.
在本發明的一實施例中,電流流經第一導電段時在第一異向性磁電阻單元與第二異向性磁電阻單元處所產生的磁場在第一方向上的分量的方向相反於電流流經第二導電段時在第三異向性磁電阻單元與第四異向性磁電阻單元處所產生的磁場在第一方向上的分量的方向。In an embodiment of the present invention, when the current flows through the first conductive section, the direction of the component of the magnetic field generated at the first anisotropic magnetoresistance unit and the second anisotropic magnetoresistance unit in the first direction is opposite to The direction of the component in the first direction of the magnetic field generated at the third anisotropic magnetoresistance unit and the fourth anisotropic magnetoresistance unit when current flows through the second conductive section.
在本發明的一實施例中,惠斯登電橋對應於在第一方向上的外在磁場分量所輸出的電壓訊號為零,對應於在第二方向上的外在磁場分量所輸出的電壓訊號為零,且對應於在一第三方向上的外在磁場分量所輸出的電壓訊號為零,其中第三方向垂直於第一方向與第二方向。In an embodiment of the present invention, the Wheatstone bridge corresponding to the output voltage signal of the external magnetic field component in the first direction is zero, which corresponds to the voltage output of the external magnetic field component in the second direction The signal is zero, and the output voltage signal corresponding to the external magnetic field component in a third direction is zero, wherein the third direction is perpendicular to the first direction and the second direction.
在本發明的一實施例中,第一異向性磁電阻單元包括沿著第二方向的反方向依序排列的一第一異向性磁電阻與一第二異向性磁電阻,第二異向性磁電阻單元包括沿著第二方向的反方向依序排列的一第三異向性磁電阻與一第四異向性磁電阻,第三異向性磁電阻單元包括沿著第二方向的反方向依序排列的一第五異向性磁電阻與一第六異向性磁電阻,且第四異向性磁電阻單元包括沿著第二方向的反方向依序排列的一第七異向性磁電阻與一第八異向性磁電阻。In an embodiment of the present invention, the first anisotropic magnetoresistive unit includes a first anisotropic magnetoresistance and a second anisotropic magnetoresistance arranged in sequence along the opposite direction of the second direction, and the second The anisotropic magnetoresistive unit includes a third anisotropic magnetoresistance and a fourth anisotropic magnetoresistance that are arranged in sequence along the direction opposite to the second direction. The third anisotropic magnetoresistance unit includes A fifth anisotropic magnetoresistance and a sixth anisotropic magnetoresistance are arranged in sequence in a direction opposite to the direction, and the fourth anisotropic magnetoresistance unit includes a first Seven anisotropic magnetoresistance and an eighth anisotropic magnetoresistance.
在本發明的一實施例中,在一第一時間,第一磁化方向設定元件將第一異向性磁電阻與第三異向性磁電阻的磁化方向設定為第二方向的反方向,且將第二異向性磁電阻與第四異向性磁電阻的磁化方向設定為第二方向。在第一時間,第二磁化方向設定元件將第五異向性磁電阻與第七異向性磁電阻的磁化方向設定為第二方向的反方向,且將第六異向性磁電阻與第八異向性磁電阻的磁化方向設定為第二方向。在一第二時間,第一磁化方向設定元件將第一異向性磁電阻與第三異向性磁電阻的磁化方向設定為第二方向,且將第二異向性磁電阻與第四異向性磁電阻的磁化方向設定為第二方向的反方向。在第二時間,第二磁化方向設定元件將第五異向性磁電阻與第七異向性磁電阻的磁化方向設定為第二方向,且將第六異向性磁電阻與第八異向性磁電阻的磁化方向設定為第二方向的反方向。In an embodiment of the present invention, at a first time, the first magnetization direction setting element sets the magnetization directions of the first anisotropic magnetic resistance and the third anisotropic magnetic resistance to the opposite direction of the second direction, and The magnetization directions of the second anisotropic magnetic resistance and the fourth anisotropic magnetic resistance are set to the second direction. At the first time, the second magnetization direction setting element sets the magnetization directions of the fifth anisotropic magnetic resistance and the seventh anisotropic magnetic resistance to the opposite direction of the second direction, and sets the sixth anisotropic magnetic resistance and the first The magnetization direction of the eight-anisotropic magnetoresistance is set to the second direction. At a second time, the first magnetization direction setting element sets the magnetization directions of the first anisotropic magnetoresistance and the third anisotropic magnetoresistance to the second direction, and sets the second anisotropic magnetoresistance to the fourth anisotropy The magnetization direction of the directional magnetoresistance is set to the opposite direction of the second direction. At the second time, the second magnetization direction setting element sets the magnetization directions of the fifth anisotropic magnetoresistance and the seventh anisotropic magnetoresistor to the second direction, and sets the sixth anisotropic magnetoresistance to the eighth anisotropy The magnetization direction of the magnetic resistance is set to the opposite direction of the second direction.
在本發明的一實施例中,第一磁化方向設定元件與第二磁化方向設定元件為導電片、導電線圈、導線或導體。In an embodiment of the present invention, the first magnetization direction setting element and the second magnetization direction setting element are conductive sheets, conductive coils, wires or conductors.
在本發明的實施例的電流感測器中,由於採用了異向性磁電阻單元連接成惠斯登電橋來感測導線中的電流所產生的磁場,因此對電流的感測具有高敏感度與高準確度。此外,由於本發明的實施例的電流感測器是利用感測電流所產生的磁場的方式來反推電流的大小,而異向性磁電阻單元不會直接接觸到電流,因此可以具有較低的功耗。In the current sensor of the embodiment of the present invention, since the anisotropic magnetoresistance unit is connected to form a Wheatstone bridge to sense the magnetic field generated by the current in the wire, it is highly sensitive to current sensing Degree and high accuracy. In addition, because the current sensor of the embodiment of the present invention uses the magnetic field generated by the sensing current to reverse the magnitude of the current, the anisotropic magnetoresistive unit does not directly contact the current, so it can have a lower Power consumption.
