阅读说明：本技术 测量非晶丝的环向磁滞回线的方法 (Method for measuring annular magnetic hysteresis loop of amorphous wire ) 是由 张济龙 许振丰 李学武 陈凯 徐玉峰 于 2020-03-27 设计创作，主要内容包括：本发明提供了一种测量非晶丝的环向磁滞回线的方法,包括：设置步骤：将待测的具有预定长度的非晶丝设置于四臂电桥中的一臂；信号施加步骤：经采样电阻对四臂电桥的输入端施加交流电压信号；采集步骤：采集四臂电桥的输出端的输出电压信号以及采样电阻两端的电压信号；以及处理步骤：对所采集的四臂电桥的输出电压信号和采样电阻两端的电压信号进行处理,以获得非晶丝的环向磁滞回线。(The invention provides a method for measuring a circumferential magnetic hysteresis loop of an amorphous wire, which comprises the following steps: the setting step: arranging an amorphous wire with a preset length to be measured on one arm of a four-arm bridge; a signal applying step: applying an alternating voltage signal to the input end of the four-arm bridge through the sampling resistor; the collection step comprises: acquiring output voltage signals of the output end of the four-arm bridge and voltage signals at two ends of the sampling resistor; and a processing step: and processing the acquired output voltage signals of the four-arm bridge and the voltage signals at two ends of the sampling resistor to obtain the annular magnetic hysteresis loop of the amorphous wire.)

1. A method for measuring a circumferential hysteresis loop of an amorphous wire comprises the following steps:

the setting step: arranging an amorphous wire with a preset length to be measured on one arm of a four-arm bridge;

a signal applying step: applying an alternating voltage signal to the input end of the four-arm bridge through a sampling resistor;

the collection step comprises: acquiring output voltage signals of the output end of the four-arm bridge and voltage signals at two ends of the sampling resistor; and

the processing steps are as follows: and processing the acquired output voltage signals of the four-arm bridge and the voltage signals at two ends of the sampling resistor to obtain the annular magnetic hysteresis loop of the amorphous wire.

2. The method of claim 1, further comprising:

and (3) balancing: after the amorphous wire is disposed in one of the four-arm bridges, the bridges of the four-arm bridge are adjusted such that the bridges of the four-arm bridge are balanced.

3. The method according to claim 2, wherein in the balancing step, a direct voltage is applied to input terminals of the four-arm bridge, a voltage of output terminals of the four-arm bridge is measured, and resistance values of variable resistors provided in the four-arm bridge are adjusted so that the voltage of the output terminals is zero, thereby balancing the bridges of the four-arm bridge.

4. The method of any one of claims 1-3, wherein the alternating voltage signal is applied to the four-arm bridge to generate an excitation current in the four-arm bridge,

the processing steps specifically include:

a magnetization calculation step of calculating the circumferential magnetization of the excitation current formed in the amorphous wire based on the acquired output voltage signal of the four-arm bridge,

a magnetic field intensity calculation step of calculating the circumferential magnetic field intensity of the excitation current formed in the amorphous wire based on the acquired voltage signals at the two ends of the sampling resistor, and

and an obtaining step of synthesizing a lissajous figure through the calculated magnetization intensity and the magnetic field intensity to obtain a circumferential hysteresis loop of the amorphous wire.

5. The method of claim 4, wherein the magnetization calculating step comprises calculating the hoop magnetization within the amorphous wire by numerically integrating the acquired output voltage signals of the four-arm bridge, and the hoop magnetization satisfies the following formula:

wherein, U₁(t) represents the result of numerical integration of the output voltage signal of the four-arm bridge at sampling time t, M (t) represents the toroidal magnetization at sampling time t, a represents the radius of the amorphous wire, L represents the length of the amorphous wire, K represents the circuit gain, μ₀The permeability in vacuum is indicated.

6. The method according to claim 4 or 5, wherein the magnetic field strength calculating step comprises calculating the toroidal magnetic field strength formed by the excitation current in the amorphous wire based on the acquired voltage signal across the sampling resistor and the resistance value of the sampling resistor, and the toroidal magnetic field strength satisfies the following formula:

wherein，U₂(t) represents a voltage signal across the sampling resistor at a sampling time t, h (t) represents a toroidal magnetic field strength at the sampling time t, R is a resistance value of the sampling resistor, and a is a radius of the amorphous wire.

