CN103940844B - The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire - Google Patents

The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire Download PDF

Info

Publication number
CN103940844B
CN103940844B CN201410206080.6A CN201410206080A CN103940844B CN 103940844 B CN103940844 B CN 103940844B CN 201410206080 A CN201410206080 A CN 201410206080A CN 103940844 B CN103940844 B CN 103940844B
Authority
CN
China
Prior art keywords
glass plate
thin glass
plane mirror
frequency modulation
measured
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.)
Expired - Fee Related
Application number
CN201410206080.6A
Other languages
Chinese (zh)
Other versions
CN103940844A (en
Inventor
李彦超
沈中辉
甄佳奇
杨九如
高扬
冉玲苓
杨瑞海
杜军
丁群
王春晖
马立峰
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Heilongjiang University
Original Assignee
Heilongjiang University
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Heilongjiang University filed Critical Heilongjiang University
Priority to CN201410206080.6A priority Critical patent/CN103940844B/en
Publication of CN103940844A publication Critical patent/CN103940844A/en
Application granted granted Critical
Publication of CN103940844B publication Critical patent/CN103940844B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Length Measuring Devices By Optical Means (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)
  • Spectrometry And Color Measurement (AREA)

Abstract

The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire, belongs to the linear expansion coefficient fields of measurement of material.The present invention is that parameter measured directly is more, complex operation in order to solve to need in existing linear expansion coefficient measuring method, so that the problem of measurement error is bigger than normal.Linear frequency modulation multi-beam laser heterodyne of the present invention measures the device and method of expansion coefficients of metal wire, based on linear frequency modulation technology and laser heterodyne technique, parameter information to be measured is modulated in heterodyne signal difference on the frequency using linear frequency modulation technology, by the way that multiple parameters to be measured can be obtained simultaneously to the demodulation of heterodyne signal, weight averaged processing, and then obtain accurate parameter information to be measured.The present invention is applied to ultra precise measurement, detection, process equipment, laser radar system etc., and substantially, experimental data is reliable, especially suitable in the engineering design fields such as coherent laser windfinding radar for experimental phenomena of the present invention.