為讓本發明的上述特徵和優點能更明顯易懂,下文特舉實施例,並配合所附圖式作詳細說明如下。In order to make the above-mentioned features and advantages of the present invention more comprehensible, the following specific embodiments are described in detail in conjunction with the accompanying drawings.
圖1是本發明的一實施例的一種電流感測器的上視示意圖,而圖2是圖1的電流感測器沿著A-A線的剖面示意圖。請參照圖1與圖2,本實施例的電流感測器100包括一基板210、一導線110、一第一異向性磁電阻單元222、一第二異向性磁電阻單元224、一第三異向性磁電阻單元226、一第四異向性磁電阻單元228、一第一磁化方向設定元件M1及一第二磁化方向設定元件M2。導線110具有一第一導電段C1與一第二導電段C2,其中第一導電段C1與第二導電段C2排列於一第一方向D1上,各自沿著一第二方向D2延伸,且分別配置於基板210之相對的一第一端212與一第二端214下方。電流感測器100所存在的空間可以由彼此不同的第一方向D1、第二方向D2及第三方向D3所建構,在本實施例中,第一方向D1、第二方向D2及第三方向D3可以彼此互相垂直。然而,在其他實施例中,第一方向D1、第二方向D2及第三方向D3也可以是彼此不垂直且不相同。1 is a schematic top view of a current sensor according to an embodiment of the present invention, and FIG. 2 is a schematic cross-sectional view of the current sensor of FIG. 1 along the line A-A. 1 and 2, the
第一異向性磁電阻單元222與第二異向性磁電阻單元224配置於基板210的第一端212上方,且沿著第一方向D1排列。第三異向性磁電阻單元226與第四異向性磁電阻單元228配置於基板210的第二端214上方,且沿著第一方向D1的反方向排列。上述基板210的第一端212下方至基板210的第一端212上方的方向即為第三方向D3。The first anisotropic
第一磁化方向設定元件M1用以設定第一異向性磁電阻單元222與第二異向性磁電阻單元224的磁化方向。第二磁化方向設定元件M2用以設定第三異向性磁電阻單元226與第四異向性磁電阻單元228的磁化方向。The first magnetization direction setting element M1 is used to set the magnetization directions of the first anisotropic
當一電流I流經導線110時,因感應於電流I所產生的磁場,第一異向性磁電阻單元222所產生的電阻值變化相反於第二異向性磁電阻單元224所產生的電阻值變化,且第三異向性磁電阻單元226所產生的電阻值變化相反於第四異向性磁電阻單元228所產生的電阻值變化,且第一、第二、第三及第四異向性磁電阻單元222、224、226及228電性連接成一惠斯登電橋,以輸出對應於第一、第二、第三及第四異向性磁電阻單元222、224、226及228所產生的電阻值變化的電壓訊號。When a current I flows through the
在本實施例中,第一異向性磁電阻單元222包括沿著第二方向D2的反方向依序排列的一第一異向性磁電阻(anisotropic magnetoresistor, AMR)R1與一第二異向性磁電阻R2,第二異向性磁電阻單元224包括沿著第二方向D2的反方向依序排列的一第三異向性磁電阻R3與一第四異向性磁電阻R4,第三異向性磁電阻單元226包括沿著第二方向D2的反方向依序排列的一第五異向性磁電阻R5與一第六異向性磁電阻R6,且第四異向性磁電阻單元228包括沿著第二方向D2的反方向依序排列的一第七異向性磁電阻R7與一第八異向性磁電阻R8。上述的第一至第八異向性磁電阻R1~R8的數量都是各自以一個為例,然而,在其他實施例中,每一個異向性磁電阻亦可以用串聯的多個異向性磁電阻來取代。舉例而言,第一異向性磁電阻R1可以用多個串聯的第一異向性磁電阻R1來取代。In this embodiment, the first anisotropic
在本實施例中,第一磁化方向設定元件M1與第二磁化方向設定元件M2及第一至第四異向性磁電阻單元222、224、226及228可設置於基板210上,而磁化方向設定元件與異向性磁電阻單元之間可藉由絕緣層來隔開。在本實施例中,第一磁化方向設定元件M1配置於第一及第二異向性磁電阻單元222、224與第一導電段C1之間,且第二磁化方向設定元件M2配置於第三及第四異向性磁電阻單元226、228與第二導電段C2之間。然而,在其他實施例中,亦可以是第一及第二異向性磁電阻單元222、224配置於第一磁化方向設定元件M1與第一導電段C1之間,且第三及第四異向性磁電阻單元226、228配置於第二磁化方向設定元件M2與第二導電段C2之間。或者,在其他實施例中,第一磁化方向設定元件M1亦可以是在第一及第二異向性磁電阻單元222、224的上下兩方都有分佈,且第二磁化方向設定元件M2亦可以是在第三及第四異向性磁電阻單元226、228的上下兩方都有分佈。In this embodiment, the first magnetization direction setting element M1 and the second magnetization direction setting element M2, and the first to fourth
另外,導線110可被一封裝體120包覆,而導線110的兩端則暴露於封裝體120外,其中封裝體120例如是絕緣材質。基板210可配置於封裝體120上。In addition, the
圖3A與圖3B是用以說明圖1中的異向性磁電阻的運作原理。請先參照圖3A,異向性磁電阻300具有理髮店招牌(barber pole)狀結構,亦即其表面設有相對於異向性磁電阻300的延伸方向D傾斜45度延伸的多個短路棒(electrical shorting bar)310,這些短路棒310彼此相間隔且平行地設置於鐵磁膜(ferromagnetic film)320上,而鐵磁膜320為異向性磁電阻300的主體,其延伸方向即為異向性磁電阻300的延伸方向D。此外,鐵磁膜320的相對兩端可製作成尖端狀。3A and 3B are used to illustrate the operation principle of the anisotropic magnetoresistance in FIG. 1. Please refer to FIG. 3A first, the
異向性磁電阻300在開始量測外在磁場H之前,可先藉由磁化方向設定元件(例如圖1的第一磁化方向設定元件M1或第二磁化方向設定元件M2)來設定其磁化方向,其中磁化方向設定元件例如是可以藉由通電產生磁場的線圈、導線、金屬片或導體。在圖3A中,磁化方向設定元件可藉由通電產生沿著延伸方向D的磁場,以使異向性磁電阻300具有磁化方向M。Before measuring the external magnetic field H of the
接著,磁化方向設定元件不通電,以使異向性磁電阻300開始量測外在磁場H。當沒有外在磁場H時,異向性磁電阻300的磁化方向M維持在延伸方向D上,此時施加一電流i,使電流i從異向性磁電阻300的左端流往右端,則短路棒310附近的電流i的流向會與短路棒310的延伸方向垂直,而使得短路棒310附近的電流i流向與磁化方向M夾45度,此時異向性磁電阻300的電阻值為R。Next, the magnetization direction setting element is not energized, so that the
當有一外在磁場H朝向垂直於延伸方向D的方向時,異向性磁電阻300的磁化方向M會往外在磁場H的方向偏轉,而使得磁化方向與短路棒附近的電流i流向的夾角大於45度,此時異向性磁電阻300的電阻值有-ΔR的變化,即成為R-ΔR,也就是電阻值變小,其中ΔR大於0。When an external magnetic field H faces a direction perpendicular to the extension direction D, the magnetization direction M of the
然而,若如圖3B所示,當圖3B的短路棒310的延伸方向設於與圖3A的短路棒310的延伸方向夾90度的方向時(此時圖3B的短路棒310的延伸方向仍與異向性磁電阻300的延伸方向D夾45度),且當有一外在磁場H時,此外在磁場H仍會使磁化方向M往外在磁場H的方向偏轉,此時磁化方向M與短路棒310附近的電流i流向的夾角會小於45度,如此異向性磁電阻300的電阻值會變成R+ΔR,亦即異向性磁電阻300的電阻值變大。However, as shown in FIG. 3B, when the extension direction of the shorting
