CN108896664A - The velocity of sound and attenuation coefficient integrated detection method in a kind of polymer - Google Patents

The velocity of sound and attenuation coefficient integrated detection method in a kind of polymer Download PDF

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CN108896664A
CN108896664A CN201810573609.6A CN201810573609A CN108896664A CN 108896664 A CN108896664 A CN 108896664A CN 201810573609 A CN201810573609 A CN 201810573609A CN 108896664 A CN108896664 A CN 108896664A
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CN108896664B (en
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赵朋
夏能
赵耀
张剑锋
黄俊业
傅建中
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Zhejiang University ZJU
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/04Analysing solids
    • G01N29/11Analysing solids by measuring attenuation of acoustic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N29/00Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object
    • G01N29/04Analysing solids
    • G01N29/07Analysing solids by measuring propagation velocity or propagation time of acoustic waves
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
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    • G01N2291/01Indexing codes associated with the measuring variable
    • G01N2291/011Velocity or travel time
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
    • G01N2291/01Indexing codes associated with the measuring variable
    • G01N2291/015Attenuation, scattering
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    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2291/00Indexing codes associated with group G01N29/00
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Abstract

本发明公开了一种聚合物中声速与衰减系数一体化检测方法,其特征在于,包括:(1)将超声探头正对待检测样品发射超声波;(2)采集样品上下表面的反射回波,求取反射回波的幅值谱,所述样品正对超声探头的一侧定义为上表面,背对的一侧为下表面;(3)根据得到的反射回波的幅值谱,求得待检测样品的超声传播速度、样品的厚度以及样品的衰减系数。本发明检测方法操作简单,计算方便,检测成本低廉,不破坏被测样品,易于实现在线监测,可以同时检测聚合物零件的声速、衰减系数、壁厚。

The invention discloses a method for integrated detection of sound velocity and attenuation coefficient in polymers, which is characterized in that it comprises: (1) sending an ultrasonic probe facing a sample to be detected; Get the amplitude spectrum of the reflected echo, the side of the sample facing the ultrasonic probe is defined as the upper surface, and the side facing away from it is the lower surface; (3) according to the amplitude spectrum of the obtained reflected echo, obtain the Detect the ultrasonic propagation velocity of the sample, the thickness of the sample and the attenuation coefficient of the sample. The detection method of the invention is simple in operation, convenient in calculation, low in detection cost, does not damage the sample to be tested, is easy to realize on-line monitoring, and can simultaneously detect the sound velocity, attenuation coefficient and wall thickness of polymer parts.

Description

一种聚合物中声速与衰减系数一体化检测方法An integrated detection method of sound velocity and attenuation coefficient in polymer

技术领域technical field

本发明属于检测方法技术领域,具体是涉及一种聚合物中声速与衰减系数一体化检测方法。The invention belongs to the technical field of detection methods, and in particular relates to an integrated detection method of sound velocity and attenuation coefficient in polymers.

背景技术Background technique

聚合物零件多采用注塑方式成型,超声波在其中的传播速度和衰减系数是其微观结构的重要表征指标。声速可以表征聚合物零件的结晶度和取向度,衰减系数与结晶零件的晶粒粒度紧密关联。针对聚合物零件的声速,目前主要采用渡越时间法测量,即测量零件的壁厚以及超声波传播时间计算声速;针对衰减系数,目前主要是根据回波信号的幅值结合衰减系数定义进行计算。这些检测方式具有以下缺点:Polymer parts are mostly formed by injection molding, and the propagation speed and attenuation coefficient of ultrasonic waves in them are important indicators of their microstructure. The speed of sound can characterize the degree of crystallinity and orientation of polymer parts, and the attenuation coefficient is closely related to the grain size of crystalline parts. For the sound velocity of polymer parts, currently the transit time method is mainly used to measure the sound velocity, that is, to measure the wall thickness of the part and the ultrasonic propagation time to calculate the sound velocity; for the attenuation coefficient, the current calculation is mainly based on the amplitude of the echo signal combined with the definition of the attenuation coefficient. These detection methods have the following disadvantages:

(1)渡越时间法需要已知被测聚合物的壁厚,该方法不能用于聚合物注塑过程的在线监测。(1) The transit time method needs to know the wall thickness of the polymer to be tested, and this method cannot be used for online monitoring of the polymer injection molding process.

(2)根据回波信号幅值计算衰减系数,所利用信息少且声压幅值受干扰因素众多,计算精度低。(2) Calculating the attenuation coefficient based on the amplitude of the echo signal requires less information and the amplitude of the sound pressure is disturbed by many factors, so the calculation accuracy is low.

