CN1916640A - Device and method in use for measuring angular velocity of pointing scan mirror - Google Patents

Abstract

A device used to measure angular speed pointing to scanning mirror is prepared as using optical unit to convert angular micro variation pointing to scanning mirror to be intensity signal interfered by laser beam, utilizing detector to convert light intensity signal to be electric signal, using inversion software stored in internal memory of PC computer to obtain angular speed pointing to scanning mirror after electric signal is processed by information processing module.

Description

A kind of device and method that is used to measure angular velocity of pointing scan mirror

Technical field

The present invention relates to the measurement mechanism and the method for angular velocity, specifically be meant a kind of angle rotation-speed measuring device and method that is used for the pointing scan mirror of space flight and aviation remote sensing instrument.

Background technology

In field of aerospace, pointing scan mirror is the important component part of earth observation load.These load often all are that the low speed continuous sweep by scan mirror obtains high-quality remote sensing images, and can the angular velocity that therefore accurately measure pointing scan mirror just seem particularly important.

The method of traditional measurement low speed angular velocity of pointing scan mirror is based on generally that laser alignment and area array CCD realize, ultimate principle as shown in Figure 1.The exit direction of fixed laser, when pointing scan mirror turned over θ, reflection ray turned over 2 θ.Drive CCD by the Electric Machine Control roller bearing and follow the tracks of emergent ray, the read output signal of fast detecting CCD just can be finally inversed by the angular velocity of pointing scan mirror like this.The measuring accuracy of this kind device is relevant with the roller bearing precision with the frame frequency of CCD, if obtain 1 " precision, must adopt big face battle array scientific grade CCD and high-precision stepper motor, cost is high, and the driving of area array CCD and signal Processing are all very complicated.

Summary of the invention

Problem based on above-mentioned measurement mechanism exists the objective of the invention is to propose angular velocity of pointing scan mirror measurement mechanism and method a kind of simple in structure, with low cost.

Angular velocity of pointing scan mirror measurement mechanism of the present invention comprises: opticator and electronics part.

Opticator is made up of corner cube mirror and two spectroscopes.

The electronics part is made up of laser instrument, unit light electric explorer, message processing module.

Said pointing scan mirror is fixed in the rotating shaft, minute surface and rotating shaft axially parallel, and rotating shaft is by Electric Machine Control.

Said corner cube mirror is made up of two orthogonal plane mirrors, and the seamed edge that two catoptrons intersect is fixed in the rotating shaft of pointing scan mirror, and seamed edge is in the rotating shaft coaxial direction, and corner cube mirror and pointing scan mirror angle are fixed.

Said message processing module is by the prime amplifier that becomes circuit to connect successively, filtering circuit, and the A/D conversion, data formatter and PC are formed.Data formatter is made up of extensive Programmable Logic Controller CPLD and two static memory SRAM, and it is to utilize two buffer memory SRAM of CPLD control to rattle to read and write to switch, and realizes that the continuous transmission of digital signal streams improves circuit efficiency.There is the motion angular velocity software that digital signal is finally inversed by pointing scan mirror in the PC.

Detector becomes circuit to be connected with prime amplifier.

The light beam that laser instrument sends is divided into transmitted light beam X and folded light beam Y with 45 ° of incident first spectroscopes by first spectroscope, and folded light beam Y, is received by detector through the reflection of second spectroscope again with 45 ° of incident second spectroscopes.The corner cube mirror reflection of transmitted light beam X through rotating synchronously with pointing scan mirror through the second spectroscope transmission, received by detector again.The signal input information processing module that detector receives is handled.

The concrete steps of angular velocity of pointing scan mirror measuring method of the present invention are as follows:

1. the fixing position of corner cube mirror and pointing scan mirror, the i.e. fixing angle of corner cube mirror and pointing scan mirror.The seamed edge that corner cube mirror two reflectings surface intersect is fixed in the rotating shaft, and coaxial with rotating shaft, fixing means can adopt splicing, also can adopt to be spirally connected.

2. light path adjustment: open laser instrument, rotate pointing scan mirror, adjust first spectroscope and second spectroscopical position, observe the exit direction of laser instrument, if this light beam, illustrates first spectroscope and second spectroscopical position along with the rotation direction of pointing scan mirror does not change and adjusts.

3. open message processing module and detector, start the motor of pointing scan mirror, pointing scan mirror begins to rotate, PC opening entry photodetector detects, obtain output signal through the message processing module processing, the signal of record is the digital signal of having passed through formatting, and the motion angular velocity software processes that is finally inversed by pointing scan mirror by the digital signal that has in the PC obtains the magnitude of angular velocity of pointing scan mirror again.

The present invention has following beneficial effect:

1. measurement mechanism of the present invention is simple in structure, compact.For identical measuring accuracy requirement, realize that cost of the present invention significantly reduces with respect to traditional C CD measurement mechanism.

