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標(biāo)校經(jīng)緯儀航向標(biāo)定修正方法

2011-11-06 05:49:02高慧斌
中國(guó)光學(xué) 2011年6期

李 淼,高慧斌

(1.中國(guó)科學(xué)院長(zhǎng)春光學(xué)精密機(jī)械與物理研究所,吉林長(zhǎng)春130033; 2.中國(guó)科學(xué)院 研究生院,北京100039)

1 Introduction

Calibration theodolite is an important device for the heading calibration of spacecraft TT&C(Telemetry,Track& Command).It is used for precision calibration when the spacecraft is at a dock or a deport[1-2].During the manufacture of spacecraft,the reflection mirror is put into the inertial navigation hanging cular,which stands for the straight north of inertial navigation.The azimuth datum mirror is put onto the theodolite platform,then we make the two mirrors'normal direction in parallel to stand for spacecraft TT&C's heading direction.When the theodolite is imported onto the ship,we need to make the calibration theodolite's azimuth encoder zero angle line and the azimuth datum mirrors'normal direction alignment before we do other measurement work.However,in practice,there are single errors.We can only get the precision heading data until all the single errors have been corrected.With the precision heading data,we can build the ship's azimuth datum to ensure fulfillment of the measurement mission.

2 Heading calibration system for spacecraft TT&C theodolite

The spacecraft TT&C theodolite's heading calibration system can be described as Fig.1[3-4].

The whole system consists of a calibration theodolite,a theodolite platform,a hanging cular and a inertial navigation system.The hang cular reflection mirror is put into the hang cular of inertial navigation,and the mirror's normal direction stands for the direction of inertial navigation.The azimuth datum mirror is equiped on the theodolite platform,which makes its normal direction parallel with the reflection mirror's normal direction.During the calibration process,the azimuth datum mirror's normal direction is considered as the ship's azimuth direction.When the theodolite is imported onto the ship,we use one 0.2″collimator tube and two reflex lighttubes to align the hang cular reflection mirror,azimuth datum mirror as well as calibration theodolite's azimuth zero angle line[3-5].

Fig.1 Heading calibration system and optical path of calibration theodolite

3 Influence of theodolite single error on azimuth measurement

The calibration theodolite uses the horizontal structure which has three main axes:horizontal,vertical and collimating.Since the limitation of manufacture and adjustment using factors,the three axes are not vertical with each other.So there is an angular measurement error,and we called it axis error,including horizontal error,vertical error as well as collimating error[6-7].They all have influence on the azimuth measurement.In this paper,we just only focus on the influence of collimating error,and neglect others.

3.1 Collimating error

The theodolite's collimating axis is not vertical to the horizontal axis and it will form an angular measurement error which is called sighting error and standed byC.The theodolite uses a positive and inverse mirror to point on the horizontal object to measure sighting errorC.By setting the positive azi-muth angle reading asApositive,and the inverse azimuth angle reading asAinverse,then we get the sight error as Eq.(1):

It can be proved that the influence of a sight error on the azimuth measurement is[6-7]:

whereEnis the elevation angle of measurement object.

3.2 Orientation error of azimuth encoder

When the theodolite's optical axis points on the orientation direction(usually,we use the north as the orientation direction),the angle between azimuth encoder zero angle line and orientation line is azimuth encoder reading,and we call it orientation error,and use thegto stand for it[6-7].In practice,we use ground azimuth flag to orient,and set the ground azimuth flag relative to equipment's azimuth angle asA0.We make the theodolite point on this flag,and the azimuth encoder's reading isAi,that is:

The orientation error reveals that the azimuth encoder's zero angle line and the set zero angle line is inconsistent.That is to say the start line of azimuth angle is not precision.And the orientation errorgis an constant which can only be measured and corrected but not be eliminated[7].

The orientation errorgis measured by the positive and inverse mirror method[7].Provided that there is a horizontal object in the straight north,with the positive pointing reading asApositive,and inverse pointing reading asAinverse,and then the orientation error is:

4 Headingcalibration mathematic modeland heading correction method

In the third part,we talk about the sight error,azimuth encoder orientation error and their measurement methods as well as their influences on azimuth measurement.The above analysis based on the hypothesis shows that there is one item error without other errors.

However,in practice,the equipment's three axes are closely related with each other,as for a specific equipment,these item errors are in existance simultaneously.

In this part,we focus on the heading correction mathematic model and correction method with sight errorCand orientation error considered.