Description

The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire
Technical field
The invention belongs to the linear expansion coefficient fields of measurement of material.
Background technology
The hot expansion property of object reflects the attribute of material in itself, generally by solid it is heated after in one-dimensional square length Change be referred to as line expansion.The linear expansion coefficient of material is measured, not only the development to new material is significant, and is also One of important indicator of the selection of material.All must during manufacture, processing of material of Structural Design, machinery and instrument etc. The thermal expansion character of material must be considered.Otherwise, by the stability and the precision of instrument that influence structure.It is improper to consider, or even can make Into the damage of engineering, the failure of instrument, and the defect processed in welding and failure etc..At present, to expansion coefficients of metal wire Measure have the measuring methods such as optical lever method, reading microscope method, electrothermal way and laser interferance method.
During being measured with these methods, due to needing parameter measured directly excessive, operation is more complicated, so that The systematic error of experiment and accidental error are bigger than normal, for example, when surveying expansion coefficients of metal wire with optical lever method, due to approximate formula Make its systematic error bigger than normal using with complicated operation, simultaneously as reading plotter is equipped with the accidental error of unreasonable introducing It is larger, so that its relative error is up to 4.4%;Reading microscope method is due to accidental error caused by vision and the actual temperature of electrothermal way Systematic error etc. all significantly limit its measurement accuracy caused by the delay of degree and sensor;Laser interferance method is due to the device The sharp thin, high resolution of interference fringe, while experimental implementation is simple, so as to substantially reduce experimental error, realize metal wire The accurate measurement of the coefficient of expansion, the relative error of measurement can be 2%, but this method exists when reading number of interference fringes and regarded Accidental error caused by feeling, causes precision not improve again, can not meet the requirement of current superhigh precision measurement.
The content of the invention
The present invention is that parameter measured directly is more, it is multiple to operate in order to solve to need in existing linear expansion coefficient measuring method It is miscellaneous, so that the problem of measurement error is bigger than normal, now provides linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire Method.
Linear frequency modulation multi-beam laser heterodyne measures the device of expansion coefficients of metal wire, and it includes:Chirped laser device, Thin glass plate, plane mirror, electrothermal furnace, temperature controller, convergent lens and photodetector;
The chirped laser of chirped laser device output incides the preceding surface of thin glass plate, and incidence angle θ0To be sharp Angle, the laser beam splitter is reflected light and refraction light by thin glass plate, and thin glass plate is by a reflected light back to meeting On poly- lens, thin glass plate is by the refraction anaclasis a to plane mirror, a plane mirror and thin glass plate Rear surface No. two reflected lights of multi beam will be obtained after the refraction light multiple reflections, No. two reflected lights of the multi beam reflect through thin glass plate To convergent lens, on the photosurface of the light collection that convergent lens is received to photodetector;
Electrothermal furnace is used to uniformly heat for metallic rod to be measured, and temperature controller is used for the temperature for controlling and detecting electrothermal furnace;
A number plane mirror is fixed on one end of metallic rod to be measured, and vertical with the axis of metallic rod to be measured, thin glass Plate be arranged in parallel with a plane mirror, and the distance between thin glass plate and plane mirror 20mm to 30mm it Between.
Linear frequency modulation multi-beam laser heterodyne based on said apparatus measures the method for expansion coefficients of metal wire, this method bag Include following steps:
Step one:The chirped laser that opening chirped laser device sends chirped laser device incides thin glass In glass plate, and ensure incidence angle θ0For acute angle;Electrothermal furnace and temperature controller are opened simultaneously, and the temperature of temperature controller control electrothermal furnace is simultaneously adopted Collect the temperature of metallic rod to be measured;
Step 2:The photoelectric current I of photodetector output signal is gathered, and photoelectric current I DC terms are filtered Except so as to obtain electric current of intermediate frequency IIF
Step 3:The electric current of intermediate frequency I obtained to step 2IFAnalyzed, obtain the frequency f of interference signalp
Wherein, p is nonnegative integer,For the rate of change of the modulating bandwidth of chirped laser device, T is frequency modulation week Phase, △ F are modulating bandwidth, and n is the refractive index of medium between thin glass plate and a plane mirror, and d is thin glass plate and one The distance between number plane mirror, θ is the refraction angle that incident light transmits thin glass plate, and c is the light velocity of incident light, KpRepresent Proportionality coefficient between the frequency and refraction angle θ cosine of intermediate frequency heterodyne signal;
Step 4:Utilize the frequency f of interference signalpThe distance between thin glass plate and plane mirror d is obtained, is obtained The distance between thin glass plate and plane mirror variable quantity △ d,
△ d=d0- d,
Wherein, d0Represent the initial distance between thin glass plate and a plane mirror;
Step 5:The linear expansion coefficient α of metallic rod to be measured is obtained using following formula,
Wherein, l0Represent the initial length of metallic rod to be measured, △ T=T1-T2The temperature variation of metallic rod to be measured is represented, T1Represent the temperature of metallic rod to be measured at room temperature, T2It is to be measured when representing the distance between thin glass plate and a plane mirror for d The temperature of metallic rod.
