CN113820033B - A temperature measurement method based on ferromagnetic resonance frequency - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及温度测量技术领域,具体涉及一种利用铁磁纳米粒子进行温度测量的方法。The invention relates to the technical field of temperature measurement, in particular to a temperature measurement method using ferromagnetic nanoparticles.
背景技术Background technique
温度是反映被测对象内部状态的重要指标,对其进行准确快速的测量在很多情况下非常重要。温度测量方法一般可分为接触式测温和非接触式测温,相比接触式测温,非接触式测温由于不会破坏被测对象的温度场,因而可以获得更为准确的测温结果。Temperature is an important indicator reflecting the internal state of the measured object, and its accurate and fast measurement is very important in many cases. Temperature measurement methods can generally be divided into contact temperature measurement and non-contact temperature measurement. Compared with contact temperature measurement, non-contact temperature measurement can obtain more accurate temperature measurement because it will not destroy the temperature field of the measured object. result.
铁磁纳米粒子因其独特的磁学性质已开始应用于多领域和多场合的温度测量,而且由于铁磁纳米粒子属于纳米级的,因而适于应用在非接触式的温度测量中,其基本原理是将铁磁纳米粒子加入被测对象内,例如注入人体内或材料内部或涂敷于材料表面,然后通过测量铁磁纳米粒子的一定物理量并基于所建立的数学模型计算出被测对象的温度信息。现有的铁磁纳米粒子的非接触式温度测量方法主要包括以下几种:Due to their unique magnetic properties, ferromagnetic nanoparticles have been used in temperature measurement in many fields and occasions, and because ferromagnetic nanoparticles are nanoscale, they are suitable for non-contact temperature measurement. The principle is to add ferromagnetic nanoparticles into the measured object, such as injecting into the human body or inside the material or coating on the surface of the material, and then calculate the measured object’s temperature by measuring a certain physical quantity of the ferromagnetic nanoparticles and based on the established mathematical model. temperature information. The existing non-contact temperature measurement methods of ferromagnetic nanoparticles mainly include the following:
1、基于铁磁纳米粒子在静态磁场下磁化后的磁化率倒数的温度依赖性进行温度测量,但该方法的测量时间较长,难以满足需要快速测温的应用需求。1. The temperature is measured based on the temperature dependence of the reciprocal of the magnetic susceptibility of ferromagnetic nanoparticles magnetized under a static magnetic field, but the measurement time of this method is long, which is difficult to meet the application requirements of rapid temperature measurement.
2、基于单频交流磁场激励下铁磁纳米粒子的磁化强度的温度依赖性进行温度测量,但该方法需要测铁磁纳米粒子磁化响应的高次谐波,增加了测量的难度。2. Temperature measurement is based on the temperature dependence of the magnetization of ferromagnetic nanoparticles excited by a single-frequency AC magnetic field, but this method needs to measure the higher harmonics of the magnetization response of ferromagnetic nanoparticles, which increases the difficulty of measurement.
3、基于铁磁纳米粒子磁化响应的齐次谐波或偶次谐波幅值与温度的关系进行温度测量,但相应的测温模型复杂,增加了测量和处理的复杂程度。3. Temperature measurement is based on the relationship between the homogeneous or even harmonic amplitude of the magnetization response of ferromagnetic nanoparticles and temperature, but the corresponding temperature measurement model is complex, which increases the complexity of measurement and processing.
发明内容Contents of the invention
为实现基于铁磁纳米粒子的简便快速的非接触式温度测量,本发明提供了一种基于铁磁共振频率的温度测量方法。In order to realize the simple and fast non-contact temperature measurement based on ferromagnetic nanoparticles, the invention provides a temperature measurement method based on ferromagnetic resonance frequency.