发明内容Contents of the invention

本发明针对现有检测方式的问题,基于超声传播理论,提出了一种超声波声速与衰减系数的一体化检测方法,可用于在线监测,精度高。Aiming at the problems of the existing detection methods, the present invention proposes an integrated detection method of ultrasonic sound velocity and attenuation coefficient based on the ultrasonic propagation theory, which can be used for online monitoring and has high precision.

一种聚合物中声速与衰减系数一体化检测方法,包括如下步骤:An integrated detection method for sound velocity and attenuation coefficient in a polymer, comprising the following steps:

(1)将超声探头正对待检测样品发射超声波;(1) The ultrasonic probe is facing the sample to be tested to emit ultrasonic waves;

(2)采集样品上下表面的反射回波,求取反射回波的幅值谱,所述样品正对超声探头的一侧定义为上表面,背对的一侧为下表面;(2) collect the reflected echoes of the upper and lower surfaces of the sample, and obtain the amplitude spectrum of the reflected echoes, the side of the sample facing the ultrasonic probe is defined as the upper surface, and the side facing away from it is the lower surface;

(3)根据得到的反射回波的幅值谱,求得待检测样品的超声传播速度、样品的厚度以及样品的衰减系数。(3) According to the obtained amplitude spectrum of the reflected echo, the ultrasonic propagation velocity of the sample to be tested, the thickness of the sample and the attenuation coefficient of the sample are obtained.

作为优选,步骤(3)中,具体包括:As preferably, in step (3), specifically include:

(3-1)对得到的幅值谱H(f)求对数;其中U1(f)为上表面反射回波的频谱,U2(f)为下表面反射回波的频谱;(3-1) find the logarithm to the amplitude spectrum H (f) that obtains; Wherein U 1 (f) is the spectrum of the echo reflected from the upper surface, and U 2 (f) is the spectrum of the echo reflected from the lower surface;

(3-2)求取反射回波的幅值谱的对数与频率f的关系图,并对其进行线性拟合得到线性函数关系图;其中,f为离散频率;(3-2) obtain the relation diagram of the logarithm of the amplitude spectrum of the reflection echo and the frequency f, and carry out linear fitting to it to obtain the linear function relation diagram; Wherein, f is the discrete frequency;

(3-3)求取得到的线性函数关系图的纵轴截距D,根据下式求取超声波在待检测样品的传播速度c:(3-3) Find the vertical axis intercept D of the linear function diagram obtained, and obtain the propagation velocity c of the ultrasonic wave at the sample to be tested according to the following formula:

Z=ρcZ = ρc

D=lnKD=lnK

上述式中:Z0为待检测样品上表面与超声探头之间介质的声阻抗,Z为待检测样品的声阻抗,ρ为待检测样品的密度,c为超声波在待检测样品的传播速度;In the above formula: Z0 is the acoustic impedance of the medium between the upper surface of the sample to be tested and the ultrasonic probe, Z is the acoustic impedance of the sample to be tested, ρ is the density of the sample to be tested, and c is the propagation velocity of ultrasonic waves in the sample to be tested;

(3-4),通过上下表面反射回波的时间差Δt计算样品的厚度x,其表达式如下:(3-4), the thickness x of the sample is calculated by the time difference Δt of the reflected echoes on the upper and lower surfaces, and its expression is as follows:

x=c×Δt/2x=c×Δt/2

(3-5)求取得到的线性函数关系图的斜率k,根据k=-2mxα÷fc,求得衰减系数α;其中m=0.115为衰减系数单位由dB/cm转化为Np/cm的系数,fc为超声探头的中心频率。(3-5) Find the slope k of the obtained linear function diagram, and obtain the attenuation coefficient α according to k=-2mxα÷f c ; wherein m=0.115 is the unit of the attenuation coefficient converted from dB/cm to Np/cm Coefficient, f c is the center frequency of the ultrasonic probe.

本发明中,所述的f为离散频率,具体讲在接收超声回波时按照一定的采样频率fs和采样点数:2N进行采样,f就是0-fs之间的离散值,步长为fs/2N,也就说f表示一系列离散的频率:0,fs/2N,(fs/2N)*2,(fs/2N)*2*2,......,fsIn the present invention, said f is a discrete frequency, specifically when receiving ultrasonic echoes, according to a certain sampling frequency f s and sampling points: 2 N for sampling, f is exactly the discrete value between 0-f s , step size It is f s /2 N , that is to say, f represents a series of discrete frequencies: 0, f s /2 N , (f s /2 N )*2, (f s /2 N )*2*2,.. ...., f s .