Linear frequency modulation multi-beam laser heterodyne of the present invention measures the device and method of expansion coefficients of metal wire, is based on Parameter information to be measured, is modulated in heterodyne signal by linear frequency modulation technology and laser heterodyne technique using linear frequency modulation technology, is led to Parameter information to be measured can accurately be obtained by crossing the demodulation to heterodyne, in the parameter information measurement process, and measuring speed is fast, line Property degree is good, strong antijamming capability, dynamic response is fast, reproducible and measurement range is big;Apparatus structure of the present invention is simple, It is small power consumption, easy to operate;The method of the invention experimental result error is small, precision is high;Tested by taking brass as an example, line expansion The relative error of coefficient measurement is only 0.1%.The present invention is applied to ultra precise measurement, detection, process equipment, laser radar system Deng, experimental phenomena of the present invention substantially, experimental data is reliable, especially suitable in engineering design fields such as coherent laser windfinding radars In.
Brief description of the drawings
Fig. 1 is the dress of the linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire described in embodiment one The structural representation put.
Fig. 2 is principle of interference signal of the linear frequency modulation multi-beam laser between thin glass plate and a plane mirror Figure;Wherein E represents to incide the laser on thin glass plate, E1For the laser of thin glass plate front surface reflection, E2To EmRepresent thin glass The laser of surface refraction after glass plate, d represents the distance between thin glass plate and plane mirror.
Fig. 3 is the dress of the linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire described in embodiment two The structural representation put.
Fig. 4 is the dress of the linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire described in embodiment three The structural representation put.
Fig. 5 is the dress of the linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire described in embodiment four The structural representation put.
Fig. 6 be room temperature at 15 DEG C, the Fourier transformation spectrogram of linear frequency modulation multi-beam laser heterodyne signal.
Embodiment
Embodiment one:Present embodiment, the linear tune described in present embodiment are illustrated referring to Figures 1 and 2 Frequency multi-beam laser heterodyne measures the device of expansion coefficients of metal wire, and it includes:Chirped laser device 1, thin glass plate 2, one Number plane mirror 3, electrothermal furnace 4, temperature controller 6, convergent lens 7 and photodetector 8;
The chirped laser that chirped laser device 1 is exported incides the preceding surface of thin glass plate 2, and incidence angle θ0For Acute angle, the laser beam splitter is reflected light and refraction light by thin glass plate 2, and thin glass plate 2 is by a reflected light back To convergent lens 7, thin glass plate 2 by the refraction anaclasis a to plane mirror 3, a plane mirror 3 with The rear surface of thin glass plate 2 will obtain No. two reflected lights of multi beam after the refraction light multiple reflections, No. two reflected lights of the multi beam are through thin Glass plate 2 is refracted on convergent lens 7, the photosurface of the light collection that convergent lens 7 is received to photodetector 8 On;
Electrothermal furnace 4 is used to uniformly heat for metallic rod 5 to be measured, and temperature controller 6 is used for the temperature for controlling and detecting electrothermal furnace 4;
A number plane mirror 3 is fixed on one end of metallic rod 5 to be measured, and vertical with the axis of metallic rod 5 to be measured, thin glass Glass plate 2 be arranged in parallel with a plane mirror 3, and the distance between thin glass plate 2 and plane mirror 3 in 20mm extremely Between 30mm.
Temperature controller 6 described in present embodiment is digital readout temperature controller, and the digital readout temperature controller is easy to reading, easy to operate, energy Enough make measurement process easy.
Embodiment two:Reference picture 3 illustrates present embodiment, and present embodiment is to embodiment one The device of described linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire is described further, present embodiment In, it also includes:Data handling system 9;
The electrical signal of photodetector 8 connects the electric signal input end of data handling system 9;The data processing The module of software realization is embedded with system 9, the module is included with lower unit:
Gather the signal gathering unit for the photoelectric current I that photodetector 8 is exported;
Photoelectric current I is filtered, so as to obtain electric current of intermediate frequency IIFFilter unit;
Utilize electric current of intermediate frequency IIFObtain the frequency f of interference signalpUnit;
Utilize the frequency f of interference signalpObtain the distance between thin glass plate 2 and plane mirror 3 d unit;
Thin glass plate 2 and a plane reflection are obtained according to the distance between thin glass plate 2 and plane mirror 3 d The distance between mirror 3 variable quantity △ d unit;
The line for obtaining metallic rod 5 to be measured using distance change amount △ d between thin glass plate 2 and a plane mirror 3 is swollen The unit of swollen factor alpha.
Embodiment three:Reference picture 4 illustrates present embodiment, and present embodiment is to embodiment one The device of described linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire is described further, present embodiment In, it also includes:Wave filter 9-1, amplifier 9-2, A/D converter 9-3 and DSP9-4;
The electrical signal connection wave filter 9-1 of photodetector 8 electric signal input end, wave filter 9-1 telecommunications Number output end connection amplifier 9-2 electric signal input end, amplifier 9-2 electrical signal connection A/D converter 9-3's Input end of analog signal, A/D converter 9-3 digital signal output end connects DSP9-4 digital signal input end;
The module of software realization is embedded with the DSP9-4, the module is included with lower unit:
Gather the electric current of intermediate frequency I of A/D converter 9-3 outputsIFSignal gathering unit;
Utilize electric current of intermediate frequency IIFObtain the frequency f of interference signalpUnit;
Utilize the frequency f of interference signalpObtain the distance between thin glass plate 2 and plane mirror 3 d unit;
Thin glass plate 2 and a plane reflection are obtained according to the distance between thin glass plate 2 and plane mirror 3 d The distance between mirror 3 variable quantity △ d unit;
The line for obtaining metallic rod 5 to be measured using distance change amount △ d between thin glass plate 2 and a plane mirror 3 is swollen The unit of swollen factor alpha.
The temperature probe of digital readout temperature controller obtains the signal for representing temperature by platinum resistance thermometer sensor,;And desired temperature is used " setting knob " is adjusted, two chosen switches of signal and A/D converter, can be shown measurement temperature respectively on charactron and be set Constant temperature degree.Electrothermal furnace heating uniform to testing sample disconnects heater circuit automatically close to design temperature by relay;In measurement State, shows the temperature being currently detected.