此外,藉由磁化方向設定元件將異向性磁電阻300的磁化方向M設定為圖3A所示的反向時,之後在外在磁場H下的圖3A的異向性磁電阻300的電阻值會變成R+ΔR。再者,藉由磁化方向設定元件將異向性磁電阻300的磁化方向M設定為圖3B所示的反向時,之後在外在磁場H下的圖3B的異向性磁電阻300的電阻值會變成R-ΔR。In addition, when the magnetization direction M of the
綜合上述可知,當短路棒310的設置方向改變時,異向性磁電阻300的電阻值R對應於外在磁場H的變化會從+ΔR變為-ΔR或反之,且當磁化方向設定元件所設定的磁化方向M改變成反向時,異向性磁電阻300的電阻值R對應於外在磁場H的變化會從+ΔR變為-ΔR或反之。當外在磁場H的方向變為反向時,異向性磁電阻300的電阻值R對應於外在磁場H的變化會從+ΔR變為-ΔR或反之。然而,當通過異向性磁電阻300的電流i變成反向時,異向性磁電阻300的電阻值R對應於外在磁場H的變化則維持與原來相同正負號,即原本若為+ΔR,改變電流方向後仍為+ΔR,若原本為-ΔR,改變電流方向後仍為-ΔR。Based on the above, when the setting direction of the shorting
依照上述的原則,便可藉由設計短路棒310的延伸方向或磁化方向設定元件所設定的磁化方向M來決定當異向性磁電阻300受到外在磁場H的某一分量時,異向性磁電阻300的電阻值R的變化方向,即電阻值R變大或變小,例如變化量是+ΔR或-ΔR。According to the above principles, the anisotropic magnetization direction M can be determined by designing the extension direction of the shorting
圖4A與圖4B分別繪示圖1之電流感測器於第一時間與第二時間之異向性磁電阻的磁化方向及其後的電阻值變化,並繪示了第一至第八異向性磁電阻R1~R8中的短路棒的延伸方向。請參照圖4A與圖4B,在本實施例中,第一至第八異向性磁電阻R1~R8的延伸方向皆為第二方向D2,而其短路棒310的延伸方向則如圖4A所繪示,其分別在兩個不同的方向上與第二方向D2夾45度,且這兩個不同的方向是平行於第一方向D1與第二方向D2所建構的平面。4A and 4B illustrate the magnetization direction of the anisotropic magnetoresistance at the first time and the second time of the current sensor of FIG. 1 and the resistance value changes thereafter, respectively, and illustrate the first to eighth anomalies The extension direction of the shorting bar in the directional magnetoresistance R1 to R8. 4A and 4B, in this embodiment, the extension direction of the first to eighth anisotropic magnetoresistor R1 to R8 is the second direction D2, and the extension direction of the shorting
當導線110被通以電流I(如圖1所繪示)時,在第一導電段C1中的電流I1與在第二導電段C2中的電流I2的方向例如分別為第二方向D2與第二方向D2的反方向。此時,電流I1在第一至第四異向性磁電阻R1~R4上產生沿著第一方向D1的磁場分量HC,且電流I2在第五至第八異向性磁電阻R5~R8上產生沿著第一方向D1的反方向的磁場分量HC。在本實施例中,電流I1的大小等於電流I2的大小。此外,在本實施例中,當電流I流經導線110時,電流I在第一導電段C1中的流向(即電流I1的流向)相反於在第二導電段C2中的流向(即電流I2的流向)。此外,在本實施例中,電流I1流經第一導電段C1時在第一異向性磁電阻單元222與第二異向性磁電阻單元224處所產生的磁場在第一方向D1上的分量(即圖4A與圖4B左方的磁場分量HC,其朝向第一方向D1)的方向相反於電流I2流經第二導電段C2時在第三異向性磁電阻單元226與第四異向性磁電阻單元228處所產生的磁場在第一方向D1上的分量(即圖4A與圖4B右方的磁場分量HC,其朝向第一方向D1的反方向)的方向。When the
在一第一時間,第一磁化方向設定元件M1將第一異向性磁電阻R1與第三異向性磁電阻R3的磁化方向M13設定為第二方向D2的反方向,且將第二異向性磁電阻R2與第四異向性磁電阻R4的磁化方向M24設定為第二方向D2。此外,在第一時間,第二磁化方向設定元件M2將第五異向性磁電阻R5與第七異向性磁電阻R7的磁化方向M57設定為第二方向D2的反方向,且將第六異向性磁電阻R6與第八異向性磁電阻R8的磁化方向M68設定為第二方向D2。在本實施例中,第一磁化方向設定元件M1與第二磁化方向設定元件M2例如為可以藉由通電產生磁場的導電線圈、導線、導電片(例如金屬片)或導體,只要是能夠產生沿著磁化方向M13、M24、M57、M68的磁場之導電結構皆可作為第一磁化方向設定元件M1與第二磁化方向設定元件M2。At a first time, the first magnetization direction setting element M1 sets the magnetization direction M13 of the first anisotropic magnetic resistance R1 and the third anisotropic magnetic resistance R3 to the opposite direction of the second direction D2, and sets the second different The magnetization direction M24 of the directional magnetic resistance R2 and the fourth anisotropic magnetic resistance R4 is set to the second direction D2. In addition, at the first time, the second magnetization direction setting element M2 sets the magnetization direction M57 of the fifth anisotropic magnetic resistance R5 and the seventh anisotropic magnetic resistance R7 to the opposite direction of the second direction D2, and sets the sixth The magnetization direction M68 of the anisotropic magnetic resistance R6 and the eighth anisotropic magnetic resistance R8 is set to the second direction D2. In this embodiment, the first magnetization direction setting element M1 and the second magnetization direction setting element M2 are, for example, conductive coils, wires, conductive sheets (for example, metal sheets), or conductors that can generate a magnetic field by energization, as long as they can generate along The conductive structure of the magnetic field in the magnetization directions M13, M24, M57, and M68 can be used as the first magnetization direction setting element M1 and the second magnetization direction setting element M2.