本发明可以对离线样品(零件)进行检测,作为优选,所述样品为离线样品,检测前将所述样品置于介质液中,检测时,所述超声探头浸渍于所述介质液中,所述Z0为介质液的声阻抗。The present invention can detect off-line samples (parts), preferably, the sample is an off-line sample, and the sample is placed in a medium liquid before detection, and during detection, the ultrasonic probe is immersed in the medium liquid, and the Z 0 is the acoustic impedance of the medium liquid.

所述介质液充当耦合剂,用于保证超声波能够有效进入被测样品。所述耦合剂为水或者甘油、机油等。The medium liquid acts as a coupling agent to ensure that the ultrasonic wave can effectively enter the sample to be tested. The coupling agent is water or glycerin, machine oil and the like.

本发明也可以用于在线样品的检测,作为优选,所述样品为在线样品,所述超声探头紧贴在线样品外侧的模腔侧壁,所述Z0为所述模腔侧壁的声阻抗。可选择的,可在超声探头与模腔侧壁之间涂抹所述的耦合剂,以提高检测精度。The present invention can also be used for the detection of online samples, as preferably, the sample is an online sample, the ultrasonic probe is close to the mold cavity side wall outside the online sample, and the Z 0 is the acoustic impedance of the mold cavity side wall . Optionally, the coupling agent can be applied between the ultrasonic probe and the side wall of the mold cavity to improve detection accuracy.

作为优选,所述待检测样品为表面平整的聚合物物品,比如可以为离线的塑料件或者在线的采用注塑成型的塑料件样品等。Preferably, the sample to be tested is a polymer object with a flat surface, such as an offline plastic part or an online injection-molded plastic sample.

以检测离线塑料件,并且采用水为介质液为例,上述基于超声传播理论的声速和衰减系数的一体化检测方法,其原理如下:超声波在塑料零件中传播时,会在塑料上下表面产生回波信号,上下表面回波信号之间的关系由传递函数决定:Taking the detection of offline plastic parts and using water as the medium liquid as an example, the above-mentioned integrated detection method of sound velocity and attenuation coefficient based on the ultrasonic propagation theory works as follows: when ultrasonic waves propagate in plastic parts, echoes will be generated on the upper and lower surfaces of the plastic. Wave signal, the relationship between the upper and lower surface echo signals is determined by the transfer function:

其中H(f)为传递函数(即回波幅值谱),U1(f)为上表面回波的频谱(U1(f)=FT(u1(t))),U2(f)为下表面回波的频谱。H(f)与介质的密度、声速、衰减系数有关:Where H(f) is the transfer function (i.e. the echo amplitude spectrum), U 1 (f) is the spectrum of the upper surface echo (U 1 (f)=FT(u 1 (t))), U 2 (f ) is the spectrum of the subsurface echo. H(f) is related to the density, sound velocity and attenuation coefficient of the medium:

式中:Z0为水的声阻抗,Z为塑料零件的声阻抗,Z=ρc,ρ为塑料的密度,c为超声波在塑料中的传播速度。m=0.115为衰减系数单位由dB/cm转化为Np/cm的系数。x为塑料零件厚度,α为衰减系数,fc为超声探头的中心频率,f为离散频率(比如采集数据的时候采样频率是50MHz,采样点数是128个点,那这个f就表示用128个点将0-50MHz平均等分的离散频率值)。Φ1(f),Φ2(f)分别为上下表面反射回波的相位谱。对传递函数等式两边同时取对数可得:In the formula: Z 0 is the acoustic impedance of water, Z is the acoustic impedance of plastic parts, Z=ρc, ρ is the density of plastic, and c is the propagation speed of ultrasonic wave in plastic. m=0.115 is the coefficient for converting the attenuation coefficient unit from dB/cm to Np/cm. x is the thickness of the plastic part, α is the attenuation coefficient, f c is the center frequency of the ultrasonic probe, f is the discrete frequency (for example, when collecting data, the sampling frequency is 50MHz, and the number of sampling points is 128 points, then this f means to use 128 Points divide 0-50MHz into equal equal parts for discrete frequency values). Φ 1 (f), Φ 2 (f) are the phase spectra of the reflected echoes from the upper and lower surfaces, respectively. Take the logarithm on both sides of the transfer function equation at the same time:

其中|H(f)|表示对H(f)取模;Where |H(f)| means to take the modulus of H(f);