Embodiment four:Reference picture 5 illustrates present embodiment, and present embodiment is to embodiment one The device of described linear frequency modulation multi-beam laser heterodyne measurement expansion coefficients of metal wire is described further, present embodiment In, it also includes:No. two plane mirrors 10;
The laser light incident that chirped laser device 1 is exported is on No. two plane mirrors 10, and No. two plane mirrors 10 will The laser reflection is to the preceding surface of thin glass plate 2, and incidence angle θ0For acute angle.
Embodiment five:Present embodiment be to the linear frequency modulation multi-beam laser described in embodiment one outside The device of difference measurements expansion coefficients of metal wire is described further, in present embodiment, the frequency modulation of the chirped laser device 1 Cycle is 1ms, and modulating bandwidth is 5GHz, and the wavelength of output laser is 1.55 μm.
Embodiment six:Present embodiment be to the linear frequency modulation multi-beam laser described in embodiment one outside The device of difference measurements expansion coefficients of metal wire is described further, in present embodiment, incidence angle θ0For 15.26 °.
Embodiment seven:Present embodiment be to the linear frequency modulation multi-beam laser described in embodiment one outside The device of difference measurements expansion coefficients of metal wire is described further, in present embodiment, and the thickness of the thin glass plate 2 is more than 0mm and less than 1mm.
Embodiment eight:Present embodiment be to the linear frequency modulation multi-beam laser described in embodiment one outside The device of difference measurements expansion coefficients of metal wire is described further, in present embodiment, the frequency f of interference signalpFor:
Wherein, p is nonnegative integer,For the rate of change of the modulating bandwidth of chirped laser device 1, T is frequency modulation week Phase, △ F be modulating bandwidth, n between thin glass plate 2 and a plane mirror 3 medium refractive index, d be thin glass plate 2 with The distance between number plane mirror 3, θ is the refraction angle that incident light transmits thin glass plate 2, and c is the light velocity of incident light, Kp Represent the proportionality coefficient between the frequency and refraction angle θ cosine of intermediate frequency heterodyne signal.
Embodiment nine:Present embodiment be to the linear frequency modulation multi-beam laser described in embodiment one outside The device of difference measurements expansion coefficients of metal wire is described further, in present embodiment, and metallic rod 5 to be measured is obtained using following formula Linear expansion coefficient α,
Wherein, l0Represent the initial length of metallic rod 5 to be measured, △ T=T1-T2Represent the temperature change of metallic rod 5 to be measured Amount, T1Represent the temperature of metallic rod 5 to be measured at room temperature, T2Represent the distance between thin glass plate 2 and plane mirror 3 for d When metallic rod 5 to be measured temperature.
Embodiment ten:Linear frequency modulation multi-beam laser heterodyne measurement metal wire based on embodiment one is swollen In the method for swollen coefficient, present embodiment, this method comprises the following steps:
Step one:The chirped laser that opening chirped laser device 1 sends chirped laser device 1 incides thin On glass plate 2, and ensure incidence angle θ0For acute angle;Electrothermal furnace 4 and temperature controller 6 are opened simultaneously, and temperature controller 6 gathers metallic rod to be measured 5 temperature;
Step 2:The signal for the photoelectric current I that photodetector 8 is exported is gathered, and photoelectric current I DC terms are filtered Except so as to obtain electric current of intermediate frequency IIF
Step 3:The electric current of intermediate frequency I obtained to step 2IFAnalyzed, obtain the frequency f of interference signalp
Wherein, p is nonnegative integer,For the rate of change of the modulating bandwidth of chirped laser device 1, T is frequency modulation week Phase, △ F be modulating bandwidth, n between thin glass plate 2 and a plane mirror 3 medium refractive index, d be thin glass plate 2 with The distance between number plane mirror 3, θ is the refraction angle that incident light transmits thin glass plate 2, and c is the light velocity of incident light, Kp Represent the proportionality coefficient between the frequency and refraction angle θ cosine of intermediate frequency heterodyne signal;
Step 4:Utilize the frequency f of interference signalpThe distance between thin glass plate 2 and plane mirror 3 d is obtained, The distance between thin glass plate 2 and plane mirror 3 variable quantity △ d are obtained,
△ d=d0- d,
Wherein, d0Represent the initial distance between thin glass plate 2 and a plane mirror 3;
Step 5:The linear expansion coefficient α of metallic rod 5 to be measured is obtained using following formula,
Wherein, l0Represent the initial length of metallic rod 5 to be measured, △ T=T1-T2Represent the temperature change of metallic rod 5 to be measured Amount, T1Represent the temperature of metallic rod 5 to be measured at room temperature, T2Represent the distance between thin glass plate 2 and plane mirror 3 for d When metallic rod 5 to be measured temperature.
As shown in Fig. 2 because light beam constantly can reflect and reflect between thin glass plate and a plane mirror, and This reflection and refraction are all contributed for the interference of reflected light and transmitted light at infinity or on lens focal plane, so When interference is discussed, it is necessary to consider multiple reflections and refraction effect, i.e., it should discuss that multi-beam laser is interfered.
In the case where not considering thin glass plate its thickness, the laser after linear frequency modulation is with incidence angle θ0Oblique incidence When, the mathematic(al) representation of incident field is:
E (t)=E0exp{i(ω0t+kt2)} (1)
Wherein,For the rate of change of the modulating bandwidth of chirped laser device, T is the frequency modulation cycle, and △ F are frequency modulation band It is wide;E0For incident field amplitude, t is time, ω0For light field angular frequency.If the light path for reaching the preceding surface of thin glass plate is L,The reflection light field that moment reaches thin glass plate preceding surface is:
Wherein, α1=r, r are the reflectivity of thin glass plate.
And the light transmitted through thin glass plate by plane mirror multiple reflections and is not transmiting thin glass plate in the same time, its The light field expression formula of transmitted light can be written respectively as following form:
Wherein, α22R ' ..., αm2r′m-1rm-2, β is the transmissivity of thin glass plate, and r ' is the reflection of plane mirror Rate, d is the distance between thin glass plate and plane mirror, and θ is that incident light transmits the refraction angle after thin glass plate, and n is thin The refractive index of medium between glass plate and plane mirror, the value of subscript m is 2,3,4 ....Due to have ignored thin glass plate Thickness, therefore do not consider the influence on surface after thin glass plate.
So, total light field that detector is received can be expressed as:
