CN104034463A - High-linearity segmented-excitation type torque sensor - Google Patents
High-linearity segmented-excitation type torque sensor Download PDFInfo
- Publication number
- CN104034463A CN104034463A CN201410258858.8A CN201410258858A CN104034463A CN 104034463 A CN104034463 A CN 104034463A CN 201410258858 A CN201410258858 A CN 201410258858A CN 104034463 A CN104034463 A CN 104034463A
- Authority
- CN
- China
- Prior art keywords
- winding
- axis
- iron core
- excitation
- torque sensor
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000004804 winding Methods 0.000 claims abstract description 217
- 230000005284 excitation Effects 0.000 claims abstract description 88
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims abstract description 21
- 230000003993 interaction Effects 0.000 claims 1
- 230000011218 segmentation Effects 0.000 claims 1
- 230000008859 change Effects 0.000 abstract description 2
- 230000008878 coupling Effects 0.000 abstract 1
- 238000010168 coupling process Methods 0.000 abstract 1
- 238000005859 coupling reaction Methods 0.000 abstract 1
- 230000004907 flux Effects 0.000 description 24
- 238000005259 measurement Methods 0.000 description 8
- 238000006073 displacement reaction Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 3
- NCGICGYLBXGBGN-UHFFFAOYSA-N 3-morpholin-4-yl-1-oxa-3-azonia-2-azanidacyclopent-3-en-5-imine;hydrochloride Chemical compound Cl.[N-]1OC(=N)C=[N+]1N1CCOCC1 NCGICGYLBXGBGN-UHFFFAOYSA-N 0.000 description 2
- 230000005674 electromagnetic induction Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 230000035699 permeability Effects 0.000 description 2
- 229910000851 Alloy steel Inorganic materials 0.000 description 1
- 229910000975 Carbon steel Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910000976 Electrical steel Inorganic materials 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 239000010962 carbon steel Substances 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- UGKDIUIOSMUOAW-UHFFFAOYSA-N iron nickel Chemical compound [Fe].[Ni] UGKDIUIOSMUOAW-UHFFFAOYSA-N 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 229910001004 magnetic alloy Inorganic materials 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 229920002635 polyurethane Polymers 0.000 description 1
- 239000004814 polyurethane Substances 0.000 description 1
- 230000035939 shock Effects 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
Landscapes
- Force Measurement Appropriate To Specific Purposes (AREA)
Abstract
一种高线性度分段激磁式扭矩传感器,主要包括传感器轴、内环铁心、第一段激磁绕组、补偿绕组、外环铁心、输出绕组和第二段激磁绕组,第一段激磁绕组和补偿绕组固定在内环铁心中,两相绕组在空间上正交,第二段激磁绕组和输出绕组固定在外环铁心中,两相绕组在空间上也正交,传感器工作时,两段激磁绕组串接,通入正弦交变电压,传感器轴受到负载扭矩作用时,第二段激磁绕组和输出绕组在空间上的位置,相对于初始无负载扭矩作用时发生改变,经过电磁耦合,输出绕组产生与负载扭矩对应的感应电动势,通过合理调节两段激磁绕组的匝数与输出绕组的匝数,可以使得输出绕组产生的感应电动势与负载扭矩呈高度的线性对应关系。
A segmented excitation torque sensor with high linearity, which mainly includes a sensor shaft, an inner ring iron core, a first excitation winding, a compensation winding, an outer ring iron core, an output winding and a second excitation winding, the first excitation winding and compensation The windings are fixed in the inner ring iron core, the two-phase windings are orthogonal in space, the second excitation winding and the output winding are fixed in the outer ring iron core, the two-phase windings are also orthogonal in space, when the sensor is working, the two excitation windings Connected in series, input sinusoidal alternating voltage, when the sensor shaft is subjected to the load torque, the position of the second excitation winding and the output winding in space will change compared to the initial no-load torque, and through electromagnetic coupling, the output winding will generate The induced electromotive force corresponding to the load torque can make the induced electromotive force generated by the output winding and the load torque have a highly linear correspondence relationship by reasonably adjusting the number of turns of the two-stage excitation winding and the number of turns of the output winding.
Description
技术领域technical field
本发明涉及一种新型扭矩传感器,更具体的是涉及一种基于磁电感应原理的高线性度分段激磁式扭矩传感器。The invention relates to a novel torque sensor, more specifically to a high linearity segmented excitation torque sensor based on the principle of magnetoelectric induction.
背景技术Background technique
随着科学技术的不断进步和生产发展的各种需要,扭矩测量技术在工业、航空航天、农业、军事等多个领域获得了广泛的应用。例如在塑壳式低压断路器智能测控系统中,采用扭矩传感器对电机轴输出扭矩进行实时检测,当螺丝刀对螺母锁紧到一定程度时,扭矩瞬时增大,磁电式扭矩传感器检测到该阶跃信号,控制电机停转。With the continuous advancement of science and technology and the various needs of production development, torque measurement technology has been widely used in many fields such as industry, aerospace, agriculture, and military affairs. For example, in the intelligent measurement and control system of molded case low-voltage circuit breakers, the torque sensor is used to detect the output torque of the motor shaft in real time. When the screwdriver locks the nut to a certain degree, the torque increases instantaneously, and the magnetic torque sensor detects this stage jump signal to control the motor to stop.