当作出f-ln|H(f)|曲线时,lnK为纵轴截距,-2mxa÷fc为斜率。因此得到样品的上下表面回波后,可以作出回波幅值谱的对数与频率的关系图,并对其进行线性拟合得到线性函数关系。通过该拟合直线得到K值,进而可以计算出超声传播速度c,通过上下表面反射回波的时间差计算壁厚,其表达式如下:When making the f-ln|H(f)| curve, lnK is the intercept of the vertical axis, and -2mxa÷f c is the slope. Therefore, after obtaining the upper and lower surface echoes of the sample, the logarithm of the echo amplitude spectrum and the frequency relationship diagram can be made, and the linear function relationship can be obtained by linear fitting. The K value is obtained through the fitting straight line, and then the ultrasonic propagation velocity c can be calculated, and the wall thickness can be calculated by the time difference of reflected echoes from the upper and lower surfaces, and the expression is as follows:

x=c×Δt/2x=c×Δt/2

式中x为塑料零件壁厚,Δt为上下表面反射回波的时间差。In the formula, x is the wall thickness of the plastic part, and Δt is the time difference of reflected echoes from the upper and lower surfaces.

上述基于超声传播理论的声速和衰减系数的一体化检测方法,应当在检测前已知被测塑料的密度。The above-mentioned integrated detection method of sound velocity and attenuation coefficient based on ultrasonic propagation theory should know the density of the plastic to be tested before the detection.

与现有技术相比,本发明的有益效果是:Compared with prior art, the beneficial effect of the present invention is:

本发明检测方法操作简单,计算方便,检测成本低廉,不破坏被测样品,易于实现在线监测,可以同时检测聚合物零件的声速、衰减系数、壁厚。The detection method of the invention is simple in operation, convenient in calculation, low in detection cost, does not damage the sample to be tested, is easy to realize on-line monitoring, and can simultaneously detect the sound velocity, attenuation coefficient and wall thickness of polymer parts.

附图说明Description of drawings

图1是本发明超声检测原理图。Fig. 1 is a schematic diagram of the ultrasonic detection principle of the present invention.

图2是本发明用于PMMA检测的反射回波实测图。Fig. 2 is an actual measurement diagram of reflected echoes used in PMMA detection according to the present invention.

图3是本发明用于PMMA检测的回波幅值谱的对数值与频率的关系图。Fig. 3 is a graph showing the relationship between the logarithmic value and the frequency of the echo amplitude spectrum used for PMMA detection according to the present invention.

具体实施方式Detailed ways

为使本发明被更清楚地理解,下面根据本发明的具体实例及附图,对本发明进行进一步的说明。In order to make the present invention more clearly understood, the present invention will be further described below according to specific examples and accompanying drawings of the present invention.

如图1所示,是本发明的超声检测原理图,包括超声探头1,容器2,水3,样品4。As shown in FIG. 1 , it is a principle diagram of ultrasonic detection of the present invention, including an ultrasonic probe 1 , a container 2 , water 3 , and a sample 4 .

塑料零件的超声检测方法,包括:Ultrasonic testing methods for plastic parts, including:

将样品放置在装满水的容器中。Place the sample in a container filled with water.

使用水浸超声探头发射具有一定中心频率的脉冲波。检测时保证超声探头正对样品上表面。Use a water immersion ultrasonic probe to emit pulse waves with a certain center frequency. When testing, ensure that the ultrasonic probe is facing the upper surface of the sample.

使用示波器采集接收样品上下表面的反射回波。Use an oscilloscope to collect the reflected echoes from the upper and lower surfaces of the receiving sample.

根据傅里叶变换计算样品上下表面反射回波的频谱。Calculate the frequency spectrum of the reflected echoes from the upper and lower surfaces of the sample according to the Fourier transform.

做出反射回波幅值谱的对数值与频率的关系图,并进行线性拟合。Make a graph of the relationship between the logarithmic value of the reflected echo amplitude spectrum and frequency, and perform linear fitting.

找到拟合直线的纵轴截距并计算K值。Find the vertical intercept of the fitted line and calculate the K value.

根据K值计算超声波传播速度c。Calculate the ultrasonic propagation speed c according to the K value.

根据声速c以及上下表面反射回波的时间差计算壁厚。The wall thickness is calculated from the sound velocity c and the time difference between the reflection echoes from the upper and lower surfaces.

根据壁厚以及拟合曲线的斜率值计算衰减系数。The attenuation coefficient is calculated from the wall thickness and the slope value of the fitted curve.