在第一時間之後,第一磁化方向設定元件M1與第二磁化方向設定元件M2會停止產生磁場,例如第一磁化方向設定元件M1與第二磁化方向設定元件M2不再被通以電流而產生磁場,此時,第一至第四異向性磁電阻R1~R4便能夠感應於電流I1所產生的磁場分量HC而分別產生-ΔR、-ΔR、+ΔR及+ΔR的電阻值變化,且第五至第八異向性磁電阻R5~R8便能夠感應於電流I2所產生的磁場分量HC而分別產生+ΔR、+ΔR、-ΔR及-ΔR的電阻值變化。After the first time, the first magnetization direction setting element M1 and the second magnetization direction setting element M2 will stop generating magnetic fields. For example, the first magnetization direction setting element M1 and the second magnetization direction setting element M2 will no longer be energized. Magnetic field. At this time, the first to fourth anisotropic magnetoresistances R1 to R4 can induce the magnetic field component HC generated by the current I1 to generate -ΔR, -ΔR, +ΔR, and +ΔR resistance changes, respectively, and The fifth to eighth anisotropic magnetic resistors R5 to R8 can induce the magnetic field component HC generated by the current I2 to generate resistance changes of +ΔR, +ΔR, -ΔR, and -ΔR, respectively.
在本實施例中,第一異向性磁電阻R1、第二異向性磁電阻R2、第六異向性磁電阻R6及第五異向性磁電阻R5可從接點P1依序串聯至接點P2,接點P3可電性連接至第二異向性磁電阻R2與第六異向性磁電阻R6之間的導電路徑,第三異向性磁電阻R3與第四異向性磁電阻R4可從接點P1依序串聯至接點P4,而第七異向性磁電阻R7與第八異向性磁電阻R8可從接點P2依序串聯至接點P5。接點P3可接收參考電壓VDD,而接點P4與接點P5可耦接至地(ground),此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會是(VDD)×(ΔR/R),其可以為輸出訊號,此輸出訊號為一差分訊號,其大小會對應於磁場分量HC的大小,進而對應於流經導線110的電流I的大小,此後將此輸出訊號稱為第一電壓訊號V1
。在另一實施例中,亦可以是接點P3耦接至地,而接點P4與接點P5接收參考電壓VDD。In this embodiment, the first anisotropic magnetic resistance R1, the second anisotropic magnetic resistance R2, the sixth anisotropic magnetic resistance R6, and the fifth anisotropic magnetic resistance R5 can be connected in series from the contact point P1 to Contact point P2, contact point P3 can be electrically connected to the conductive path between the second anisotropic magnetic resistance R2 and the sixth anisotropic magnetic resistance R6, the third anisotropic magnetic resistance R3 and the fourth anisotropic magnetic resistance The resistor R4 can be connected in series from the connection point P1 to the connection point P4, and the seventh anisotropic magnetic resistance R7 and the eighth anisotropic magnetic resistance R8 can be connected in series from the connection point P2 to the connection point P5. The contact P3 can receive the reference voltage VDD, and the contact P4 and the contact P5 can be coupled to ground. At this time, the voltage difference between the contact P1 and the contact P2 in the Wheatstone bridge formed will be (VDD)×(ΔR/R), it can be an output signal, this output signal is a differential signal, and its magnitude will correspond to the magnitude of the magnetic field component HC, which in turn corresponds to the magnitude of the current I flowing through the
在此之後的一第二時間,第一磁化方向設定元件M1將第一異向性磁電阻R1與第三異向性磁電阻R3的磁化方向M13’設定為第二方向D2,且將第二異向性磁電阻R2與第四異向性磁電阻R4的磁化方向M24’設定為第二方向D2的反方向。此外,在第二時間,第二磁化方向設定元件M2將第五異向性磁電阻R5與第七異向性磁電阻R7的磁化方向M57’設定為第二方向D2,且將第六異向性磁電阻R6與第八異向性磁電阻R8的磁化方向M68’設定為第二方向D2的反方向。At a second time after this, the first magnetization direction setting element M1 sets the magnetization direction M13' of the first anisotropic magnetic resistance R1 and the third anisotropic magnetic resistance R3 to the second direction D2, and sets the second The magnetization direction M24' of the anisotropic magnetic resistance R2 and the fourth anisotropic magnetic resistance R4 is set to the opposite direction of the second direction D2. In addition, at the second time, the second magnetization direction setting element M2 sets the magnetization direction M57' of the fifth anisotropic magnetic resistance R5 and the seventh anisotropic magnetic resistance R7 to the second direction D2, and sets the sixth anisotropy The magnetization direction M68' of the linear magnetic resistance R6 and the eighth anisotropic magnetic resistance R8 is set to the opposite direction of the second direction D2.