目前在扭矩测量中,传递类扭矩传感器应用十分广泛,传递类扭矩传感器按扭矩信号的产生方式可分为光学式、光电式、磁电式、应变式、电容式等等,其中市场上较成熟的扭矩传感器主要是磁电式和应变式。磁电式扭矩传感器输出信号的本质是两路具有相位差的角位移信号,对信号进行组合处理后得到扭矩信息,它是非接触式传感器,无磨损、无摩擦,可用于长期测量,不足之处是体积大,不易安装,德国HBM公司、日本小野测器和中国湘西仪表厂均有生产;应变式转矩传感器以电阻应变片为敏感元件,如德国HBM公司的T1,T2,T4系列转矩传感器、北京三晶集团的JN338系列传感器等,它们在转轴或与转轴串接的弹性轴上安装四片精密电阻应变片,并连接成惠思顿电桥,扭矩使轴的微小变形引起应变阻值发生变化,电桥输出的信号与扭矩成比例,传感器可以测量静态和动态转矩、高频冲击和振动信息,具有体积小重量轻等优点,不足之处是信号的传输易受干扰且损耗较大,导致测量精度不是很高。At present, in torque measurement, transmission torque sensors are widely used. According to the generation mode of torque signals, transmission torque sensors can be divided into optical type, photoelectric type, magnetoelectric type, strain type, capacitive type, etc., among which the market is relatively mature. The current torque sensor is mainly magnetoelectric type and strain type. The essence of the output signal of the magnetoelectric torque sensor is two angular displacement signals with phase difference. The torque information is obtained after the signal is combined and processed. It is a non-contact sensor without wear and friction. It can be used for long-term measurement. It is large in size and difficult to install. It is produced by German HBM, Japan's Ono Shoki and China's Xiangxi Instrument Factory; strain-type torque sensors use resistance strain gauges as sensitive components, such as the T1, T2, and T4 series torque sensors of German HBM. Sensors, JN338 series sensors of Beijing Sanjing Group, etc., they install four precision resistance strain gauges on the rotating shaft or the elastic shaft connected in series with the rotating shaft, and connect them to form a Whiston bridge. The torque makes the small deformation of the shaft cause strain resistance When the value changes, the signal output by the bridge is proportional to the torque. The sensor can measure static and dynamic torque, high-frequency shock and vibration information. It has the advantages of small size and light weight. The disadvantage is that the transmission of the signal is susceptible to interference and loss Larger, the measurement accuracy is not very high.
发明内容Contents of the invention
本发明提供了一种新结构高线性度分段激磁式扭矩传感器,主要包括传感器轴、内环铁心、第一段激磁绕组、补偿绕组、外环铁心、第二段激磁绕组和输出绕组。第一段激磁绕组和补偿绕组固定在内环铁心中,两相绕组在空间上正交,第二段激磁绕组和输出绕组固定在外环铁心中,两相绕组在空间上也正交。The invention provides a new structure high linearity section excitation torque sensor, which mainly includes a sensor shaft, an inner ring iron core, a first section excitation winding, a compensation winding, an outer ring iron core, a second section excitation winding and an output winding. The first excitation winding and compensation winding are fixed in the inner ring iron core, and the two-phase windings are orthogonal in space. The second excitation winding and output winding are fixed in the outer ring iron core, and the two-phase windings are also orthogonal in space.
传感器工作时,两段激磁绕组串接,通入正弦交变电压,无负载扭矩作用时,第一段激磁绕组的轴线与第二段激磁绕组的轴线在空间上的位置相同,补偿绕组的轴线与输出绕组的轴线在空间上的位置也相同,激磁绕组产生的脉振磁通与输出绕组无匝链,输出绕组的感应电动势为零;传感器轴受到负载扭矩作用时,第二段激磁绕组与输出绕组同时扭转过一定的空间角度,相对无负载扭矩作用时的初始位置发生了改变,此时激磁绕组产生的脉振磁通与输出绕组匝链,经过电磁耦合,输出绕组产生与负载扭矩对应的感应电动势,通过合理调节两段激磁绕组的匝数与输出绕组的匝数,可以使得输出绕组产生的感应电动势与负载扭矩呈高度的线性关系。When the sensor is working, the two excitation windings are connected in series, and a sinusoidal alternating voltage is applied. When there is no load torque, the axis of the first excitation winding and the axis of the second excitation winding have the same position in space, and the axis of the compensation winding The position of the axis of the output winding is also the same in space. The pulsating magnetic flux generated by the excitation winding has no turn link with the output winding, and the induced electromotive force of the output winding is zero; when the sensor shaft is subjected to the load torque, the second excitation winding and The output winding is twisted through a certain space angle at the same time, and the initial position has changed relative to the action of no load torque. At this time, the pulsating magnetic flux generated by the excitation winding and the output winding turn chain are electromagnetically coupled, and the output winding generates a corresponding load torque. The induced electromotive force generated by the output winding can be made to have a highly linear relationship with the load torque by reasonably adjusting the number of turns of the two excitation windings and the number of turns of the output winding.