7. The method according to any one of claims 4-6, wherein the calculated magnetization is taken as the horizontal axis and the calculated magnetic field strength is taken as the vertical axis to synthesize a lissajous diagram.

8. The method according to any one of claims 1-7, wherein the output voltage signal at the output of the four-arm bridge and the voltage signal across the sampling resistor are collected using an analog-to-digital converter.

9. The method of any of claims 1-8, wherein the processing step is performed using a processing device.

10. The method of any one of claims 1-9, wherein the applied alternating voltage signal is a sinusoidal voltage signal.

Technical Field

The invention relates to the technical field of sensors, in particular to a method for measuring a circumferential magnetic hysteresis loop of an amorphous wire.

Background

The amorphous wire metal soft magnetic material has a unique magnetic domain structure, shows obvious magnetic characteristics such as giant magneto-impedance effect and the like, is often used for manufacturing a high-precision magnetic sensor, and has very important influence on the overall performance of the sensor, particularly for a fluxgate sensor, the amorphous wire metal soft magnetic material utilizes a core-shell structure of the amorphous wire material to respond to the change of a magnetic field in an excitation state, so that the performance of a circumferential magnetic characteristic sensor probe of an amorphous wire magnetic core has important influence.

The magnetic hysteresis loop is a general method for describing the characteristics of the magnetic material, the annular magnetic hysteresis loop of the amorphous metal wire is obtained through measurement, the output characteristics, noise and other performances of the amorphous metal wire when the amorphous metal wire is applied to a fluxgate probe can be evaluated, and meanwhile, effective references can be provided for material type selection and heat treatment.

The traditional axial hysteresis loop measurement of the cylindrical magnetic material has a mature method and commercial equipment, but cannot be used for measuring the toroidal hysteresis loop, so that a method for measuring the toroidal hysteresis loop of the amorphous metal wire is needed and used for measuring and obtaining the toroidal hysteresis loop of the amorphous metal wire.

Disclosure of Invention

In view of the above, the present invention provides a method for measuring a toroidal hysteresis loop of an amorphous wire, in which the amorphous wire is placed in a four-arm bridge and excitation is applied to the bridge, and the output and excitation signals of the bridge are measured at the same time, so as to obtain the hysteresis loop through calculation, thereby evaluating the performance of a magnetic core by using the toroidal hysteresis loop measurement, and providing a basis for magnetic core selection and heat treatment.

According to an aspect of the present invention, there is provided a method of measuring a circumferential hysteresis loop of an amorphous wire, comprising: the setting step: arranging an amorphous wire with a preset length to be measured on one arm of a four-arm bridge; a signal applying step: applying an alternating voltage signal to the input end of the four-arm bridge through a sampling resistor; the collection step comprises: acquiring output voltage signals of the output end of the four-arm bridge and voltage signals at two ends of the sampling resistor; and a processing step: and processing the acquired output voltage signals of the four-arm bridge and the voltage signals at two ends of the sampling resistor to obtain the annular magnetic hysteresis loop of the amorphous wire.

Preferably, the method for measuring the circumferential hysteresis loop of the amorphous wire further comprises a balancing step: after the amorphous wire is disposed in one of the four-arm bridges, the bridges of the four-arm bridge are adjusted such that the bridges of the four-arm bridge are balanced.

Preferably, in the balancing step, a direct current voltage is applied to the input terminals of the four-arm bridge, the voltage of the output terminals of the four-arm bridge is measured, and the resistance value of the variable resistor provided in the four-arm bridge is adjusted so that the voltage of the output terminals is zero, thereby balancing the bridges of the four-arm bridge.

Preferably, the alternating voltage signal is applied to the four-arm bridge to generate an excitation current in the four-arm bridge, and the processing step specifically includes: calculating the circumferential magnetization intensity in the amorphous wire based on the acquired output voltage signals of the four-arm bridge, calculating the magnetic field intensity, calculating the circumferential magnetic field intensity formed by the excitation current in the amorphous wire based on the acquired voltage signals at two ends of the sampling resistor, and synthesizing a Lissajous diagram through the calculated magnetization intensity and the magnetic field intensity to obtain the circumferential hysteresis loop of the amorphous wire.