在第二時間之後,第一磁化方向設定元件M1與第二磁化方向設定元件M2會停止產生磁場,此時,第一至第四異向性磁電阻R1~R4便能夠感應於電流I1所產生的磁場分量HC而分別產生+ΔR、+ΔR、-ΔR及-ΔR的電阻值變化,且第五至第八異向性磁電阻R5~R8便能夠感應於電流I2所產生的磁場分量HC而分別產生-ΔR、-ΔR、+ΔR及+ΔR的電阻值變化。此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會是(VDD)×(-ΔR/R),其可以為輸出訊號,此輸出訊號為一差分訊號,其大小會對應於磁場分量HC的大小,進而對應於流經導線110的電流I的大小,此後將此輸出訊號稱為第二電壓訊號V2
。After the second time, the first magnetization direction setting element M1 and the second magnetization direction setting element M2 will stop generating a magnetic field. At this time, the first to fourth anisotropic magnetoresistances R1 to R4 can be induced by the current I1. The magnetic field component HC generated by the resistance value changes of +ΔR, +ΔR, -ΔR, and -ΔR, and the fifth to eighth anisotropic magnetoresistance R5 to R8 can induce the magnetic field component HC generated by the current I2. Respectively produce -ΔR, -ΔR, +ΔR and +ΔR resistance value changes. The voltage difference between the contact point P1 and the contact point P2 in the Wheatstone bridge formed at this time will be (VDD)×(-ΔR/R), which can be an output signal, and this output signal is a differential signal. The magnitude will correspond to the magnitude of the magnetic field component HC, and in turn correspond to the magnitude of the current I flowing through the
圖5為圖4A與圖4B的惠斯登電橋的輸出電壓-電流曲線圖,而圖6繪示圖4A與圖4B的惠斯登電橋耦接至一運算器。請參照圖4A、圖4B、圖5與圖6,在本實施例中,電流感測器100更包括一運算器400,電性連接至惠斯登電橋的一輸出端(即接收第一電壓訊號V1
與第二電壓訊號V2
),其中第一磁化方向設定元件M1與第二磁化方向設定元件M2將第一、第二、第三及第四異向性磁電阻單元222、224、226及228的磁化方向組合設定為一第一組合(即如圖4A之磁化方向M13、磁化方向M24、磁化方向M57及磁化方向M68的組合),以使惠斯登電橋之後輸出第一電壓訊號V1
,且第一磁化方向設定元件M1與第二磁化方向設定元件M2再將第一、第二、第三及第四異向性磁電阻單元222、224、226及228的磁化方向組合設定為相反於第一組合的一第二組合(即如圖4B之磁化方向M13’、磁化方向M24’、磁化方向M57’及磁化方向M68’的組合),以使惠斯登電橋之後輸出第二電壓訊號V2
。運算器400用以將第一電壓訊號V1
與第二電壓訊號V2
相減,以輸出一對應於電流I所產生的磁場的大小的輸出電壓訊號Vout
。此外,在本實施例中,運算器400亦可用以將第一電壓訊號V1
與第二電壓訊號V2
相加,以輸出一偏移電壓訊號Voff
。5 is a graph showing the output voltage-current curve of the Wheatstone bridge in FIGS. 4A and 4B, and FIG. 6 shows the Wheatstone bridge in FIGS. 4A and 4B coupled to an arithmetic unit. 4A, 4B, 5 and 6, in this embodiment, the
具體而言,運算器400可包括一算術運算器410與一算術運算器420,其中算術運算器410例如為一加法器,其用以將第一電壓訊號V1
與第二電壓訊號V2
相加,以輸出偏移電壓訊號Voff
。此外,算術運算器420例如為一減法器,其用以將第一電壓訊號V1
與第二電壓訊號V2
相減,以輸出對應於電流I所產生的磁場的大小的輸出電壓訊號Vout
。Specifically, the
由圖5可知,惠斯登電橋的輸出電壓-電流曲線可能存在一偏移電壓訊號Voff ,而第一電壓訊號V1 與第二電壓訊號V2 相加之後則可剩下偏移電壓訊號Voff ,且第一電壓訊號V1 與第二電壓訊號V2 相減後,其輸出電壓-電流曲線會通過電壓與電流皆為零的點,而使得在某一段範圍內電壓與電流幾乎成正比,而使得電阻值變化ΔR可以準確地經由輸出電壓訊號Vout 來估算。It can be seen from Figure 5 that there may be an offset voltage signal V off in the output voltage-current curve of the Wheatstone bridge, and the offset voltage can be left after the first voltage signal V 1 and the second voltage signal V 2 are added. After the signal V off and the first voltage signal V 1 and the second voltage signal V 2 are subtracted, the output voltage-current curve will pass through the point where both voltage and current are zero, so that the voltage and current are almost It is proportional to, so that the resistance change ΔR can be accurately estimated through the output voltage signal V out .