本发明的目的采取下述技术方案实现:The purpose of the present invention takes the following technical solutions to achieve:
一种高线性度分段激磁式扭矩传感器,主要包括传感器轴、内环铁心、第一段激磁绕组、补偿绕组、外环铁心、输出绕组和第二段激磁绕组;A segmented excitation torque sensor with high linearity, which mainly includes a sensor shaft, an inner ring core, a first excitation winding, a compensation winding, an outer ring core, an output winding, and a second excitation winding;
内环铁心的左端与传感器轴固定,内环铁心的右端通过轴承与传感器轴接触且可以相对传感器轴转动;The left end of the inner ring core is fixed to the sensor shaft, and the right end of the inner ring core is in contact with the sensor shaft through a bearing and can rotate relative to the sensor shaft;
外环铁心的右端与传感器轴固定,外环铁心的左端通过轴承与内环铁心接触且可以相对内环铁心转动;The right end of the outer ring core is fixed to the sensor shaft, and the left end of the outer ring core is in contact with the inner ring core through a bearing and can rotate relative to the inner ring core;
内环铁心设有绕组槽,第一段激磁绕组和补偿绕组嵌放在内环铁心绕组槽中,且第一段激磁绕组的轴线与补偿绕组的轴线在空间上互相垂直;The inner ring core is provided with a winding slot, and the first section of the excitation winding and the compensation winding are embedded in the inner ring core winding slot, and the axis of the first section of the excitation winding and the axis of the compensation winding are perpendicular to each other in space;
外环铁心设有绕组槽,第二段激磁绕组和输出绕组嵌放在外环铁心绕组槽中,且第二段激磁绕组的轴线与输出绕组的轴线在空间上互相垂直;The outer ring core is provided with a winding slot, the second field winding and the output winding are embedded in the outer ring core winding slot, and the axis of the second field winding and the axis of the output winding are perpendicular to each other in space;
无负载扭矩作用时,第一段激磁绕组的轴线与第二段激磁绕组的轴线在空间上位置相同,补偿绕组的轴线与输出绕组的轴线在空间上位置相同。When there is no load torque, the axis of the first excitation winding and the axis of the second excitation winding have the same position in space, and the axis of the compensation winding and the axis of the output winding have the same position in space.
嵌放在内环铁心中的第一段激磁绕组和嵌放在外环铁心中的第二段激磁绕组为串联方式连接,工作时通入正弦交流电压:The first excitation winding embedded in the inner ring core and the second excitation winding embedded in the outer ring core are connected in series, and a sinusoidal AC voltage is applied during operation:
嵌放在内环铁心中的补偿绕组的两端引出线直接短接;The lead wires at both ends of the compensation winding embedded in the inner ring core are directly shorted;
第二段激磁绕组的匝数与输出绕组的匝数相同。The number of turns of the second excitation winding is the same as that of the output winding.
第一段激磁绕组的匝数与输出绕组的匝数之间的比值为0.56-0.59之间。The ratio between the number of turns of the first stage excitation winding and the number of turns of the output winding is between 0.56-0.59.
如上述的结构,本发明的新型高线性度分段激磁式扭矩传感器,其工作原理为:As above-mentioned structure, novel high linearity subsection excitation type torque sensor of the present invention, its working principle is:
第一段激磁绕组和第二段激磁绕组串接后通入正弦交流电压,进而产生磁势幅值随时间变化的脉振磁场,经由外环铁心、空气隙和内环铁心形成闭合回路。传感器轴一端固定,另一端加载扭矩,当负载扭矩为零时,传感器轴不发生形变,分别与传感器轴两端固定的内环铁心和外环铁心的初始位置保持不变,固定于内环铁心的第一段激磁绕组和固定于外环铁心的输出绕组,其初始位置在空间上互差90°,固定于外环铁心的第二段激磁绕组和输出绕组,其初始位置在空间上互差90°,第一段激磁绕组的轴线与第二段激磁绕组的轴线在空间上的位置相同,补偿绕组的轴线与输出绕组的轴线在空间上的位置也相同,此时激磁磁场为直轴磁场,与输出绕组无交链,输出绕组产生的感应电动势为零;当负载扭矩不为零时,传感器轴发生形变,第二段激磁绕组和输出绕组同时扭转过一定的空间角度,相对初始位置发生改变,激磁绕组产生的激磁磁场与输出绕组交链,输出绕组产生相应的感应电动势,该感应电动势与传感器轴加载的负载扭矩相对应。The first section of excitation winding and the second section of excitation winding are connected in series, and a sinusoidal AC voltage is applied to generate a pulse vibration magnetic field whose magnetic potential amplitude changes with time, forming a closed loop through the outer ring core, air gap and inner ring core. One end of the sensor shaft is fixed, and the other end is loaded with torque. When the load torque is zero, the sensor shaft does not deform, and the initial positions of the inner ring core and the outer ring core fixed at both ends of the sensor shaft remain unchanged, and are fixed on the inner ring core. The initial positions of the first section of excitation winding and the output winding fixed on the outer ring core are 90° in space, and the initial positions of the second section of excitation winding and output winding fixed on the outer ring core are different in space 90°, the axis of the first excitation winding is in the same spatial position as the axis of the second excitation winding, and the axis of the compensation winding is in the same spatial position as the axis of the output winding. At this time, the excitation magnetic field is a direct axis magnetic field , there is no interlinkage with the output winding, and the induced electromotive force generated by the output winding is zero; when the load torque is not zero, the sensor shaft is deformed, and the second excitation winding and the output winding are twisted through a certain space angle at the same time, relative to the initial position. Change, the excitation magnetic field generated by the excitation winding is interlinked with the output winding, and the output winding generates a corresponding induced electromotive force, which corresponds to the load torque loaded on the sensor shaft.