本发明提供的基于铁磁共振频率的温度测量方法,包括:The temperature measurement method based on the ferromagnetic resonance frequency provided by the present invention includes:
对包含铁磁纳米粒子的被测对象施加静磁场使铁磁纳米粒子饱和磁化;Apply a static magnetic field to the measured object containing ferromagnetic nanoparticles to saturate and magnetize the ferromagnetic nanoparticles;
沿所述静磁场的垂直方向施加交变脉冲激励磁场;applying an alternating pulse excitation magnetic field along the vertical direction of the static magnetic field;
通过扫频法确定所述铁磁纳米粒子发生铁磁共振时的铁磁共振频率;Determine the ferromagnetic resonance frequency when the ferromagnetic nanoparticles undergo ferromagnetic resonance by frequency sweep method;
根据所确定的所述铁磁共振频率计算出所述被测对象的温度,计算公式如下:Calculate the temperature of the measured object according to the determined ferromagnetic resonance frequency, the calculation formula is as follows:
其中,f是铁磁共振频率,单位为GHz,γe是电子的磁旋比,单位为GHz/T,kB是波尔兹曼常数,单位为J/K,M是所述铁磁纳米粒子被磁化后的未耦合的自由电子自旋的宏观磁化强度,单位为A/m,θ是所述宏观磁化强度的章动角,单位为rad,T为所述被测对象的温度,单位为K;Among them, f is the ferromagnetic resonance frequency in GHz, γ e is the magnetic gyro ratio of electrons in GHz/T, k B is Boltzmann's constant in J/K, and M is the ferromagnetic nanometer The macro-magnetization of the uncoupled free electron spins after the particles are magnetized, in A/m, θ is the nutation angle of the macro-magnetization, in rad, T is the temperature of the measured object, in is K;
所述宏观磁化强度由以下公式计算出:The macroscopic magnetization is calculated by the following formula:
其中,B是铁磁共振发生时所述铁磁纳米粒子内部的磁感应强度,由公式2πf=γeB计算出,单位为T,H0是所述静磁场的磁场强度,单位为A/m,μ0是真空磁导率,单位为Tm/A。Wherein, B is the magnetic induction intensity inside the ferromagnetic nanoparticles when ferromagnetic resonance occurs, calculated by the formula 2πf= γeB , and the unit is T, and H0 is the magnetic field intensity of the static magnetic field, and the unit is A/m , μ 0 is the vacuum permeability, the unit is Tm/A.
可选地,所述章动角由以下公式计算出:Optionally, the nutation angle is calculated by the following formula:
θ=γeB1Tp,θ=γ e B 1 T p ,
其中,B1是所述交变脉冲激励磁场的磁感应强度的幅值,单位为T,Tp是所述交变脉冲激励磁场的脉冲宽度,单位为ps。Wherein, B 1 is the amplitude of the magnetic induction intensity of the alternating pulse excitation magnetic field, and the unit is T, and T p is the pulse width of the alternating pulse excitation magnetic field, and the unit is ps.
可选地,所述施加静磁场采用永磁体、亥姆霍兹线圈或电磁铁。Optionally, permanent magnets, Helmholtz coils or electromagnets are used for applying the static magnetic field.
可选地,所述交变脉冲激励磁场为脉冲微波场或脉冲射频场。Optionally, the alternating pulse excitation magnetic field is a pulsed microwave field or a pulsed radio frequency field.
本发明提供的上述基于铁磁共振频率的温度测量方法,通过所构建的铁磁共振频率与温度的关系模型进行测温,该模型形式简单,测量方法简便,能够实现对被测对象内部温度的快速简便测量,并且具有很高的测量精确度。The above-mentioned temperature measurement method based on ferromagnetic resonance frequency provided by the present invention measures temperature through the constructed relationship model between ferromagnetic resonance frequency and temperature. Quick and easy measurement with high measurement accuracy.
根据下文结合附图对本发明的具体实施例的详细描述,本领域技术人员将会更加明了本发明的上述以及其他目的、优点和特征。According to the following detailed description of specific embodiments of the present invention in conjunction with the accompanying drawings, those skilled in the art will be more aware of the above and other objects, advantages and features of the present invention.
附图说明Description of drawings
后文将参照附图以示例性而非限制性的方式详细描述本发明的一些具体实施例。附图中相同的附图标记标示了相同或类似的部件或部分。本领域技术人员应该理解,这些附图未必是按比例绘制的。附图中:Hereinafter, some specific embodiments of the present invention will be described in detail by way of illustration and not limitation with reference to the accompanying drawings. The same reference numerals in the drawings designate the same or similar parts or parts. Those skilled in the art will appreciate that the drawings are not necessarily drawn to scale. In the attached picture:
图1为本发明一个实施例中,基于铁磁共振频率的温度测量方法的流程示意图;Fig. 1 is a schematic flow chart of a temperature measurement method based on a ferromagnetic resonance frequency in one embodiment of the present invention;
图2为本发明一个实施例中,测温设备的结构示意图;Fig. 2 is a schematic structural diagram of a temperature measuring device in one embodiment of the present invention;
图3为本发明一个仿真实例中,铁磁共振频率随温度的变化曲线;Fig. 3 is in a simulation example of the present invention, the variation curve of ferromagnetic resonance frequency with temperature;
图4为上述仿真实例中,由实测频率反演出的的f-T2曲线及与真实温度之间的对比图;Fig. 4 is in the above-mentioned simulation example, the fT2 curve and the comparison chart between the actual temperature inverted by the measured frequency;
图5为上述仿真实例中,测量误差随温度变化图。Figure 5 is a diagram of the measurement error changing with temperature in the above simulation example.