2. measurement mechanism of the present invention all is suitable for the angular velocity measurement of the low speed pointing scan mirror of different purposes.

Description of drawings

Fig. 1 traditional measurement device synoptic diagram.

Fig. 2 is a proving installation schematic diagram of the present invention.

Fig. 3 is the connection diagram of pointing scan mirror and corner cube mirror.

Fig. 4 is optical path difference computational analysis figure of the present invention.

Fig. 5 is an inversion algorithm analog prober output signal simulation synoptic diagram.

Fig. 6 is the signal processing module structural representation.

Fig. 7 is the software flow pattern that has in the PC.

Embodiment

Below in conjunction with accompanying drawing the specific embodiment of the present invention is described in further detail:

Measurement mechanism of the present invention as shown in Figure 2, tested pointing scan mirror 1 is axial restraints with its rotating shaft 3, minute surface and its rotating shaft axially parallel, rotating shaft is by Electric Machine Control.Corner cube mirror 2 is made up of two orthogonal plane mirrors, and the seamed edge that two catoptrons intersect is fixed in the rotating shaft 3, and is coaxial with rotating shaft, and it and rotating shaft 3 affixed modes can be to glued joint, and also can be to be spirally connected.Therefore, the angle of corner cube mirror and pointing scan mirror is fixed.

The light beam that laser instrument 7 sends is divided into transmitted light beam X and folded light beam Y with 45 ° of incidents, first spectroscope 4 by first spectroscope, and folded light beam Y, is received by detector 6 through the reflection of second spectroscope again with 45 ° of incidents, second spectroscope 5.Corner cube mirror 2 reflections of transmitted light beam X through rotating with pointing scan mirror through 5 transmissions of second spectroscope, are received by detector again.

Because the light path of light beam Y is changeless, light beam X changes with the rotation of pointing scan mirror, so detector receives is the signal of the intensity alternate that interferes of two bundles.The beam signal that the present invention utilizes two bundles to interfere is measured the rotating speed of pointing scan mirror.

Fig. 3 is seen in the light beam light path difference computational analysis that two bundles interfere, and is a straight line MN perpendicular to incident and emergent ray by pivot point O, and we make | MO|=b, | NO|=a, so according to θ ₂Be the incident angle before rotating, θ ₁Be the incident angle after rotating, can obtain both optical path difference L by geometric relationship and be (AB+BC)-(AD+CD).Calculating this four segment distance respectively obtains:

$\mathrm{AB}=a\sin ({\mathrm{\θ}}_1-{\mathrm{\θ}}_2)\frac{1}{\cos \left({\mathrm{\θ}}_1\right)\cos \left({\mathrm{\θ}}_2\right)},...\left(1\right)$

$\mathrm{CD}=b\sin ({\mathrm{\θ}}_1-{\mathrm{\θ}}_2)\frac{1}{\cos \left({\mathrm{\θ}}_1\right)\cos \left({\mathrm{\θ}}_2\right)},...\left(2\right)$

$\mathrm{BC}=\frac{(a+b)}{\sin \left(2{\mathrm{\θ}}_1\right)},...\left(3\right)$

$\mathrm{AD}=\frac{(a+b)}{\sin \left(2{\mathrm{\θ}}_2\right)},...\left(4\right)$

According to the optical interference theory, when the optical path difference of two bundle coherent lights is the wavelength integral multiple, obtain to interfere maximum value, when optical path difference is the odd-multiple of half-wavelength, obtain to interfere minimal value.If L=m is λ (m is an integer), photodetector will detect owing to interfere m signal maximum and m the signal minimum that produces so, because the rotating speed of tested pointing scan mirror is extremely low, it is that alternately continually varying is similar to sinusoidal waveform that detector will obtain maximin.Any is arranged here is to be worth explanation, and the size of a and b is certain equating among Fig. 3, and this point is easy to proof.

Calculate for example: a=b=0.05m, initial beam incident angle θ ₂=20 °, rotational angle Δ θ=θ ₁-θ ₂=0.01 ° of θ ₁=20.01 °, wavelength is got λ=0.6g μ m, obtains: AB=9.88333082577 * 10 ^-6M, CD=7.45651338489 * 10 ^-5M, AD=0.155572382686m, BC=0.155507700883m, L=1.2936360604631 * 10 ^-4M; We can obtain m=L/ λ ≈ 190, that is to say, when initial incident angle was 20 °, if system rotates 0.01 °, the signal that reflects on detector so will be to occur about 190 to interfere maximal value and interfere minimum value.