此时第二段激磁绕组相对于初始位置转过一定的空间角度,第二段激磁绕组产生的脉振磁通存在交轴分量,由于补偿绕组直接短接,且补偿绕组的阻抗很小,根据楞次定律,补偿绕组产生与该交轴磁场对抗的磁场,保证传感器工作时的磁场基本只有直轴磁场。At this time, the second excitation winding rotates through a certain space angle relative to the initial position, and the pulsating magnetic flux generated by the second excitation winding has a quadrature axis component. Since the compensation winding is directly short-circuited, and the impedance of the compensation winding is very small, according to According to Lenz's law, the compensation winding generates a magnetic field against the quadrature-axis magnetic field to ensure that the magnetic field of the sensor is basically only the direct-axis magnetic field when it is working.
为了使传感器输出绕组产生的感应电动势与负载扭矩成高度的线性关系,第二段激磁绕组的匝数与输出绕组的匝数相同,且第一段激磁绕组的匝数和输出绕组的匝数比值应在0.56-0.59之间。In order to make the induced electromotive force generated by the output winding of the sensor have a highly linear relationship with the load torque, the number of turns of the second excitation winding is the same as the number of turns of the output winding, and the ratio of the number of turns of the first excitation winding to the number of turns of the output winding It should be between 0.56-0.59.
如上述的结构,本发明利用电磁感应原理构成的新型高线性度分段激磁式转矩传感器,传感器轴一端固定,一端与负载同轴安装,能够把负载扭矩转换成电信号输出,且输出绕组产生的电信号与负载扭矩呈高度对应的线性关系。As the above-mentioned structure, the present invention uses the principle of electromagnetic induction to form a new type of high linearity segmental excitation torque sensor. One end of the sensor shaft is fixed, and the other end is coaxially installed with the load, which can convert the load torque into an electrical signal output, and the output winding The resulting electrical signal is highly linear to the load torque.
附图说明Description of drawings
图1为本发明的高线性度分段激磁式扭矩传感器的结构示意图;Fig. 1 is the structural representation of high linearity segmental excitation type torque sensor of the present invention;
图2为图1的A-A面的剖视图;Fig. 2 is the sectional view of A-A plane of Fig. 1;
图3为本发明的扭矩传感器实施扭矩测量的工作原理图;Fig. 3 is the working principle figure that torque sensor of the present invention implements torque measurement;
图4为图2中补偿绕组的工作原理图。FIG. 4 is a working schematic diagram of the compensation winding in FIG. 2 .
具体实施方式Detailed ways
以下结合附图进一步描述本发明扭矩传感器的结构特征。The structural features of the torque sensor of the present invention will be further described below in conjunction with the accompanying drawings.
图1为本发明扭矩传感器的结构示意图,包括传感器轴1、轴承2、内环铁心3、第一段激磁绕组绕组4、补偿绕组5、外环铁心6、第二段激磁绕组7、输出绕组8和轴承9。Fig. 1 is a structural schematic diagram of a torque sensor of the present invention, including a sensor shaft 1, a bearing 2, an inner ring core 3, a first segment excitation winding winding 4, a compensation winding 5, an outer ring core 6, a second segment excitation winding 7, and an output winding 8 and bearing 9.
内环铁心3的左端与传感器轴1固定,内环铁心3的右端通过轴承2与传感器轴1接触且可以相对传感器轴1转动。The left end of the inner ring iron core 3 is fixed to the sensor shaft 1 , and the right end of the inner ring iron core 3 is in contact with the sensor shaft 1 through the bearing 2 and can rotate relative to the sensor shaft 1 .
外环铁心6的右端与传感器轴1固定,外环铁心6的左端通过轴承9与内环铁心3接触且可以相对内环铁心3转动。The right end of the outer ring core 6 is fixed to the sensor shaft 1 , and the left end of the outer ring core 6 is in contact with the inner ring core 3 through a bearing 9 and can rotate relative to the inner ring core 3 .
内环铁心3设有绕组槽,第一段激磁绕组4和补偿绕组5嵌放在内环铁心3绕组槽中。The inner ring core 3 is provided with a winding slot, and the first section of the excitation winding 4 and the compensation winding 5 are embedded in the winding slot of the inner ring core 3 .
外环铁心6设有绕组槽,第二段激磁绕组7和输出绕组8嵌放在外环铁心6的绕组槽中。The outer ring core 6 is provided with a winding slot, and the second section of the excitation winding 7 and the output winding 8 are embedded in the winding slot of the outer ring core 6 .
嵌放在内环铁心3中的第一段激磁绕组4和嵌放在外环铁心6中的第二段激磁绕组7为串联方式连接,工作时通入正弦交流电压。The first excitation winding 4 embedded in the inner ring core 3 and the second excitation winding 7 embedded in the outer ring core 6 are connected in series, and a sinusoidal AC voltage is applied during operation.