在本實施例中,接點P1~P5及運算器400例如是存在於基板210中,而基板210為一線路基板,例如是半導體基板。In this embodiment, the contacts P1 to P5 and the
圖7、圖8及圖9分別繪示圖1之電流感測器於第二時間之異向性磁電阻的磁化方向及其後受到三個不同方向的外在磁場分量時的電阻值變化。請先參照圖7,第一磁化方向設定元件M1與第二磁化方向設定元件M2在第二時間完成磁化方向M13’、M24’、M57’、M68’的設定之後,當有一沿著第一方向D1的外在磁場分量HE1存在時,第一至第八異向性磁電阻R1~R8所產生的電阻值變化分別為+ΔR、+ΔR、-ΔR、-ΔR、+ΔR、+ΔR、-ΔR及-ΔR,如此一來,當接點P3接收參考電壓VDD,而接點P4與接點P5耦接至地時,此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會為零。7, 8 and 9 respectively show the magnetization direction of the anisotropic magnetoresistance of the current sensor of FIG. 1 at the second time and the resistance value changes when it receives external magnetic field components in three different directions thereafter. Please refer to FIG. 7 first, after the first magnetization direction setting element M1 and the second magnetization direction setting element M2 complete the setting of the magnetization directions M13', M24', M57', and M68' at the second time, when there is one along the first direction When the external magnetic field component HE1 of D1 exists, the resistance value changes produced by the first to eighth anisotropic magnetoresistance R1~R8 are respectively +ΔR, +ΔR, -ΔR, -ΔR, +ΔR, +ΔR,- ΔR and -ΔR, in this way, when the contact P3 receives the reference voltage VDD, and the contact P4 and the contact P5 are coupled to the ground, the Wheatstone bridge formed at this time between the contact P1 and the contact P2 The voltage difference between will be zero.
請再參照圖8,第一磁化方向設定元件M1與第二磁化方向設定元件M2在第二時間完成磁化方向M13’、M24’、M57’、M68’的設定之後,當有一沿著第二方向D2的外在磁場分量HE2存在時,第一至第八異向性磁電阻R1~R8所產生的電阻值變化皆為零,這是因為第二方向D2不是第一至第八異向性磁電阻R1~R8所能感測的方向。如此一來,當接點P3接收參考電壓VDD,而接點P4與接點P5耦接至地時,此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會為零。Please refer to FIG. 8 again. After the first magnetization direction setting element M1 and the second magnetization direction setting element M2 complete the setting of the magnetization directions M13', M24', M57', and M68' at the second time, when there is one along the second direction When the external magnetic field component HE2 of D2 exists, the resistance value changes produced by the first to eighth anisotropic magnetoresistor R1 to R8 are all zero, because the second direction D2 is not the first to eighth anisotropic magnetism The direction that the resistors R1 to R8 can sense. In this way, when the contact P3 receives the reference voltage VDD and the contact P4 and the contact P5 are coupled to the ground, the voltage difference between the contact P1 and the contact P2 in the Wheatstone bridge formed at this time will be Is zero.
請再參照圖9,第一磁化方向設定元件M1與第二磁化方向設定元件M2在第二時間完成磁化方向M13’、M24’、M57’、M68’的設定之後,當有一沿著第三方向D3的外在磁場分量HE3存在時,第一至第八異向性磁電阻R1~R8所產生的電阻值變化皆為零,這是因為第三方向D3不是第一至第八異向性磁電阻R1~R8所能感測的方向。如此一來,當接點P3接收參考電壓VDD,而接點P4與接點P5耦接至地時,此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會為零。Please refer to FIG. 9 again. After the first magnetization direction setting element M1 and the second magnetization direction setting element M2 complete the setting of the magnetization directions M13', M24', M57', and M68' at the second time, when there is one along the third direction When the external magnetic field component HE3 of D3 exists, the resistance value changes produced by the first to eighth anisotropic magnetoresistor R1 to R8 are all zero, because the third direction D3 is not the first to eighth anisotropic magnetism The direction that the resistors R1 to R8 can sense. In this way, when the contact P3 receives the reference voltage VDD and the contact P4 and the contact P5 are coupled to the ground, the voltage difference between the contact P1 and the contact P2 in the Wheatstone bridge formed at this time will be Is zero.