We suppose that the rotational angle range of pointing scan mirror is θ ₂→ θ ₁(θ ₁〉=θ ₂), θ ₂, θ ₁It is respectively the incident angle of the successively relative corner cube mirror of transmitted light beam X.Suppose because angle subtle change Δ θ (the incident angle θ of pointing scan mirror ₂Change to θ ₂+ Δ θ) causing change in optical path length just in time is a wavelength, Δ L=(AB+BC)-(AD+CD)=λ, and we obtain the function analytic expression and are:

$\frac{a\sin \left(\mathrm{\Δ\θ}\right)}{\cos ({\mathrm{\θ}}_2+\mathrm{\Δ\θ})\cos \left({\mathrm{\θ}}_2\right)}+\frac{a+b}{\sin ({\mathrm{\θ}}_2+\mathrm{\Δ\θ})}-\frac{a+b}{\sin \left({\mathrm{\θ}}_2\right)}-\frac{b\sin \left(\mathrm{\Δ\θ}\right)}{\sin ({\mathrm{\θ}}_2+\mathrm{\Δ\θ})\sin \left({\mathrm{\θ}}_2\right)}=\mathrm{\λ}...\left(5\right)$

In the following formula, a, b, θ ₂, λ is predetermined amount, and it is exactly Δ θ that our requirement obtains, and it is very difficult that top equation will be obtained analytic solution, but utilizing software to obtain its numerical solution can accomplish.For example utilize the matlab mathematical software, get θ ₂=20 °, a=b=5cm, λ=680nm can obtain Δ θ=0.18936 ".

Equally, because the continuous variation of pointing scan mirror angle is θ in incident angle ₂+ Δ θ changes to θ ₂The optical path difference of+Δ θ+Δ θ ' also is λ, and we can list one as above-mentioned equation, because θ ₂We have calculated+Δ θ, so can obtain the value of Δ θ '.We use (Δ θ) to the Δ θ that calculates above ₁Represent Δ θ ' usefulness (Δ θ) ₂Represent.If have $L_{{\mathrm{\θ}}_1}-L_{{\mathrm{\θ}}_2}=\mathrm{n\λ}$ (the n here can round numbers), we and the like go down, we just can obtain (Δ θ) ₁, (Δ θ) ₂(Δ θ) _nValue.In the test process of reality, (Δ θ) ₁, (Δ θ) ₂(Δ θ) _nBe to calculate in advance to deposit computing machine in.

Fig. 4 is an inversion algorithm analog prober output signal simulation synoptic diagram, and as shown in Figure 4, maximum value is interfered at corresponding one of each paddy peak, and minimal value is interfered in corresponding one of each the lowest point.And can know that by top analysis pairing optical path difference is λ between per two spikes, the angular turn of corresponding pointing scan mirror is followed successively by (Δ θ) ₁, (Δ θ) ₂(Δ θ) _nt ₀, t ₁, t ₂T _N-1, t _nIt is the time information that at every turn interferes maximum value.We just can obtain pointing scan mirror from θ like this ₂→ θ ₁(θ ₁〉=θ ₂) angular velocity information.Computing formula is as follows.

${{\mathrm{\&omega;}}_{\mathrm{<figure-callout\; id="1"\; label="t"\; filenames="A20061003101500132.png"\; state="\{\{state\}\}">t</figure-callout>}}}_1=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_1}{t_1-{\mathrm{<figure-callout\; id="0"\; label="t"\; filenames="A20061003101500122.png"\; state="\{\{state\}\}">t</figure-callout>}}_0};$

${{\mathrm{\&omega;}}_{\mathrm{<figure-callout\; id="2"\; label="t"\; filenames="A20061003101500131.png,A20061003101500132.png"\; state="\{\{state\}\}">t</figure-callout>}}}_2=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_2}{t_2-{\mathrm{<figure-callout\; id="1"\; label="t"\; filenames="A20061003101500132.png"\; state="\{\{state\}\}">t</figure-callout>}}_1};$

${{\mathrm{\&omega;}}_{\mathrm{<figure-callout\; id="3"\; label="t"\; filenames="A20061003101500131.png"\; state="\{\{state\}\}">t</figure-callout>}}}_3=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_3}{t_3-{\mathrm{<figure-callout\; id="2"\; label="t"\; filenames="A20061003101500131.png,A20061003101500132.png"\; state="\{\{state\}\}">t</figure-callout>}}_2};$

${{\mathrm{\&omega;}}_t}_{n-2}=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_{n-2}}{t_{n-2}-t_{n-3}};$

${{\mathrm{\&omega;}}_t}_{n-1}=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_{n-1}}{t_{n-1}-t_{n-2}};$

${{\mathrm{\&omega;}}_t}_n=\frac{{\left(\mathrm{\&Delta;\&theta;}\right)}_n}{t_n-t_{n-1}};...\left(6\right)$

t ₀, t ₁, t ₂T _N-1, t _nCan calculate per two peak-to-peak pulse numbers of paddy and obtain by to the sampling of photodetector output signal.Our hypothesis is treated the angular velocity omega=0.35 °/s of examining system and is at the uniform velocity, gets t ₀=0, the result (Δ θ) who utilizes previous calculations to obtain ₁=0.18936 ", obtains t ₁=(Δ θ) ₁/ ω=1.5 * 10 ^-4S, following table has been listed the sampled point number in first waveform under the different A/D sample frequency.