嵌放在内环铁心3中的补偿绕组5的两端引出线直接短接。Lead wires at both ends of the compensation winding 5 embedded in the inner ring core 3 are directly shorted.
嵌放在外环铁心6中第二段激磁绕组7的匝数与嵌放在外环铁心6中的输出绕组8的匝数相同。The number of turns of the second excitation winding 7 embedded in the outer ring core 6 is the same as the number of turns of the output winding 8 embedded in the outer ring core 6 .
嵌放在内环铁心3中的第一段激磁绕组4的匝数与嵌放在外环铁心6中的输出绕组8的匝数之间的比值为0.56-0.59之间。The ratio between the number of turns of the first excitation winding 4 embedded in the inner ring core 3 and the number of turns of the output winding 8 embedded in the outer ring core 6 is between 0.56-0.59.
传感器轴1的材料为碳钢或合金钢等材料;内环铁心3和外环铁心6由高磁导率的铁镍软磁合金片或高导磁性硅钢片冲剪叠压构成;第一段激磁绕组4、补偿绕组5、第二段激磁绕组7和输出绕组8均为直焊性聚氨酯漆包圆铜线。The material of the sensor shaft 1 is carbon steel or alloy steel; the inner ring core 3 and the outer ring core 6 are composed of high magnetic permeability iron-nickel soft magnetic alloy sheets or high magnetic permeability silicon steel sheets punched and laminated; the first section The excitation winding 4, the compensation winding 5, the second excitation winding 7 and the output winding 8 are all direct solderable polyurethane enamelled round copper wires.
图2为图1的A-A面的剖视图,包括传感器轴1、内环铁心3、第一段激磁绕组绕组4、补偿绕组5、外环铁心6、第二段激磁绕组7和输出绕组8。Fig. 2 is a sectional view of A-A plane of Fig. 1, including the sensor shaft 1, the inner ring core 3, the first excitation winding winding 4, the compensation winding 5, the outer ring core 6, the second excitation winding 7 and the output winding 8.
内环铁心3设有绕组槽,第一段激磁绕组4和补偿绕组5嵌放在内环铁心3绕组槽中,第一段激磁绕组4的轴线与补偿绕组5的轴线在空间上互相垂直。The inner ring core 3 is provided with a winding slot, and the first section of the field winding 4 and the compensation winding 5 are embedded in the winding slot of the inner ring core 3, and the axis of the first section of the field winding 4 and the axis of the compensation winding 5 are perpendicular to each other in space.
外环铁心6设有绕组槽,第二段激磁绕组7和输出绕组8嵌放在外环铁心6的绕组槽中,第二段激磁绕组7的轴线与输出绕组8的轴线在空间上互相垂直。The outer ring core 6 is provided with a winding slot, and the second section of the field winding 7 and the output winding 8 are embedded in the winding slot of the outer ring core 6, and the axis of the second section of the field winding 7 and the axis of the output winding 8 are perpendicular to each other in space .
无负载扭矩作用时,第一段激磁绕组4的轴线与第二段激磁绕组7的轴线在空间上位置相同,补偿绕组5的轴线与输出绕组8的轴线在空间上位置相同。When there is no load torque, the axis of the first field winding 4 and the axis of the second field winding 7 are in the same position in space, and the axis of the compensation winding 5 and the axis of the output winding 8 are in the same position in space.
本发明的高线性度分段激磁式扭矩传感器实施扭矩测量的工作原理如图3所示:第一段激磁绕组4的两端分别为L1和L2,第一段激磁绕组4用L1-L2来表示,补偿绕组5的两端分别为C1和C2,补偿绕组5用C1-C2来表示,第二段激磁绕组7的的两端分别为L3和L4,,第二段激磁绕组7用L1-L2来表示,输出绕组8的的两端分别为R1和R2,输出绕组8用R1-R2来表示。The working principle of the high linearity sub-excitation torque sensor of the present invention to implement torque measurement is shown in Figure 3: the two ends of the first section of the excitation winding 4 are respectively L1 and L2 , and the first section of the excitation winding 4 uses L1 -L 2 , the two ends of the compensation winding 5 are respectively C 1 and C 2 , the compensation winding 5 is represented by C 1 -C 2 , and the two ends of the second excitation winding 7 are L 3 and L 4 respectively, , the second excitation winding 7 is represented by L 1 -L 2 , the two ends of the output winding 8 are respectively R 1 and R 2 , and the output winding 8 is represented by R 1 -R 2 .