具体实施方式Detailed ways
为了使本技术领域的人员更好地理解本发明,下面将结合附图,对本发明实施例中的技术方案进行清楚、完整地描述。需要说明的是,在不冲突的情况下,本发明中的实施例及实施例中的特征可以相互组合。In order to enable those skilled in the art to better understand the present invention, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the accompanying drawings. It should be noted that, in the case of no conflict, the embodiments of the present invention and the features in the embodiments can be combined with each other.
现有研究证明铁磁纳米粒子的铁磁共振频率具有温度依赖性,并且铁磁共振频率也与外加磁场有关。本发明据此出发,以外加静磁场为条件,从原子自旋系统的自由能出发,经过分析、推导与测试构建出了铁磁共振频率与温度的关系模型,该模型形式简单,测量方法简便,能够实现对被测对象内部温度的快速简便测量,并且具有很高的测量精确度。Existing studies have proved that the ferromagnetic resonance frequency of ferromagnetic nanoparticles is temperature-dependent, and the ferromagnetic resonance frequency is also related to the external magnetic field. Based on this, the present invention starts from the free energy of the atomic spin system under the condition of an external static magnetic field, and builds a relationship model between ferromagnetic resonance frequency and temperature through analysis, derivation and testing. The model has a simple form and a simple and convenient measurement method. , can realize the quick and easy measurement of the internal temperature of the measured object, and has high measurement accuracy.
下文结合图1-5详细描述本发明基于铁磁共振频率的温度测量方法的具体实施例。图1所示为该方法的一个实例的步骤,图2所示为该方法的上述实例所用到的测温设备。该测温设备包括电磁铁1、微波源2、谐振腔3、微波环形器4、检波器5、锁相放大器6和计算机处理系统7。A specific embodiment of the ferromagnetic resonance frequency-based temperature measurement method of the present invention will be described in detail below with reference to FIGS. 1-5 . Figure 1 shows the steps of an example of the method, and Figure 2 shows the temperature measuring equipment used in the above example of the method. The temperature measuring equipment includes an
如图1所示,该方法包括:As shown in Figure 1, the method includes:
S01:对包含铁磁纳米粒子的被测对象施加静磁场使铁磁纳米粒子饱和磁化。S01: Apply a static magnetic field to the measured object containing ferromagnetic nanoparticles to saturate and magnetize the ferromagnetic nanoparticles.
如图2所示,本实施例中,选用电磁铁1作为静磁场施加装置,在其他实施例中,静磁场施加装置也可选用永磁体或亥姆霍兹线圈等。可选择粒径为5-10nm的铁磁材料纳米粒子,铁磁材料例如为Fe3O4等铁氧体材料。铁磁纳米粒子加入被测对象的方式依实际情况而定,例如针对人体测温时,可以将铁磁纳米粒子用有机物分子包裹制作成造影剂,皮下注入人体;再如对某种材料测温时,可以将铁磁纳米粒子涂覆到待测材料表面。As shown in FIG. 2 , in this embodiment, the
S02:沿静磁场的垂直方向施加交变脉冲激励磁场。S02: Apply an alternating pulse excitation magnetic field along the vertical direction of the static magnetic field.
交变脉冲激励磁场由电磁波源产生,本实施例中,交变脉冲激励磁场为脉冲微波场,由微波源2产生。谐振腔3放置在电磁铁1的两个极头之间,被测对象则置于谐振腔3中。微波源2产生的脉冲微波,经微波环形器4,以垂直于静磁场的方向施加于被测对象,即该交变脉冲激励磁场的方向垂直于该静磁场的方向。在其他实施例中,可以用脉冲射频场替代脉冲微波场作为交变脉冲激励磁场。The alternating pulse excitation magnetic field is generated by an electromagnetic wave source. In this embodiment, the alternating pulse excitation magnetic field is a pulse microwave field, which is generated by the
S03:通过扫频法确定铁磁纳米粒子发生铁磁共振时的铁磁共振频率。S03: Determine the ferromagnetic resonance frequency when the ferromagnetic nanoparticles undergo ferromagnetic resonance by frequency sweep method.