也就是說,在本實施例中,惠斯登電橋對應於在第一方向D1上的外在磁場分量HE1所輸出的電壓訊號為零,對應於在第二方向D2上的外在磁場分量HE2所輸出的電壓訊號為零,且對應於在第三方向D3上的外在磁場分量HE3所輸出的電壓訊號為零。因此,無論外在磁場是在哪個方向上,都不會影響本實施例的電流感測器100的感測結果,也就是不會對電流感測器100的輸出電壓產生干擾。That is, in this embodiment, the Wheatstone bridge corresponds to the external magnetic field component HE1 in the first direction D1 and the output voltage signal is zero, which corresponds to the external magnetic field component in the second direction D2. The voltage signal output by HE2 is zero, and the voltage signal output by HE3 corresponding to the external magnetic field component in the third direction D3 is zero. Therefore, no matter which direction the external magnetic field is in, it will not affect the sensing result of the
以上惠斯登電橋對於外在磁場分量HE1、HE2及HE3的反應是以第二時間之後的反應為例,至於在第一時間之後,即在第一磁化方向設定元件M1與第二磁化方向設定元件M2在第一時間完成如圖4A的磁化方向M13、M24、M57、M68的設定之後,第一至第八異向性磁電阻R1~R8反應於外在磁場分量HE1所產生的電阻值變化分別為-ΔR、-ΔR、+ΔR、+ΔR、-ΔR、-ΔR、+ΔR及+ΔR,如此一來,當接點P3接收參考電壓VDD,而接點P4與接點P5耦接至地時,此時形成的惠斯登電橋中接點P1與接點P2之間的電壓差會為零。而對於外在磁場分量HE2與HE3,第一至第八異向性磁電阻R1~R8不會受到它們的影響,因此不會產生電阻值變化,因此惠斯登電橋中接點P1與接點P2之間的電壓差仍會為零。所以,無論是在第一時間或第二時間之後,本實施例的電流感測器100皆不會受到任何方向的外在磁場的干擾。The above response of the Wheatstone bridge to the external magnetic field components HE1, HE2, and HE3 is based on the response after the second time as an example. After the first time, the element M1 and the second magnetization direction are set in the first magnetization direction. After the setting element M2 completes the setting of the magnetization directions M13, M24, M57, and M68 as shown in Fig. 4A at the first time, the first to eighth anisotropic magnetoresistance R1 to R8 react to the resistance value generated by the external magnetic field component HE1 The changes are -ΔR, -ΔR, +ΔR, +ΔR, -ΔR, -ΔR, +ΔR, and +ΔR. In this way, when the contact P3 receives the reference voltage VDD, and the contact P4 is coupled to the contact P5 When reaching the ground, the voltage difference between the contact point P1 and the contact point P2 in the Wheatstone bridge formed at this time will be zero. For the external magnetic field components HE2 and HE3, the first to eighth anisotropic magnetoresistance R1 to R8 will not be affected by them, so there will be no resistance change. Therefore, the contact point P1 in the Wheatstone bridge is connected to the The voltage difference between points P2 will still be zero. Therefore, no matter after the first time or the second time, the
此外,基板210中或基板210上也可設有一反饋線圈(feedback coil),其與第一至第八異向性磁電阻R1~R8至少部分重疊,以作為閉迴路控制(close-loop control)的用途。In addition, the
綜上所述,在本發明的實施例的電流感測器中,由於採用了異向性磁電阻單元連接成惠斯登電橋來感測導線中的電流所產生的磁場,因此對電流的感測具有高敏感度與高準確度。此外,由於本發明的實施例的電流感測器是利用感測電流所產生的磁場的方式來反推電流的大小,而異向性磁電阻單元不會直接接觸到電流,因此可以具有較低的功耗。To sum up, in the current sensor of the embodiment of the present invention, because the anisotropic magnetoresistance unit is connected to form a Wheatstone bridge to sense the magnetic field generated by the current in the wire, the current The sensing has high sensitivity and high accuracy. In addition, because the current sensor of the embodiment of the present invention uses the magnetic field generated by the sensing current to reverse the magnitude of the current, the anisotropic magnetoresistive unit does not directly contact the current, so it can have a lower Power consumption.
雖然本發明已以實施例揭露如上,然其並非用以限定本發明,任何所屬技術領域中具有通常知識者,在不脫離本發明的精神和範圍內,當可作些許的更動與潤飾,故本發明的保護範圍當視後附的申請專利範圍所界定者為準。Although the present invention has been disclosed in the above embodiments, it is not intended to limit the present invention. Anyone with ordinary knowledge in the relevant technical field can make slight changes and modifications without departing from the spirit and scope of the present invention. The scope of protection of the present invention shall be determined by the scope of the attached patent application.