E ' (t)=E1(t)+E2(t)+…+Em(t)+… (4)
Then the photoelectric current of detector output can be expressed as:
Wherein, e is electron charge, and Z is the intrinsic impedance of detector surface medium, and η is quantum efficiency, and h is that Planck is normal Number, ν is laser frequency, No. * expression complex conjugate.
Because heterodyne signal DC terms can be filtered out after low pass filter, therefore, exchange item is only considered here, this friendship It is commonly referred to as electric current of intermediate frequency to flow item, and the electric current of intermediate frequency that arrangement can obtain chirped laser heterodyne signal is:
(2) formula and (3) formula are substituted into (6) formula, final result is:
Wherein, p and j are nonnegative integer.
It can see by (7) formula, an intermediate frequency that linear frequency modulation multiple beam heterodyne measurement method is obtained difference on the frequency and phase There is the information apart from d between thin glass plate and plane mirror in difference.Analyzed mainly for difference on the frequency in intermediate frequency, because To be easily achieved frequency measurement using Fourier transformation.Now, can be outside linear frequency modulation multi-beam laser according to (7) formula The frequency of difference signal is designated as:
It should be noted that the photoelectric current expression formula that can be seen that detector output by (7) formula is fourier transformed it Afterwards it can be seen that linear frequency modulation multi-beam laser heterodyne signal frequency crest, is believed by measuring multi-beam laser heterodyne on frequency spectrum Number frequency, it is possible to the distance between thin glass plate and plane mirror d are measured, when d changes, it is possible to surveyed according to (8) formula Go out correspondence d variable quantity △ d, it is known that △ d can just be calculated according to (9) formula and be obtained testing sample linear expansion coefficient.
Based on the measurement scheme of linear frequency modulation multi-beam laser heterodyne shown in Fig. 2, long 150mm, a diameter of Φ 18mm are measured Brass wire bar material linear expansion coefficient, and verify the feasibility of multi-beam laser heterodyne measuring method.Configured in measurement Temperature control instrument be XMT type digital displaying temperature adjusting apparatus;Chirped laser device wavelength is 1.55 μm, frequency modulation cycle T =1ms, modulating bandwidth △ F=5GHz.
According to the emulation of (7) formula it can be seen that, when metal bar is in 15 DEG C of room temperature, the linear frequency modulation obtained through signal transacting The Fourier transformation frequency spectrum of multi-beam laser heterodyne signal is as shown in fig. 6, wherein solid line is 15 DEG C of room temperature and laser oblique incidence feelings Under condition, the Fourier transformation frequency spectrum of correspondence linear frequency modulation multi-beam laser heterodyne signal during measurement metal bar length change amount △ l; In the case of dotted line is 15 DEG C of room temperature and laser normal incidence, correspondence linear frequency modulation multiple beam during measurement metal bar length change amount △ l The Fourier transformation frequency spectrum of heterodyne signal.
It will be seen from figure 6 that the theoretical curve in the case of normal incidence is given in experiment, it is therefore an objective to:Linearly adjusting In frequency multi-beam laser heterodyne signal spectrum figure, linear frequency modulation multi-beam laser heterodyne signal frequency during oblique incidence can be obtained simultaneously The numerical value of the centre frequency of theoretical curve when the centre frequency and normal incidence of first main peak of spectrum, in this way it is easy to obtain two The ratio of individual centre frequency:
ζ=cos θ (10)
In theoretical derivation, the thickness that have ignored thin glass plate does not consider the reflected light on surface after device to linear tune The influence of frequency multi-beam laser heterodyne signal, but the thickness of actually thin glass plate is present generally less than 1mm, to overcome this Influence is planted, the linear frequency modulation multiple beam heterodyne signal that the reflected light that can be seen that surface after thin glass plate according to (10) formula is produced Frequency distribution near the zero-frequency of frequency spectrum, the dry of low frequency heterodyne signal can just be filtered out by experiment light path adding wave filter Disturb.Using above-mentioned linear frequency modulation multi-beam laser heterodyne mensuration, continuously eight groups of data of measurement, have obtained laser light incident angle θ0= At 15.26 °, the measurement result of metal bar length change amount to be measured in the case of different temperatures, as shown in table 1.
In the case of the different temperatures T of table 1, the measurement result of metal bar length change amount
It should be noted that:In table 1 15 DEG C be laboratory temperature.Meanwhile, the simulation experiment result in table 1 can be led Go out each data of correlation:
(1) temperature T standard uncertainties σc(△T)
Duplicate measurementsThen, type A standard uncertaintyThe limit error Δ that temperature controller is introduced1=0.002 DEG C Then, type B standard uncertaintyThen σc(△ T)=(0.0002+0.0012)1/2=0.001 DEG C.
(2) length l0Standard uncertainty σc(l0)
Use slide measure duplicate measurementsThen, type A standard uncertainty:
The limit error Δ that slide measure is introduced2=0.02mm then, type B standard uncertaintyThen σc(l0)=(0.0092+0.0122)1/2=0.015mm.
Using the experimental data of table 1, the average measurement value of the linear expansion coefficient of metal bar is
The standard uncertainty of linear expansion coefficient is
The measurement result of linear expansion coefficient can be expressed as:
And the theoretical value 2.06 × 10 of the linear expansion coefficient of metal bar-5/ DEG C, it so can be obtained by the phase of measurement result It is to error:
By data processing as can be seen that measuring metal wire expansion with linear frequency modulation multi-beam laser heterodyne method measurement apparatus The relative measurement error of coefficient is only 0.1%, compared with traditional measuring method, and the result measured by this method has more preferable Precision.Meanwhile, analyze data can also be seen that in the case where sample is uniformly heated, and environmental error is to neglect in an experiment Slightly.Error in experiment mostlys come from the precision after the limit error of measurement apparatus, and Fast Fourier Transform (FFT) (FFT) Rounding error in error and calculating process, can reduce limit error by improving the measurement accuracy of measurement apparatus, pass through Processing for Data Analysis in Physics is improved to miss to reduce the rounding-off in the trueness error and calculating process after Fast Fourier Transform (FFT) (FFT) Difference, it is final further to improve measurement accuracy.