第一段激磁绕组L1-L2和第二段激磁绕组L3-L4通入交流电Uf后,分别产生脉振磁通Φ1和脉振磁通Φ2,经由内环铁心3、空气隙和外环铁心6形成闭合磁路。当传感器轴未受负载扭矩作用时,传感器的剖面图和对应的电路接线图如图3(a)所示,脉振磁通Φ1和脉振磁通Φ2都与输出绕组R1-R2、补偿绕组C1-C2无匝链,输出绕组R1-R2产生的感应电动势eo=0,补偿绕组C1-C2产生的感应电动势ec=0,图3(a)中的磁通Φ为脉振磁通Φ1和脉振磁通Φ2的合成磁通。After the first section of excitation winding L 1 -L 2 and the second section of excitation winding L 3 -L 4 are supplied with alternating current U f , they generate pulsed magnetic flux Φ 1 and pulsed magnetic flux Φ 2 respectively, which pass through the inner ring core 3, The air gap and the outer ring core 6 form a closed magnetic circuit. When the sensor shaft is not affected by the load torque, the cross-sectional view of the sensor and the corresponding circuit wiring diagram are shown in Figure 3 (a), the pulse vibration flux Φ 1 and the pulse vibration flux Φ 2 are connected to the output winding R 1 -R 2. The compensation winding C 1 -C 2 has no turn chain, the induced electromotive force e o =0 generated by the output winding R 1 -R 2 , and the induced electromotive force e c =0 generated by the compensation winding C 1 -C 2 , Figure 3(a) The magnetic flux Φ in is the composite magnetic flux of pulse vibration magnetic flux Φ 1 and pulse vibration magnetic flux Φ 2 .
当传感器轴受到负载扭矩作用时,传感器的剖面图和对应的电路接线图如图3(b)所示,输出绕组R1-R2相对图3(a)中的初始位置逆时针产生对应角位移θ,该角位移θ与所加负载扭矩存在一一对应关系,输出绕组R1-R2轴线与第一段激磁绕组L1-L2轴线的夹角为90-θ,则输出绕组R1-R2产生的感应电动势eo≠0。此外,第二段激磁绕组L3-L4同样逆时针转过θ角度,则第二段激磁绕组L3-L4产生的脉振磁通Φ2存在交轴分量,由于补偿绕组C1-C2直接短接,且补偿绕组C1-C2的阻抗很小,根据楞次定律,补偿绕组C1-C2感应电流产生的磁通基本上能够将第二段激磁绕组L3-L4产生的脉振磁通Φ2的交轴分量抵消,因此,传感器工作时的磁通可以近似认为只有直轴磁通Φ。When the sensor shaft is subjected to load torque, the cross-sectional view of the sensor and the corresponding circuit wiring diagram are shown in Figure 3(b), and the output windings R 1 -R 2 produce a corresponding angle counterclockwise relative to the initial position in Figure 3(a) Displacement θ, there is a one-to-one correspondence between the angular displacement θ and the applied load torque, the angle between the axis of the output winding R 1 -R 2 and the axis of the first section of the excitation winding L 1 -L 2 is 90-θ, then the output winding R The induced electromotive force e o ≠0 generated by 1 -R 2 . In addition, the second section of excitation winding L 3 -L 4 also rotates counterclockwise through the angle θ, then the pulsating magnetic flux Φ 2 generated by the second section of excitation winding L 3 -L 4 has a quadrature axis component, due to the compensation winding C 1 - C 2 is directly short-circuited, and the impedance of the compensation winding C 1 -C 2 is very small. According to Lenz's law, the magnetic flux generated by the induced current of the compensation winding C 1 -C 2 can basically drive the second segment of the excitation winding L 3 -L The quadrature axis component of the pulsating magnetic flux Φ generated by 4 cancels out, so the magnetic flux when the sensor is working can be approximately considered as only the direct axis magnetic flux Φ.
根据电磁感应定律,直轴脉振磁通Φ在第一段激磁绕组L1-L2中产生的感应电动势的有效值EL为:According to the law of electromagnetic induction, the effective value E L of the induced electromotive force generated in the first stage of the excitation winding L 1 -L 2 by the direct-axis pulsating magnetic flux Φ is:
EL=4.44fWfΦ (1)E L =4.44fW f Φ (1)
式中f为交流电压Uf的频率,Wf为第一段激磁绕组L1-L2匝数。In the formula, f is the frequency of the AC voltage U f , and W f is the number of turns of the first excitation winding L 1 -L 2 .
同理,直轴脉振磁通Φ在第二段激磁绕组L3-L4中产生感应电动势的有效值Em为:Similarly, the effective value E m of the induced electromotive force generated by the direct-axis pulsating magnetic flux Φ in the second section of the excitation winding L 3 -L 4 is:
Em=4.44fWmΦcosθ=kEL cosθ (2)E m =4.44fW m Φcosθ=kE L cosθ (2)
式中Wm为第二段激磁绕组L3-L4匝数,k=Wf/Wm为第一段激磁绕组L1-L2的匝数与第二段激磁绕组L3-L4的匝数的比值。In the formula, W m is the number of turns of the second excitation winding L 3 -L 4 , k=W f /W m is the number of turns of the first excitation winding L 1 -L 2 and the second excitation winding L 3 -L 4 The ratio of the number of turns.