Preferably, the magnetization calculating step includes calculating the circumferential magnetization in the amorphous wire by numerically integrating the acquired output voltage signals of the four-arm bridge, and the circumferential magnetization satisfies the following formula:

wherein, U₁(t) represents the result of numerical integration of the output voltage signal of the four-arm bridge at sampling time t, M (t) represents the toroidal magnetization at sampling time t, a represents the radius of the amorphous wire, L represents the length of the amorphous wire, K represents the circuit gain, μ₀The permeability in vacuum is indicated.

Preferably, the magnetic field strength calculating step includes calculating the toroidal magnetic field strength formed by the excitation current in the amorphous wire based on the collected voltage signals at two ends of the sampling resistor and the resistance value of the sampling resistor, where the toroidal magnetic field strength satisfies the following formula:

wherein, U₂(t) represents a voltage signal across the sampling resistor at a sampling time t, h (t) represents a toroidal magnetic field strength at the sampling time t, R is a resistance value of the sampling resistor, and a is a radius of the amorphous wire.

Preferably, the calculated magnetization is taken as a horizontal axis and the calculated magnetic field strength is taken as a vertical axis to synthesize a lissajous diagram.

Preferably, an analog-to-digital converter is used for collecting an output voltage signal of the output end of the four-arm bridge and voltage signals at two ends of the sampling resistor.

Preferably, the processing step is performed using a processing device.

Preferably, the alternating voltage signal applied is a sinusoidal voltage signal.

Advantageous effects of the invention

According to the method for measuring the annular hysteresis loop of the amorphous wire, the amorphous wire is excited, output signals generated by the amorphous wire are collected and combined with the excitation signals for processing, so that the annular hysteresis loop curve of the amorphous wire is obtained, and the method can be used for the aspects of material selection, performance evaluation and the like; in addition, the adopted measuring method and measuring hardware are simpler, and the measuring method and the measuring hardware are convenient to use in actual measurement.

Further effects of the above-mentioned alternatives, which are not conventional, will be described in connection with the embodiments below

Drawings

The accompanying drawings, which are included to provide a further understanding of the invention and are incorporated in and constitute a part of this specification, illustrate embodiment(s) of the invention and together with the description serve to explain the invention without limiting the invention.

Fig. 1 is a schematic flow chart of a method of measuring a circumferential hysteresis loop of an amorphous wire according to an embodiment of the present invention.

Fig. 2 is a schematic diagram of an example of a measurement method including a balancing step.

Fig. 3 shows a schematic structural view of a more specific example of the measuring method according to the present invention.

Fig. 4 shows a lissajous diagram synthesized according to a more specific example of the measurement method of the present invention.

Detailed Description

The present invention will be described below based on examples, but the present invention is not limited to only these examples. In the following detailed description of the present invention, certain specific details are set forth. It will be apparent to one skilled in the art that the present invention may be practiced without these specific details. Well-known methods, procedures, and components have not been described in detail so as not to obscure the present invention.

The method for measuring the circumferential hysteresis loop of the amorphous wire of the invention is described with reference to fig. 1-4. Fig. 1 is a schematic flow chart of a method of measuring a circumferential hysteresis loop of an amorphous wire according to an embodiment of the present invention. Fig. 2 is a schematic diagram of an example of a measurement method including a balancing step. Fig. 3 shows a schematic structural diagram of a specific example of the measurement method according to the present invention. Fig. 4 shows a lissajous diagram synthesized according to a specific example of the measurement method of the present invention.

The invention provides a method for measuring a circumferential magnetic hysteresis loop of an amorphous wire, wherein the amorphous wire is made of an amorphous metal wire material.

The method for measuring the circumferential hysteresis loop of the amorphous wire according to the embodiment of the invention, as shown in fig. 1, comprises the following steps: a setting step S1, setting the amorphous wire with the preset length to be measured on one arm of the four-arm bridge; signal applying step S2: applying an alternating voltage signal to the input end of the four-arm bridge through the sampling resistor; an acquisition step S3, acquiring output voltage signals of the output end of the four-arm bridge and voltage signals at two ends of the sampling resistor; and a processing step S4, processing the acquired output voltage signal of the four-arm bridge and the voltage signals at the two ends of the sampling resistor to obtain a toroidal hysteresis loop of the amorphous wire.