Claims (7)

1. the method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire, it is swashed based on linear frequency modulation multiple beam What the device of optical heterodyne expansion coefficients of metal wire was realized, described device includes:Chirped laser device (1), thin glass plate (2), plane mirror (3), electrothermal furnace (4), temperature controller (6), convergent lens (7) and photodetector (8);
The chirped laser of chirped laser device (1) output incides the preceding surface of thin glass plate (2), and incidence angle θ0For The laser beam splitter is a reflected light and refraction light by acute angle, thin glass plate (2), and thin glass plate (2) is anti-by a reflected light It is incident upon on convergent lens (7), thin glass plate (2) is by the refraction anaclasis a to plane mirror (3), and a plane is anti- No. two reflected lights of multi beam, the multi beam two will be obtained by penetrating the rear surface of mirror (3) and thin glass plate (2) after the refraction light multiple reflections Reflected light is refracted on convergent lens (7) through thin glass plate (2), the light collection that convergent lens (7) is received to photoelectricity On the photosurface of detector (8);
Electrothermal furnace (4) is used to uniformly heat for metallic rod to be measured (5), and temperature controller (6) is used for the temperature for controlling and detecting electrothermal furnace (4) Degree;
A number plane mirror (3) is fixed on one end of metallic rod to be measured (5), and vertical with the axis of metallic rod to be measured (5), thin Glass plate (2) be arranged in parallel with a plane mirror (3), and between thin glass plate (2) and a plane mirror (3) away from From in 20mm between 30mm;
Characterized in that, the described method comprises the following steps:
Step one:The chirped laser that opening chirped laser device (1) sends chirped laser device (1) incides thin On glass plate (2), and ensure incidence angle θ0For acute angle;Electrothermal furnace (4) and temperature controller (6) are opened simultaneously, and temperature controller (6) collection is treated Survey the temperature of metallic rod (5);
Step 2:The photoelectric current I of photodetector (8) output signal is gathered, and photoelectric current I DC terms are filtered out So as to obtain electric current of intermediate frequency IIF
Step 3:The electric current of intermediate frequency I obtained to step 2IFAnalyzed, obtain the frequency f of interference signalp
<mrow> <msub> <mi>f</mi> <mi>p</mi> </msub> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>p</mi> <mi>k</mi> <mi>n</mi> <mi>d</mi> <mi> </mi> <mi>c</mi> <mi>o</mi> <mi>s</mi> <mi>&amp;theta;</mi> </mrow> <mrow> <mi>&amp;pi;</mi> <mi>c</mi> </mrow> </mfrac> <mo>=</mo> <msub> <mi>K</mi> <mi>p</mi> </msub> <mi>d</mi> <mo>,</mo> </mrow>
Wherein, p is nonnegative integer,For the rate of change of the modulating bandwidth of chirped laser device (1), T is the frequency modulation cycle, △ F are modulating bandwidth, and n is the refractive index of medium between thin glass plate (2) and a plane mirror (3), and d is thin glass plate (2) the distance between with plane mirror (3), θ is the refraction angle that incident light transmits thin glass plate (2), and c is incident light The light velocity, KpRepresent the proportionality coefficient between the frequency and refraction angle θ cosine of intermediate frequency heterodyne signal;
Step 4:Utilize the frequency f of interference signalpThe distance between thin glass plate (2) and plane mirror (3) d is obtained, The distance between thin glass plate (2) and plane mirror (3) variable quantity △ d are obtained,
△ d=d0- d,
Wherein, d0Represent the initial distance between thin glass plate (2) and a plane mirror (3);
Step 5:The linear expansion coefficient α of metallic rod (5) to be measured is obtained using following formula,
<mrow> <mi>&amp;alpha;</mi> <mo>=</mo> <mfrac> <mrow> <mi>&amp;Delta;</mi> <mi>d</mi> </mrow> <mrow> <msub> <mi>l</mi> <mn>0</mn> </msub> <mi>&amp;Delta;</mi> <mi>T</mi> </mrow> </mfrac> <mo>,</mo> </mrow>
Wherein, l0Represent the initial length of metallic rod to be measured (5), △ T=T1-T2Represent the temperature change of metallic rod to be measured (5) Amount, T1Represent the temperature of metallic rod (5) to be measured at room temperature, T2Represent between thin glass plate (2) and a plane mirror (3) The temperature of metallic rod (5) to be measured when distance is d.
2. the method that linear frequency modulation multi-beam laser heterodyne according to claim 1 measures expansion coefficients of metal wire, it is special Levy and be, described device also includes:Data handling system (9);
The electric signal input end of the electrical signal connection data handling system (9) of photodetector (8);The data processing The module of software realization is embedded with system (9), the module is included with lower unit:
Gather the photoelectric current I of photodetector (8) output signal gathering unit;
Photoelectric current I is filtered, so as to obtain electric current of intermediate frequency IIFFilter unit;
Utilize electric current of intermediate frequency IIFObtain the frequency f of interference signalpUnit;
Utilize the frequency f of interference signalpObtain the distance between thin glass plate (2) and plane mirror (3) d unit;
Thin glass plate (2) is obtained according to the distance between thin glass plate (2) and a plane mirror (3) d and a plane is anti- Penetrate the distance between mirror (3) variable quantity △ d unit;
The line of metallic rod (5) to be measured is obtained using distance change amount △ d between thin glass plate (2) and a plane mirror (3) Coefficient of expansion α unit.
3. the method that linear frequency modulation multi-beam laser heterodyne according to claim 1 measures expansion coefficients of metal wire, it is special Levy and be, described device also includes:Wave filter (9-1), amplifier (9-2), A/D converter (9-3) and DSP (9-4);
The electric signal input end of the electrical signal connection wave filter (9-1) of photodetector (8), the electricity of wave filter (9-1) The electric signal input end of signal output part connection amplifier (9-2), the electrical signal connection A/D conversions of amplifier (9-2) The input end of analog signal of device (9-3), the digital signal output end connection DSP (9-4) of A/D converter (9-3) data signal Input;
The module of software realization is embedded with the DSP (9-4), the module is included with lower unit:
Gather the electric current of intermediate frequency I of A/D converter (9-3) outputIFSignal gathering unit;
Utilize electric current of intermediate frequency IIFObtain the frequency f of interference signalpUnit;
Utilize the frequency f of interference signalpObtain the distance between thin glass plate (2) and plane mirror (3) d unit;
Thin glass plate (2) is obtained according to the distance between thin glass plate (2) and a plane mirror (3) d and a plane is anti- Penetrate the distance between mirror (3) variable quantity △ d unit;
The line of metallic rod (5) to be measured is obtained using distance change amount △ d between thin glass plate (2) and a plane mirror (3) Coefficient of expansion α unit.
4. the method that the linear frequency modulation multi-beam laser heterodyne according to claim 1,2 or 3 measures expansion coefficients of metal wire, Characterized in that, described device also includes:No. two plane mirrors (10);
The laser light incident of chirped laser device (1) output is on No. two plane mirrors (10), No. two plane mirrors (10) By the preceding surface of laser reflection to thin glass plate (2), and incidence angle θ0For acute angle.
5. the method that linear frequency modulation multi-beam laser heterodyne according to claim 4 measures expansion coefficients of metal wire, it is special Levy and be, the frequency modulation cycle of the chirped laser device (1) is 1ms, and modulating bandwidth is 5GHz, the wavelength of output laser is 1.55μm。
6. the method that linear frequency modulation multi-beam laser heterodyne according to claim 5 measures expansion coefficients of metal wire, it is special Levy and be, incidence angle θ0For 15.26 °.
7. the method that linear frequency modulation multi-beam laser heterodyne according to claim 6 measures expansion coefficients of metal wire, it is special Levy and be, the thickness of the thin glass plate (2) is more than 0mm and less than 1mm.
CN201410206080.6A 2014-05-15 2014-05-15 The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire Expired - Fee Related CN103940844B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410206080.6A CN103940844B (en) 2014-05-15 2014-05-15 The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410206080.6A CN103940844B (en) 2014-05-15 2014-05-15 The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire

Publications (2)

Publication Number Publication Date
CN103940844A CN103940844A (en) 2014-07-23
CN103940844B true CN103940844B (en) 2017-10-10

Family

ID=51188602

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410206080.6A Expired - Fee Related CN103940844B (en) 2014-05-15 2014-05-15 The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire

Country Status (1)

Country Link
CN (1) CN103940844B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107884433A (en) * 2017-11-10 2018-04-06 哈尔滨学院 A kind of experimental provision using Newton's ring instrument metal linear expansion coefficient measurement

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101825590A (en) * 2009-12-24 2010-09-08 哈尔滨工业大学 Device and method for high-accuracy measurement of expansion coefficients of metal wire
CN102175711A (en) * 2011-01-11 2011-09-07 华中科技大学 Measuring method and device for coefficients of thermal expansion
CN102253073A (en) * 2011-05-31 2011-11-23 哈尔滨工业大学 Device and method for measuring metal linear expansion coefficient by adopting Doppler galvanometer sine modulated multi-beam laser heterodyne
CN102353916A (en) * 2011-05-31 2012-02-15 哈尔滨工业大学 Device and measuring method for measuring magnetoconstriction coefficient through multi-beam laser heterodyne secondary harmonic method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005083920A (en) * 2003-09-09 2005-03-31 Mitsutoyo Corp Linear expansion coefficient measuring device
US7548317B2 (en) * 2006-05-05 2009-06-16 Agc Flat Glass North America, Inc. Apparatus and method for angular colorimetry