具体来说,此步骤中,在所施加的静磁场保持恒定的情况下,改变微波频率,谐振腔3内的反射功率经微波环形器4进入检波器5,当发生铁磁共振时,铁磁纳米粒子会吸收一部分微波功率,从而导致反射功率降低,检波器5检测出频率扫描过程中每个微波频率对应的反射功率的幅值信号,并将其转换为直流电压信号。该直流电压信号经过锁相放大器6放大后,记录在计算机处理系统7内。由于当发生铁磁共振时,对微波的吸收达到最大,因此当直流电压的幅值降到最低时,所对应的微波频率即为铁磁共振频率。因铁磁共振频率的扫频法检测属于现有技术,故此处仅作示例性简要说明。Specifically, in this step, when the applied static magnetic field remains constant, the microwave frequency is changed, and the reflected power in the
S04:根据所确定的铁磁共振频率计算出被测对象的温度,计算公式如下:S04: Calculate the temperature of the measured object according to the determined ferromagnetic resonance frequency, the calculation formula is as follows:
其中,f是铁磁共振频率,单位为GHz,γe是电子的磁旋比,单位为GHz/T,kB是波尔兹曼常数,单位为J/K,M是铁磁纳米粒子被磁化后的未耦合的自由电子自旋的宏观磁化强度,通过铁磁共振频率计算得出,单位为A/m,θ是宏观磁化强度的章动角,可由交变脉冲激励磁场磁感应强度的幅值和脉冲宽度计算得出,单位为rad(弧度)。由此可见,上述参数均已知,通过上述公式即可计算出被测对象内部的单位为K的绝对温度T。Among them, f is the ferromagnetic resonance frequency in GHz, γ e is the magnetic gyro ratio of electrons in GHz/T, k B is the Boltzmann constant in J/K, M is the ferromagnetic nanoparticle The macroscopic magnetization of the uncoupled free electron spins after magnetization is calculated by ferromagnetic resonance frequency, and the unit is A/m. θ is the nutation angle of the macroscopic magnetization. Value and pulse width calculated in rad (radians). It can be seen that the above parameters are all known, and the absolute temperature T inside the measured object in K can be calculated through the above formula.
宏观磁化强度由以下公式计算出:The macroscopic magnetization is calculated by the following formula:
其中,B是铁磁共振发生时铁磁纳米粒子内部的磁感应强度,由外加静磁场和交变脉冲激励磁场共同决定,可由铁磁共振条件,即2πf=γeB算出,单位为T,H0是外加静磁场的磁场强度,单位为A/m,μ0是真空磁导率,单位为Tm/A。Among them, B is the magnetic induction intensity inside the ferromagnetic nanoparticles when the ferromagnetic resonance occurs, which is determined by the external static magnetic field and the alternating pulse excitation magnetic field, and can be calculated by the ferromagnetic resonance condition, that is, 2πf=γ e B, and the unit is T, H 0 is the magnetic field strength of the external static magnetic field, the unit is A/m, μ 0 is the vacuum permeability, the unit is Tm/A.
在本实施例中,章动角由以下公式计算出:In this embodiment, the nutation angle is calculated by the following formula:
θ=γeB1Tp θ=γ e B 1 T p
其中,B1是交变脉冲激励磁场磁感应强度的幅值,单位为T,Tp是交变脉冲激励磁场的脉冲宽度,单位为ps(皮秒)。Among them, B 1 is the amplitude of the magnetic induction intensity of the alternating pulse excitation magnetic field, and the unit is T, and T p is the pulse width of the alternating pulse excitation magnetic field, and the unit is ps (picosecond).
仿真实例Simulation example
为了验证上述基于铁磁共振频率的温度测量方法的可行性,发明人根据发明内容设计了仿真实验对该方法进行了反复验证,下面通过一个具体实例进行说明:In order to verify the feasibility of the above-mentioned temperature measurement method based on ferromagnetic resonance frequency, the inventor designed a simulation experiment according to the content of the invention to repeatedly verify the method. A specific example is used to illustrate:
将加入铁磁纳米粒子的被测对象放入磁感应强度为μ0H0=2T的静磁场中。The measured object added with ferromagnetic nanoparticles is placed in a static magnetic field with a magnetic induction intensity of μ 0 H 0 =2T.