100‧‧‧電流感測器 110‧‧‧導線 120‧‧‧封裝體 210‧‧‧基板 212‧‧‧第一端 214‧‧‧第二端 222‧‧‧第一異向性磁電阻單元 224‧‧‧第二異向性磁電阻單元 226‧‧‧第三異向性磁電阻單元 228‧‧‧第四異向性磁電阻單元 300‧‧‧異向性磁電阻 310‧‧‧短路棒 320‧‧‧鐵磁膜 400‧‧‧運算器 410、420‧‧‧算術運算器 C1‧‧‧第一導電段 C2‧‧‧第二導電段 D‧‧‧延伸方向 D1‧‧‧第一方向 D2‧‧‧第二方向 D3‧‧‧第三方向 H‧‧‧外在磁場 HC‧‧‧磁場分量 HE1、HE2、HE3‧‧‧外在磁場分量 I、i、I1、I2‧‧‧電流 M、M13、M13’、M24、M24’、M57、M57’、M68、M68’‧‧‧磁化方向 M1‧‧‧第一磁化方向設定元件 M2‧‧‧第二磁化方向設定元件 P1、P2、P3、P4、P5‧‧‧接點 R1‧‧‧第一異向性磁電阻 R2‧‧‧第二異向性磁電阻 R3‧‧‧第三異向性磁電阻 R4‧‧‧第四異向性磁電阻 R5‧‧‧第五異向性磁電阻 R6‧‧‧第六異向性磁電阻 R7‧‧‧第七異向性磁電阻 R8‧‧‧第八異向性磁電阻 ΔR‧‧‧電阻值變化 V1‧‧‧第一電壓訊號 V2‧‧‧第二電壓訊號 Voff‧‧‧偏移電壓訊號 Vout‧‧‧輸出電壓訊號100‧‧‧Current sensor 110‧‧‧Wire 120‧‧‧Package body 210‧‧‧Substrate 212‧‧‧First end 214‧‧‧Second end 222‧‧‧First anisotropic magnetoresistive unit 224‧‧‧The second anisotropic magnetoresistance unit 226‧‧‧The third anisotropic magnetoresistance unit 228‧‧‧The fourth anisotropic magnetoresistance unit 300‧‧‧Anisotropic magnetoresistance 310‧‧Short Rod 320‧‧‧Ferromagnetic film 400‧‧‧Calculator 410, 420‧‧‧Arithmetic operator C1‧‧‧First conductive segment C2‧‧‧Second conductive segment D‧‧‧Extending direction D1‧‧‧ One direction D2‧‧‧The second direction D3‧‧‧The third direction H‧‧‧External magnetic field HC‧‧‧Magnetic field components HE1, HE2, HE3‧‧‧External magnetic field components I, i, I1, I2‧‧ ‧Current M, M13, M13', M24, M24', M57, M57', M68, M68'‧‧‧Magnetic direction M1‧‧‧First magnetization direction setting element M2 P2, P3, P4, P5‧‧‧Contact R1‧‧‧First anisotropic magnetoresistance R2‧‧‧Second anisotropic magnetoresistance R3‧‧‧Third anisotropic magnetoresistance R4‧‧‧Second Four anisotropic magnetoresistance R5‧‧‧Fifth anisotropic magnetoresistance R6‧‧‧Sixth anisotropic magnetoresistance R7‧‧‧Seventh anisotropic magnetoresistance R8‧‧‧Eighth anisotropic magnetoresistance ΔR‧‧‧Resistance value change V 1 ‧‧‧First voltage signal V 2 ‧‧‧Second voltage signal V off ‧‧‧Offset voltage signal V out ‧‧‧Output voltage signal
圖1是本發明的一實施例的一種電流感測器的上視示意圖。 圖2是圖1的電流感測器沿著A-A線的剖面示意圖。 圖3A與圖3B是用以說明圖1中的異向性磁電阻的運作原理。 圖4A與圖4B分別繪示圖1之電流感測器於第一時間與第二時間之異向性磁電阻的磁化方向及其後的電阻值變化。 圖5為圖4A與圖4B的惠斯登電橋的輸出電壓-電流曲線圖。 圖6繪示圖4A與圖4B的惠斯登電橋耦接至一運算器。 圖7、圖8及圖9分別繪示圖1之電流感測器於第二時間之異向性磁電阻的磁化方向及其後受到三個不同方向的外在磁場分量時的電阻值變化。FIG. 1 is a schematic top view of a current sensor according to an embodiment of the invention. Fig. 2 is a schematic cross-sectional view of the current sensor of Fig. 1 along the line A-A. 3A and 3B are used to illustrate the operation principle of the anisotropic magnetoresistance in FIG. 1. 4A and 4B respectively show the magnetization direction of the anisotropic magnetoresistance at the first time and the second time of the current sensor of FIG. 1 and the resistance change thereafter. Fig. 5 is a graph showing output voltage-current curves of the Wheatstone bridge in Figs. 4A and 4B. FIG. 6 shows the Wheatstone bridge of FIGS. 4A and 4B coupled to an arithmetic unit. 7, 8 and 9 respectively show the magnetization direction of the anisotropic magnetoresistance of the current sensor of FIG. 1 at the second time and the resistance value changes when it receives external magnetic field components in three different directions thereafter.
100‧‧‧電流感測器 100‧‧‧Current Sensor
110‧‧‧導線 110‧‧‧Wire
120‧‧‧封裝體 120‧‧‧Package
210‧‧‧基板 210‧‧‧Substrate
212‧‧‧第一端 212‧‧‧First end
214‧‧‧第二端 214‧‧‧Second end
222‧‧‧第一異向性磁電阻單元 222‧‧‧The first anisotropic magnetoresistance unit
224‧‧‧第二異向性磁電阻單元 224‧‧‧Second Anisotropic Magnetoresistance Unit
226‧‧‧第三異向性磁電阻單元 226‧‧‧The third anisotropic magnetoresistance unit
228‧‧‧第四異向性磁電阻單元 228‧‧‧Fourth anisotropic magnetoresistance unit
C1‧‧‧第一導電段 C1‧‧‧First conductive section
C2‧‧‧第二導電段 C2‧‧‧Second conductive section
D1‧‧‧第一方向 D1‧‧‧First direction
D2‧‧‧第二方向 D2‧‧‧Second direction
D3‧‧‧第三方向 D3‧‧‧ Third party
I‧‧‧電流 I‧‧‧Current
M1‧‧‧第一磁化方向設定元件 M1‧‧‧First magnetization direction setting element
M2‧‧‧第二磁化方向設定元件 M2‧‧‧Second magnetization direction setting element
R1‧‧‧第一異向性磁電阻 R1‧‧‧First anisotropic magnetoresistance
R2‧‧‧第二異向性磁電阻 R2‧‧‧Second Anisotropic Magnetoresistance
R3‧‧‧第三異向性磁電阻 R3‧‧‧The third anisotropic magnetoresistance
R4‧‧‧第四異向性磁電阻 R4‧‧‧Fourth anisotropic magnetoresistance
R5‧‧‧第五異向性磁電阻 R5‧‧‧Fifth anisotropic magnetoresistance
R6‧‧‧第六異向性磁電阻 R6‧‧‧The sixth anisotropic magnetoresistance
R7‧‧‧第七異向性磁電阻 R7‧‧‧The seventh anisotropic magnetoresistance
R8‧‧‧第八異向性磁電阻 R8‧‧‧Eighth Anisotropic Magnetoresistance
Claims (9)
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