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101825590A (en) * 2009-12-24 2010-09-08 哈尔滨工业大学 Device and method for high-accuracy measurement of expansion coefficients of metal wire
CN102175711A (en) * 2011-01-11 2011-09-07 华中科技大学 Measuring method and device for coefficients of thermal expansion
CN102253073A (en) * 2011-05-31 2011-11-23 哈尔滨工业大学 Device and method for measuring metal linear expansion coefficient by adopting Doppler galvanometer sine modulated multi-beam laser heterodyne
CN102353916A (en) * 2011-05-31 2012-02-15 哈尔滨工业大学 Device and measuring method for measuring magnetoconstriction coefficient through multi-beam laser heterodyne secondary harmonic method

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Numerical investigation of multi-beam laser heterodyne measurement with ultra-precision for linear expansion coefficient of metal based on oscillating mirror modulation;Li Yan-Chao et al.;《Chinese Physics B》;20111231;第20卷(第1期);第014208-1页-第014208-7页 *
测量金属材料线膨胀系数的两种新方法;王军等;《物理实验》;19981231;第18卷(第4期);7-10 *

Also Published As

Publication number Publication date
CN103940844A (en) 2014-07-23

Similar Documents

Publication Publication Date Title
CN102175711B (en) Measuring method and device for coefficients of thermal expansion
CN105928906B (en) A kind of material reflectance dynamic measurement system varied with temperature and measurement method
CN105783999B (en) Reference optical fiber eliminates temperature strain cross sensitivity method in a kind of probe beam deflation
CN102253073B (en) Device and method for measuring metal linear expansion coefficient by adopting Doppler galvanometer sine modulated multi-beam laser heterodyne
CN204556093U (en) A kind of low noise micro-cantilever thermal vibration signal measurement apparatus
CN102749141A (en) Radiation temperature measuring method and apparatus for measuring true target temperature
CN107677621A (en) The temperature measuring equipment of multispectral optical technology fusion
CN109186956A (en) A kind of transient state wavefront distortion measurement method for the online situation of beam shaping element
CN102589714A (en) Temperature measuring device based on high-pressure gas Rayleigh-Brillouin scattering spectrum
CN101261224A (en) Optical non-linear method for measuring material based on 4f phase coherent imaging system
CN209590271U (en) A kind of measuring device of space length
CN110686853A (en) Focusing laser differential interferometer and non-intrusive method for measuring density pulsation of flow field of wind tunnel
CN102323555A (en) Method for measuring magnetostriction constant by using multi-beam laser heterodynes
CN103940844B (en) The method that linear frequency modulation multi-beam laser heterodyne measures expansion coefficients of metal wire
CN107727234B (en) Device and method for rapidly detecting terahertz output frequency instability of backward wave tube
CN102253075B (en) Device and method for measuring metal linear expansion coefficient based on multi-beam laser heterodyne second harmonic
CN102621096A (en) Method for high-accuracy measurement of linear refractive index of material
CN105928625B (en) Metal surface dynamic temperature point measuring method based on reflectivity change
CN103954645B (en) The device and method of linear frequency modulation double light beam laser heterodyne measurement expansion coefficients of metal wire
CN205679319U (en) Metal material surface dynamic temperature point based on reflectance change measures system
CN207751871U (en) A kind of measuring device of nonlinear refraction coefficient of materials rate coefficient
CN104655029A (en) Method and system for measuring thickness of phase-enhanced film
Yan-Chao et al. Linear frequency modulation multi-beam laser heterodyne measurement for the glass thickness
CN204612666U (en) A kind of position phase reinforced membranes thickness measurement system
CN103954646B (en) Linear frequency modulation multi-beam laser heterodyne second harmonic method is measured the device and method of expansion coefficients of metal wire

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
CB03 Change of inventor or designer information
CB03 Change of inventor or designer information

Inventor after: Li Yanchao

Inventor after: Wang Chunhui

Inventor after: Ma Lifeng

Inventor after: Shen Zhonghui

Inventor after: Zhen Jiaqi

Inventor after: Yang Jiuru

Inventor after: Gao Yang

Inventor after: Ran Linglian

Inventor after: Yang Ruihai

Inventor after: Du Jun

Inventor after: Ding Qun

Inventor before: Li Yanchao

Inventor before: Ma Lifeng

Inventor before: Zhen Jiaqi

Inventor before: Yang Jiuru

Inventor before: Gao Yang

Inventor before: Ran Linglian

Inventor before: Yang Ruihai

Inventor before: Du Jun

Inventor before: Ding Qun

Inventor before: Wang Chunhui

GR01 Patent grant
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: 20171010

Termination date: 20190515