通过微波源产生一定磁感应强度幅值μ0H1=10-4T的微波脉冲激励,脉冲宽度Tp控制在1.5ps,通过微波环形器,在与静磁场垂直的方向,施加微波脉冲激励,在静磁场磁场强度H0的大小不变的情况下,不断改变微波频率f,通过检波器检测共振吸收信号,检测到铁磁共振发生时铁磁纳米粒子的铁磁共振频率f。电子的旋磁比γe可由下式计算:A microwave pulse excitation with a certain magnetic induction intensity amplitude μ 0 H 1 =10 -4 T is generated by a microwave source, and the pulse width T p is controlled at 1.5 ps. The microwave pulse excitation is applied in a direction perpendicular to the static magnetic field through a microwave circulator. Under the condition that the magnitude of the static magnetic field strength H0 is constant, the microwave frequency f is constantly changed, and the resonant absorption signal is detected by the detector, and the ferromagnetic resonance frequency f of ferromagnetic nanoparticles is detected when ferromagnetic resonance occurs. The gyromagnetic ratio γ e of the electron can be calculated by the following formula:
其中,g为朗德因子,这里取g=2,me为电子的质量,e为电子电荷,这里取γe=1.76×107rad/(s·Oe)=176GHz/T。Wherein, g is the Landes factor, here g=2, m e is the mass of the electron, e is the charge of the electron, here γ e =1.76×10 7 rad/(s·Oe)=176GHz/T.
然后取μ0=1.26×10-6Tm/A,计算出M的值。Then take μ 0 =1.26×10 -6 Tm/A to calculate the value of M.
取kB=1.38×10-23J/K,θ由微波磁感应强度幅值μ0H1和脉冲宽度Tp计算出,将被测对象升温至373K,然后自然冷却,由温敏传感器实时记录被测对象温度T,每降5K,调节微波频率使其达到铁磁共振,记录铁磁共振频率f,直至温度下降到260K;然后将测得的f分别代入公式,经计算可反演出对应于各个频率的温度T2,根据所得的这些点,分别画出铁磁共振频率f随温度T变化曲线,如图3,以及反演出的f-T2曲线,如图4,将T2与标准温度T做对比,即可得误差ε=|T2-T|,如图5,可以看出该模型绝对误差小于0.05K。Take k B = 1.38×10 -23 J/K, θ is calculated from the amplitude of microwave magnetic induction intensity μ 0 H 1 and pulse width T p , the temperature of the measured object is raised to 373K, then cooled naturally, and recorded by the temperature sensitive sensor in real time When the temperature T of the measured object drops by 5K, adjust the microwave frequency to make it reach ferromagnetic resonance, and record the ferromagnetic resonance frequency f until the temperature drops to 260K; The temperature T 2 of each frequency, according to these obtained points, draw the curve of the ferromagnetic resonance frequency f with the temperature T, as shown in Figure 3, and the inverted fT 2 curve, as shown in Figure 4, compare T 2 with the standard temperature T For comparison, the error ε=|T 2 -T| can be obtained, as shown in Figure 5, it can be seen that the absolute error of the model is less than 0.05K.
从本发明提供的上述实施例及仿真实例可以看出,本发明提供了一种利用铁磁纳米粒子进行非接触式测温的新思路、新方法,与以往的测温模型比,本发明从铁磁共振频率角度出发建立的温度模型形式简单,仅需要测量铁磁共振频率即可计算出被测对象的温度,测量方法简单,容易实现。经验证,本发明所采用的测温模型具有很高的测温精度,在信噪比为90分贝以上时,具有良好的抗噪性能。It can be seen from the above-mentioned embodiments and simulation examples provided by the present invention that the present invention provides a new idea and new method for non-contact temperature measurement using ferromagnetic nanoparticles. Compared with the previous temperature measurement model, the present invention starts from The temperature model established from the perspective of ferromagnetic resonance frequency is simple in form, and the temperature of the measured object can be calculated only by measuring the ferromagnetic resonance frequency. The measurement method is simple and easy to implement. It has been verified that the temperature measurement model adopted in the present invention has high temperature measurement accuracy, and has good anti-noise performance when the signal-to-noise ratio is above 90 decibels.
以上所述,仅为本发明较佳的具体实施方式,但本发明的保护范围并不局限于此,任何熟悉本技术领域的技术人员在本发明揭露的技术范围内,可轻易想到的变化或替换,都应涵盖在本发明的保护范围之内。因此,本发明的保护范围应该以权利要求的保护范围为准。The above is only a preferred embodiment of the present invention, but the scope of protection of the present invention is not limited thereto. Any person skilled in the art within the technical scope disclosed in the present invention can easily think of changes or Replacement should be covered within the protection scope of the present invention. Therefore, the protection scope of the present invention should be determined by the protection scope of the claims.
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