图2为PMMA的反射回波实测示意图。第一个波形为上表面反射回波,第二个波形为下表面反射回波,两个波形之间的时间差为3.28μs。超声波的中心频率为2.5MHz。Figure 2 is a schematic diagram of the actual measurement of the reflected echo of PMMA. The first waveform is the echo reflected from the upper surface, and the second waveform is the echo reflected from the lower surface. The time difference between the two waveforms is 3.28 μs. The center frequency of ultrasound is 2.5MHz.

图3为用于PMMA检测的回波幅值谱的对数值与频率的关系图。通过线性拟合,得到lnK=-0.1245,并已知PMMA密度为1.18g/cm3,进而计算出超声波在PMMA中传播速度为2547m/s,根据时间差计算出PMMA的壁厚为4.18mm,实测厚度为4.46mm,相对误差为6.3%,衰减系数为7.25dB/cm。对比表明该方法精度较高。Fig. 3 is a graph showing the relationship between the logarithmic value and the frequency of the echo amplitude spectrum used for PMMA detection. Through linear fitting, lnK=-0.1245 is obtained, and the density of PMMA is known to be 1.18g/cm 3 , and then the propagation speed of ultrasonic wave in PMMA is calculated to be 2547m/s, and the wall thickness of PMMA is calculated according to the time difference to be 4.18mm. The thickness is 4.46mm, the relative error is 6.3%, and the attenuation coefficient is 7.25dB/cm. The comparison shows that the method has high precision.

以上所述仅为本发明的一个应用实例,并非对适用被测样品范围的限定。可应用本发明测量的零件,这里无需也无法一一穷举,凡在本发明精神和原则之内,所做的任何修改,等同替换,改进等,均应包含在本发明保护范围之内。The above description is only an application example of the present invention, and does not limit the range of applicable samples to be tested. The parts that can be measured by the present invention need not be exhausted here, and any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.

Claims (5)

1. the velocity of sound and attenuation coefficient integrated detection method in a kind of polymer, which is characterized in that include the following steps:
(1) ultrasonic probe face sample to be tested is emitted into ultrasonic wave;
(2) reflection echo for acquiring sample upper and lower surface, seeks the amplitude spectrum of reflection echo, the sample face ultrasonic probe Side is defined as upper surface, back to side be lower surface;
(3) according to the obtained amplitude spectrum of reflection echo, acquire the ultrasonic propagation velocity of sample to be tested, the thickness of sample and The attenuation coefficient of sample.
2. the velocity of sound and attenuation coefficient integrated detection method in polymer according to claim 1, which is characterized in that step (3) it in, specifically includes:
(3-1) seeks logarithm to obtained amplitude spectrum H (f);WhereinU1It (f) is the frequency of upper surface reflection echo Spectrum, U2It (f) is the frequency spectrum of lower surface reflection echo;
(3-2) seeks the logarithm of the amplitude spectrum of reflection echo and the relational graph of frequency f, and carries out linear fit to it and obtain linearly Function relation figure;Wherein, f is discrete frequency;
The vertical axis intercept D for the linear functional relation figure that (3-3) is sought seeks ultrasonic wave in sample to be tested according to the following formula Spread speed c:
Z=ρ c
D=lnK
In above-mentioned formula:Z0The acoustic impedance of medium between sample to be tested upper surface and ultrasonic probe, Z are the sound of sample to be tested Impedance, ρ are the density of sample to be tested, and c is spread speed of the ultrasonic wave in sample to be tested;
(3-4), the thickness x of sample is calculated by time difference Δ t of upper and lower surface reflection echo, and expression formula is as follows:
X=c × Δ t/2
The slope k for the linear functional relation figure that (3-5) is sought, according to k=-2mx α ÷ fc, acquire attenuation coefficient α;Wherein m =0.115 is converted into the coefficient of Np/cm, f for attenuation coefficient unit by dB/cmcFor the centre frequency of ultrasonic probe.
3. the velocity of sound and attenuation coefficient integrated detection method in polymer according to claim 2, which is characterized in that described Sample is offline sample, and the sample is placed in dielectric fluid before detection, and when detection, the ultrasonic probe is impregnated in the medium In liquid, the Z0For the acoustic impedance of dielectric fluid.
4. the velocity of sound and attenuation coefficient integrated detection method in polymer according to claim 2, which is characterized in that described Sample is on-line sample, and the ultrasonic probe is close to the die cavity side wall on the outside of on-line sample, the Z0For the die cavity side wall Acoustic impedance.
5. the velocity of sound and attenuation coefficient integrated detection method in polymer according to claim 1 or 2, which is characterized in that The sample to be tested is the polymer articles of surfacing.
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