设输出绕组的匝数同为Wm,直轴脉振磁通Φ在输出绕组R1-R2中产生感应电动势的有效值Eo为:Assuming that the number of turns of the output winding is the same as W m , the effective value E o of the induced electromotive force generated by the direct-axis pulsating magnetic flux Φ in the output winding R 1 -R 2 is:
Eo=4.44fWmΦcos(90-θ)=kELsinθ (3)E o =4.44fW m Φcos(90-θ)=kE L sinθ (3)
由于第一段激磁绕组L1-L2和第二段激磁绕组L3-L4串联,如果忽略两段激磁绕组的阻抗,根据基尔霍夫电压定律有:Since the first section of excitation winding L 1 -L 2 and the second section of excitation winding L 3 -L 4 are connected in series, if the impedance of the two sections of excitation winding is ignored, according to Kirchhoff's voltage law:
Uf=EL+Em=EL(1+kcosθ) (4)U f =E L +E m =E L (1+kcosθ) (4)
联立式(3)和式(4)可得:Simultaneous formula (3) and formula (4) can get:
由式(5)可知,输出绕组R1-R2产生的感应电动势的有效值Eo和负载扭矩产生的角位移θ存在一定的对应关系,即Eo和负载扭矩存在一定的对应关系。It can be seen from formula (5) that there is a certain correspondence between the effective value E o of the induced electromotive force generated by the output winding R 1 -R 2 and the angular displacement θ produced by the load torque, that is, there is a certain correspondence between E o and the load torque.
传感器的输出特性最好是线性,即理想输出特性为:The output characteristic of the sensor is preferably linear, that is, the ideal output characteristic is:
负载扭矩产生的角位移θ要在传感器轴的弹性范围内,度数较小,且此时负载扭矩与产生的角位移θ为线性关系。要为了达到式(6)的要求,经过数学公式推导,第一段激磁绕组L1-L2的匝数与输出绕组R1-R2的匝数之间的比值k=Wf/Wm为0.56-0.59之间,当k=Wf/Wm=0.57时,扭矩传感器标定得到的最大非线性误差约为0.26%,可以满足实际工程中扭矩测量的要求。The angular displacement θ generated by the load torque should be within the elastic range of the sensor shaft, and the degree is small, and at this time the load torque and the generated angular displacement θ have a linear relationship. In order to meet the requirements of formula (6), the ratio k=W f /W m between the number of turns of the first excitation winding L 1 -L 2 and the number of turns of the output winding R 1 -R 2 is deduced by the mathematical formula is between 0.56-0.59, when k=W f /W m =0.57, the maximum non-linear error obtained by torque sensor calibration is about 0.26%, which can meet the requirements of torque measurement in actual engineering.
本发明的扭矩传感器图2中补偿绕组5C1-C2的工作原理如图4所示:传感器轴1受到负载扭矩作用时,第二段激磁绕组L3-L4和输出绕组R1-R2同时相对于初始位置转过角度θ,假设第一段激磁绕组L1-L2和第二段激磁绕组L3-L4某瞬间激磁电流如图4所示,电流为左端流进,右端流出,则第二段激磁绕组L3-L4产生的脉振磁通Φ2存在交轴分量Φsq,根据楞次定律,补偿绕组C1-C2中会产生如图4所示感应电流,此感应电流产生磁通Φc,用于抵消第二段激磁绕组L3-L4产生的脉振磁通Φ2的交轴分量Φsq,从而保证传感器工作时的磁通基本只有直轴磁通Φ。The working principle of the compensation winding 5C 1 -C 2 in Fig. 2 of the torque sensor of the present invention is shown in Fig. 4: when the sensor shaft 1 is subjected to the load torque, the second section of the excitation winding L 3 -L 4 and the output winding R 1 -R 2 At the same time, the angle θ is rotated relative to the initial position, assuming that the excitation current of the first section of the excitation winding L 1 -L 2 and the second section of the excitation winding L 3 -L 4 is shown in Figure 4, the current flows in from the left end, and the right end flow out, the pulsating magnetic flux Φ 2 generated by the second excitation winding L 3 -L 4 has a quadrature axis component Φ sq , and according to Lenz's law, an induced current will be generated in the compensation winding C 1 -C 2 as shown in Figure 4 , the induced current generates magnetic flux Φ c , which is used to offset the quadrature-axis component Φ sq of the pulsating magnetic flux Φ 2 generated by the second excitation winding L 3 -L 4 , so as to ensure that the magnetic flux of the sensor basically only has the direct axis Magnetic flux Φ.