The A/D sample frequency	The sampling number that waveform is interior
		500K	?75
2M	?300
		5M	?750

The crystal oscillator clock accuracy that can buy in the market is better than 0.1 μ s, the A/D chip that conversion rate reaches MHz also is easy to obtain, referring to Fig. 4, fully can recovery place simulating signal two peak-to-peak samplings of paddy greater than 500 points, and according to the t that how much obtains of shared clock number ₀, t ₁, t ₂T _N-1, t _nTemporal information, so top computing method are feasible fully, by top calculating for example, accuracy of measurement system can reach the rad level.

Fig. 7 has provided the software flow pattern of the digital signal inverting pointing scan mirror motion angular velocity program that has in the PC.Initial angle information (Δ θ) wherein ₁, (Δ θ) ₂(Δ θ) _nBe according to pointing to surface sweeping mirror slewing area θ ₂→ θ ₁(θ ₁〉=θ ₂) depositing PC after the calculating in, the digital signal that obtains through message processing module also deposits PC in as starting condition.Represent the sampling clock cycle of A/D chip in the processing module among Fig. 7 with Δ t, T represents the processing time that message processing module is total, initialization time information t ₀=0, so just can obtain each temporal information t by computed in software _iThe angular velocity information ω at place _iIn subsequent treatment, store ω _iAs y coordinate, temporal information t _iJust can draw the angular velocity curve of pointing scan mirror for the x coordinate.

What deserves to be explained is that more in addition we can adjust the angle of corner cube mirror and rotation mirror to be measured as required, that is to say that even if the angular turn scope of system to be tested changes to some extent, we can still can guarantee initial incidence angle θ ₂Do not change, accomplish that data are reusable.

Claims (2)

1. device that is used to measure angular velocity of pointing scan mirror, comprising: opticator and electronics part is characterized in that:

Opticator is made up of corner cube mirror and two spectroscopes;

The electronics part is made up of laser instrument, unit light electric explorer, message processing module;

Said pointing scan mirror (1) is fixed in the rotating shaft (3), minute surface and rotating shaft axially parallel, and rotating shaft is by Electric Machine Control;

Said corner cube mirror (2) is made up of two orthogonal plane mirrors, and the seamed edge that two catoptrons intersect is fixed in the rotating shaft (3) of pointing scan mirror, and seamed edge is in the rotating shaft coaxial direction, and corner cube mirror and pointing scan mirror angle are fixed;

Said message processing module is by the prime amplifier that becomes circuit to connect successively, filtering circuit, and the A/D conversion, data formatter and PC are formed; Data formatter is made up of extensive Programmable Logic Controller CPLD and two static memory SRAM; There is the motion angular velocity software that digital signal is finally inversed by pointing scan mirror in the PC;

Detector becomes circuit to be connected with prime amplifier;

The light beam that laser instrument (7) sends is divided into transmitted light beam X and folded light beam Y with 45 ° of incident first spectroscopes (4) by first spectroscope, and folded light beam Y, is received by detector through the reflection of second spectroscope again with 45 ° of incident second spectroscopes (5); Corner cube mirror (2) reflection of transmitted light beam X through rotating synchronously with pointing scan mirror through second spectroscope (5) transmission, received by detector again.

2. measuring method of utilizing above-mentioned measurement angular velocity of pointing scan mirror device is characterized in that concrete steps are as follows:

A. the fixing position of corner cube mirror (2) and pointing scan mirror (1), promptly the fixing angle of corner cube mirror and pointing scan mirror is fixed in the rotating shaft (3) seamed edge that corner cube mirror two reflectings surface intersect, and is coaxial with rotating shaft, fixing means can adopt splicing, also can adopt to be spirally connected;

B. light path adjustment: open laser instrument, rotate pointing scan mirror, adjust the position of first spectroscope (4) and second spectroscope (5), observe the exit direction of laser, if this light beam, illustrates first spectroscope and second spectroscopical position along with the rotation direction of pointing scan mirror does not change and adjusts;

C. open message processing module and detector (6), start the motor of pointing scan mirror, pointing scan mirror begins to rotate, PC opening entry photodetector detects, obtain output signal through the message processing module processing, the signal of record is the digital signal of having passed through the data formatter layout, and the motion angular velocity software processes that is finally inversed by pointing scan mirror by the digital signal that has in the PC obtains the magnitude of angular velocity of pointing scan mirror again.

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