Preferably, as shown in fig. 2, the method for measuring the circumferential hysteresis loop of the amorphous wire according to the embodiment of the present invention further includes a balancing step S5: after disposing the amorphous wire in one of the four-arm bridges, the bridges of the four-arm bridge are adjusted such that the bridges of the four-arm bridge are balanced.

By performing the balancing step described above, the applied excitation signal does not itself generate an output voltage at the bridge output. For example, if the magnetic core is a resistor, it has no magnetic property, and when the bridge is balanced, no output signal is generated at the output terminal. The balancing step described above is therefore able to eliminate the influence of the excitation signal itself.

Further preferably, in the balancing step S5, a direct current voltage is applied to the input terminals of the four-arm bridge, the voltage at the output terminals of the four-arm bridge is measured, and the resistance value of the variable resistor provided in the four-arm bridge is adjusted so that the voltage at the output terminals is zero, thereby balancing the bridges of the four-arm bridge.

A specific example of the above processing step S4 is described below. An alternating voltage signal is applied as an excitation source to the four-arm bridge to generate an excitation current in the four-arm bridge. The processing step S4 specifically includes: calculating the magnetization, namely calculating the circumferential magnetization formed by the excitation current in the amorphous wire based on the acquired output voltage signals of the four-arm bridge; calculating the magnetic field intensity, namely calculating the annular magnetic field intensity formed by the excitation current in the amorphous wire based on the acquired voltage signals at the two ends of the sampling resistor; and an obtaining step of synthesizing a lissajous figure through the calculated magnetization intensity and magnetic field intensity to obtain a circumferential hysteresis loop of the amorphous wire.

Further, the magnetization calculating step includes: calculating the circumferential magnetization in the amorphous wire by subjecting the acquired output voltage signals of the four-arm bridge to numerical integration, and the circumferential magnetization satisfies the following formula:

wherein, U₁(t) is in the process of extractionThe output voltage signal of the four-arm bridge at sample time t is subjected to numerical integration, M (t) represents the ring magnetization at the sample time t, a represents the radius of the amorphous wire, L represents the length of the amorphous wire, K represents the circuit gain, mu₀The permeability in vacuum is indicated.

More specifically, the circumferential magnetization is calculated, for example, by the following method:

1) for a cylindrical amorphous wire with the radius of a, let A be the magnetic vector potential, t be the time, and the electric field intensity at any point in the wire isWhen the magnetization M is constant, M has a relationship with the magnetic vector potential of A ═ mu₀M (a-r), where r is the radial distance from a point to the center of the cross-section, and the voltage across a wire of length L may be expressed as Is the average electric field intensity on the cross section of the wire, wherein,is the angle from a certain point on the section to the connecting line of the circle center in the coordinate system.

In summary, the relationship between the voltage U and the circumferential magnetization M of the amorphous wire with radius a and length L is:

2) for collected bridge output U₀(t) numerical integration gives:

wherein, U₀(t) represents the time of sampling obtained by sampling the voltage output from the bridge at predetermined equal time intervalsThe voltage value sequence of the bridge output of t; the output of the electric bridge is filtered and amplified through a circuit, and K is the circuit gain; u shape₁(t) represents the output voltage signal U of the four-arm bridge at the sampling time t₀(t) the result of numerical integration; mu.s₀Is a vacuum magnetic permeability.

3) Can be integrated from the voltage₁(t) calculating M (t):

where m (t) represents the circumferential magnetization at the sampling time t.

Further, the magnetic field strength calculating step may include: calculating the toroidal magnetic field intensity formed by the excitation current in the amorphous wire based on the acquired voltage signals at two ends of the sampling resistor and the resistance value of the sampling resistor, wherein the toroidal magnetic field intensity meets the following formula:

wherein, U₂(t) represents a voltage signal across the sampling resistor at a sampling time t, h (t) represents a toroidal magnetic field strength at the sampling time t, R is a resistance value of the sampling resistor, and a is a radius of the amorphous wire.