Claims (10)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201410258858.8A CN104034463B (en) | 2014-06-04 | 2014-06-04 | A High Linearity Segment Excitation Torque Sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201410258858.8A CN104034463B (en) | 2014-06-04 | 2014-06-04 | A High Linearity Segment Excitation Torque Sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN104034463A true CN104034463A (en) | 2014-09-10 |
| CN104034463B CN104034463B (en) | 2016-03-23 |
Family
ID=51465321
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201410258858.8A Expired - Fee Related CN104034463B (en) | 2014-06-04 | 2014-06-04 | A High Linearity Segment Excitation Torque Sensor |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN104034463B (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105372006A (en) * | 2015-12-11 | 2016-03-02 | 赵浩 | Vibration torque sensor calibration device and calibration method |
| TWI577977B (en) * | 2016-01-11 | 2017-04-11 | Rotatech Int Corp | Magnetic torque sensing device for steering system |
| TWI701109B (en) * | 2017-10-27 | 2020-08-11 | 日商富士金股份有限公司 | Hand tools, screwdrivers and torque sensors used in them |
Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60122341A (en) * | 1983-12-07 | 1985-06-29 | Shibaura Eng Works Co Ltd | Washer type magnetic sensor |
| DE4229554A1 (en) * | 1992-09-04 | 1994-03-10 | Friedhelm Prof Dr Ing Milde | Shaft torque measurement for three=phase AC asynchronous induction electric motor - using terminal voltages and currents, stator winding resistance, pole-pair number, and analog computation using double integrator |
| CN101252306A (en) * | 2008-01-11 | 2008-08-27 | 东南大学 | Hybrid excitation disc type eddy current transmission speed control device |
| CN103308226A (en) * | 2012-03-16 | 2013-09-18 | 株式会社捷太格特 | Stator of torque sensor |
| CN103968984A (en) * | 2014-05-13 | 2014-08-06 | 嘉兴学院 | Self-compensating brushless differential type torque sensor |
-
2014
- 2014-06-04 CN CN201410258858.8A patent/CN104034463B/en not_active Expired - Fee Related
Patent Citations (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60122341A (en) * | 1983-12-07 | 1985-06-29 | Shibaura Eng Works Co Ltd | Washer type magnetic sensor |
| DE4229554A1 (en) * | 1992-09-04 | 1994-03-10 | Friedhelm Prof Dr Ing Milde | Shaft torque measurement for three=phase AC asynchronous induction electric motor - using terminal voltages and currents, stator winding resistance, pole-pair number, and analog computation using double integrator |
| CN101252306A (en) * | 2008-01-11 | 2008-08-27 | 东南大学 | Hybrid excitation disc type eddy current transmission speed control device |
| CN103308226A (en) * | 2012-03-16 | 2013-09-18 | 株式会社捷太格特 | Stator of torque sensor |
| CN103968984A (en) * | 2014-05-13 | 2014-08-06 | 嘉兴学院 | Self-compensating brushless differential type torque sensor |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105372006A (en) * | 2015-12-11 | 2016-03-02 | 赵浩 | Vibration torque sensor calibration device and calibration method |
| CN105372006B (en) * | 2015-12-11 | 2017-11-28 | 嘉兴学院 | A kind of Vibration Torque sensor calibration apparatus and scaling method |
| TWI577977B (en) * | 2016-01-11 | 2017-04-11 | Rotatech Int Corp | Magnetic torque sensing device for steering system |
| TWI701109B (en) * | 2017-10-27 | 2020-08-11 | 日商富士金股份有限公司 | Hand tools, screwdrivers and torque sensors used in them |
Also Published As
| Publication number | Publication date |
|---|---|
| CN104034463B (en) | 2016-03-23 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US20070227268A1 (en) | Magnetostrictive torque sensor | |
| Meydan | Application of amorphous materials to sensors | |
| US11402237B2 (en) | Device, arrangement and method for characterizing the torsion, rotation and/or positioning of a shaft | |
| SE462873B (en) | DEVICE FOR CONTACT-FREE INDIRECT ELECTRICAL SEATING OF TORQUE IN AN AXLE | |
| US12098967B2 (en) | Torque and angle sensing device | |
| CN105698671B (en) | A kind of new angular displacement sensor | |
| CN104034463B (en) | A High Linearity Segment Excitation Torque Sensor | |
| CN210774488U (en) | Signal compensation circuit of magnetoelastic sensor | |
| CN105634235A (en) | Shaft sleeve generator capable of simultaneously measuring rotating angular speed and angular acceleration | |
| CN103968984B (en) | Self-compensating brushless differential type torque sensor | |
| CN1030642A (en) | Magnetically elastic torque sensor | |
| CN204043830U (en) | Based on the induction phase shift torch measuring system of FPGA | |
| CN105181195B (en) | Torque of rotating shaft and rotating speed measurement method | |
| CN114322726A (en) | Differential angular displacement sensor based on Hall effect and sensing method | |
| CN203837853U (en) | Self-compensating brushless differential torque sensor | |
| CN110657914A (en) | Signal compensation device for magnetoelastic sensor | |
| CN204854610U (en) | Device is sent in change of displacement sensor signal | |
| CN104122020B (en) | Sensing phase shift torch measuring system based on FPGA | |
| CN203949748U (en) | A kind of high linearity segmentation excitation type torque sensor | |
| US8844375B2 (en) | Mechanical force components sensing system and an associated method thereof for a magnetically encoded device | |
| CN201177540Y (en) | Non-contact type torque transducer | |
| CN205483350U (en) | Hall formula torque sensor | |
| Hao | A differential electromagnetic induction torque sensor and its finite element analysis | |
| EP3246684A1 (en) | Systems and methods for determining mechanical stress of machinery | |
| CN2033899U (en) | Magneto-elastic torque transmitter |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| C41 | Transfer of patent application or patent right or utility model | ||
| TA01 | Transfer of patent application right |
Effective date of registration: 20160204 Address after: 314001 Yuexiu South Road, Zhejiang, No. 56 Jiaxing University, Applicant after: Jiaxing University Address before: 314001 Yuexiu South Road, Zhejiang, No. 56 Jiaxing University, Applicant before: Jiaxing University Applicant before: Zhao Hao |
|
| C14 | Grant of patent or utility model | ||
| GR01 | Patent grant | ||
| CF01 | Termination of patent right due to non-payment of annual fee | ||
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20160323 Termination date: 20170604 |