The spacecraft TT&C's heading calibration system is shown in Fig.1.During the manufacture,the azimuth datum mirror's normal direction has been already considered as the orientation directionN.When the calibration theodolite is imported onto the ship,we use one 0.2″collimator tube and two reflex light-tubes to make the azimuth datum mirror's normal direction and the theodolite's optical axis aligned.By clearing the azimuth encoder reading to zero,at this timegis equal to zero.

However,in practice,the equipment's orientation error will be changed with time.With the spacecraft TT&C at a dock,we use the above calibration tools to make optical axis point on the azimuth datum mirror's normal direction,then get the orientation error according to the formula(3),and set it asg.With the positive and inverse mirror method,we get the sight error,and denote it to beC.And their relationship is shown in Fig.2.

Fig.2 Calibration relationship at dock

In actual measurement,the theodolite has sight and orientation errors.The two item errors are all needed to be corrected[8-9].

Setting the azimuth measurement reading asAce,and the corrected data asAcorrect,we consider the sight errorCand orientation errorg(since the influence of transfer error from a reflex light tube is known and has been discussed precisely.So we neglect it.),then the correction model is:

With formula(5),we correct the sight error and analyze influences of orientation error on azimuth measurement and complete the heading calibration work[8-9].

On the spacecraft TT&C,we usually use positive mirror pointing method to measure the orientation error,and the analysis is as follows:

Provided the theodolite has a sight errorC,with positive mirror pointing method,we get the orientation errorg,and their relationship is shown in Fig.3.

Fig.3 Measurement of orientation error with positive and inverse methods

When the optical axis points on the azimuth datum mirror's normal direction,the azimuth encoder's reading is:

Then inverse the system,the theodolite needs to be turned 180°-2C,then points on azimuth datum mirror's normal direction,that is:

According to the formula(4),we can get the orientation errorg',then

From the formula(8),we arrive that considering sight error and orientation error,the result of orientation error measurement by using the positive pointing method is equal tog-C.

If we use positive pointing method to measure orientation error,the heading calibration correction model is:

Compared with the formula(5)and formula(9),they are the same.That is to say the two correction models are equal with each other.

5 Experimentsand measurement results

With the 2010's heading calibration measurement at the dock,and the azimuth datum mirror as the azimuth datum,we got the measured and computed data which are shown in Tab.1.

Tab.1 Measurement and computing results

With the positive and inverse pointing to compute the orientation error:

The measurement and computing results reveal that the two methods are consistency and reasonability.

6 Conclusion

In this paper,we focus on the heading calibration at the dock.The principle and method of heading calibration have been discussed in detail and the following main results are obtained:

(1)The heading correction mathematic model is built by considering theodolite's sight and orientation errors;

(2)Two methods for measuring the orientation error is presented.One is positive and inverse pointing method and the other is positive mirror pointing method.We analyze the differences and relationships of two methods,and develop the two correction formulas;

(3)The consistency and reasonability of two correction methods in different situations are proved.

The research in this paper can be used as spacecraft TT&C heading calibration at the dock,and it provides a constructive reference for other calibrations.

[1]PAN L.The Position Measurement Technology for Space Instrument Ships[M].Beijing:National Defence Industry Press,2009.(in Chinese)

[2]JIAN S L.The Introduction of Maritime Tracking Technology for Space Instrument Ships[M].Beijing:National Defence Industry Press,2009.(in Chinese)

[3]Rules for the Implementation of Calibration for Space Instrument Ships at Dock[M].No.23 Base,2001.(in Chinese)

[4]The Layout Calibration Scheme for Space Instrument Ships at Dock[M].No.23 Base,2007.(in Chinese)

[5]ZHANG S L.The Data Process Method for Space Instrument Ships[M].Beijing:National Defence Industry Press,2009.(in Chinese)

[6]WANG J Q.The Layout Design of the Optical Instruments[M].Changchun:Changchun Institute of Optics Fine Mechanics and Physics,Chinese Academy of Sciences,2003.(in Chinese)

[7]WANG J Q,ZHAO X Y,LI Y C.Optical Measuring in Shooting Range[M].Beijing:Academy of Equipment Command &Technology,2001.(in Chinese)

[8]WANG M,HU S L.Range Data Processing and Error Analysis[M].Beijing:National Defence Industry Press,2008.(in Chinese)

[9]HE Z C,HU G A.Optical Measurement System[M].Beijing:National Defence Industry Press,2002.(in Chinese)

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