More specifically, the toroidal magnetic field strength is calculated, for example, by the following method:

1) the voltage signal U at two ends of the sampling resistor is measured₂(t) dividing the value by the value of the sampled resistance R and dividing the value by 2 to obtain the current I passing through the wire, wherein U₂(t) a voltage value sequence of the sampling resistor at the sampling time t is obtained by sampling the voltages at two ends of the sampling resistor at preset time intervals;

2) from the ampere-loop law in conductors

Therefore, the internal circumferential magnetic field intensity of the wire can be obtained

Where H (t) represents the toroidal magnetic field strength at the sampling time t, U₂(t) represents a voltage signal across the sampling resistor at sampling time t, R is the resistance of the sampling resistor, and a is the radius of the amorphous wire.

Preferably, the calculated magnetization M or μ₀M is plotted on the horizontal axis and the calculated magnetic field strength H is plotted on the vertical axis to synthesize a Lissajous diagram. Thereby, the toroidal hysteresis loop of the amorphous wire is obtained.

Preferably, an analog-to-digital converter is used to collect the output voltage signal at the output end of the four-arm bridge and the voltage signal at the two ends of the sampling resistor. The above-mentioned treatment step is preferably performed by a treatment apparatus. The applied alternating voltage signal is preferably a sinusoidal voltage signal.

A more specific example of the method of measuring the circumferential hysteresis loop of an amorphous wire according to the present invention is described with reference to fig. 3.

In the present example, the amorphous wire is, for example, a cobalt-based amorphous wire.

A cobalt-based amorphous wire 1 with the length of L-30 mm and the radius of a-70 mu m is placed on one arm of a four-arm bridge 10, a direct-current voltage is applied to the bridge by using a direct-current voltage/alternating-current voltage signal generating circuit 3, the voltage of the other two nodes of the bridge is measured, and the resistance value of a resistor 2 in the bridge is adjusted to zero, namely the bridge is balanced.

After the bridge circuit is leveled, a sine voltage is applied to the bridge circuit through the sampling resistor R, and simultaneously, the voltage U at the two ends of the sampling resistor R is collected by the analog-to-digital converter 6₂(t), the bridge output is filtered and amplified through an amplifying and filtering circuit 5, the circuit gain is K, and the amplified output voltage U is acquired through an analog-to-digital converter 6₀(t)。

Outputting U by means of a captured bridge in a processing device, such as an upper computer 4₀(t) calculating the circumferential magnetization M (t) in the wire by numerical integration.

In particular, for the collected electric bridgeGo out U₀(t) numerical integration gives:

from the voltage integral result U₁(t) calculating M (t):

voltage U obtained by the above steps₂(t) calculating the circumferential magnetic field intensity H (t) formed in the wire by the excitation current.

Specifically, the voltage U₂(t) dividing the sampling resistance value 2R by the current I passing through the wire material to obtain the inner annular magnetic field intensity of the wire material:

the magnetization M and the magnetic field strength H obtained by the above steps are synthesized into a Lissajous diagram (for example, as shown in FIG. 4) with the horizontal axis being H and the vertical axis being μ₀And M, forming a circumferential hysteresis curve of the measured amorphous metal wire.

The acquired signals are filtered, so that the obtained curve is smoother, the practical influence on the use of the hysteresis loop is not large, and finally the toroidal hysteresis loop similar to the attached drawing can be obtained. For shorter wire materials under test, no phase adjustment is generally required.

According to the method for measuring the annular hysteresis loop of the amorphous wire, the amorphous wire is excited, output signals generated by the amorphous wire are collected and combined with the excitation signals for processing, so that the annular hysteresis loop curve of the amorphous wire is obtained, and the method can be used for the aspects of material selection, performance evaluation and the like; in addition, the adopted measuring method and measuring hardware are simpler, and the measuring method and the measuring hardware are convenient to use in actual measurement.

Those skilled in the art will readily appreciate that the above-described preferred embodiments may be freely combined, superimposed, without conflict. The above exemplary embodiments are merely illustrative of the principles of the present invention and are not intended to limit the scope of the invention. Various modifications may be made by those skilled in the art without departing from the spirit and principles of the disclosure without departing from the scope thereof, which is defined by the claims.