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<strong>TPS1100</strong> <strong>Professional</strong> <strong>Series</strong><br />

A New Generation of Total Stations from Leica Geosystems<br />

Karl Zeiske<br />

May 1999<br />

L<br />

MADE TO MEASURE<br />

1


Summary<br />

This report describes the main components of the<br />

new generation of total stations, a further development<br />

of the successful TPS System 1000 series. The<br />

angle-measuring system, the measurement of distance<br />

without the use of a reflector, the automatic<br />

target recognition and the flexible coding are all dealt<br />

with in detail.<br />

The application of new technologies and the implementation<br />

of the wishes of customers across the<br />

globe have led to appreciable improvements in the<br />

operating concept and in the functionality. The resulting<br />

expansion of the range of applications, and the<br />

simplification of procedures, have made it possible to<br />

improve productivity substantially.<br />

1. Overview<br />

The new generation of total stations has been developed<br />

from the successful TPS System 1000 series,<br />

from which it has adopted the most successful features.<br />

Much has been improved, and the functionality<br />

expanded, on the basis of input from customers all<br />

over the world. As a result of new technologies, the<br />

instruments have become smaller and lighter and the<br />

measuring procedures have been accelerated.<br />

The existing operating concept, involving the large<br />

eight-line display and the clear, systematically-arranged<br />

keyboard, has been retained. Years of experience<br />

with the TPS1000 instruments have enabled the<br />

user guidance and the operation to be clarified and<br />

simplified yet further.<br />

Fig 1: Motorized total station with automatic target<br />

recognition and EGL electronic guide light<br />

2<br />

The improved automatic target recognition system<br />

allows higher-speed tracking than was possible with<br />

the TPS1000 instruments.<br />

For the first time, an electronic total station includes<br />

not only the established infrared distancer which<br />

measures to prisms and reflector tapes, but also a<br />

distancer for reflectorless measurement and in which<br />

the emitter projects a visible laser beam.<br />

Other new features are the use of camcorder batteries<br />

as the power supply, the endless fine drives even with<br />

the instrument models which are not motorized, and<br />

the laser plummet permanently in the vertical axis as<br />

a standard feature. The spot brightness of this laser<br />

plummet is adjustable, so that the instrument can be<br />

set up over the ground point quickly and conveniently,<br />

irrespective of the ambient conditions.<br />

Many versions of the instrument are available. The<br />

user can choose the most appropriate of them:<br />

TC….. Classical total station<br />

TCM….. Motorized total station<br />

TCR….. Total station with reflectorless<br />

distancer<br />

TCRM….. Motorized total station with<br />

reflectorless distancer<br />

TCA….. Motorized total station with automatic<br />

target recognition<br />

Each of these versions is produced at four different<br />

levels of accuracy (angle-measuring accuracy in<br />

accordance with DIN 18723 and ISO 12857).<br />

Type 1101 1.5” , 0.5 mgon<br />

Type 1102 2” , 0.6 mgon<br />

Type 1103 3” , 1.0 mgon<br />

Type 1105 5” , 1.5 mgon


2. Measuring angles<br />

In the static, absolute circle-scanning system used,<br />

the coded graduations of a glass circle are read<br />

optoelectronically (fig. 2).<br />

Fig. 2: The circle-scanning principle<br />

Unlike most absolute angle-measuring systems on<br />

the market, where the position has to be decoded<br />

from several parallel tracks, the circle carries only one<br />

graduation track, the code of which continually alters<br />

and contains all of the positional information. This<br />

code is read by means of a linear CCD array and an 8bit<br />

A/D converter, and supplies the approximate<br />

position with an accuracy of around 0.3 gon.<br />

Determining the positions of the centres of the individual<br />

code lines on the array, and then using an<br />

appropriate algorithm to find the mean, produces the<br />

fine measurement. A minimum of ten code lines must<br />

be captured in order to determine the position. In<br />

general, however, a single measurement involves<br />

around 60 code lines, improving the interpolation<br />

accuracy, the redundancy and the reproducibility. The<br />

principle of this angle-measuring system is applied to<br />

all Leica theodolites and total stations.<br />

The value measured for the horizontal direction is<br />

corrected before being displayed or recorded. The<br />

correction is calculated from the following parameters,<br />

as a function of the vertical angle measured:<br />

- the latest collimation error and tilting-axis error to<br />

be determined and stored in the instrument<br />

- the momentary component of the vertical-axis tilt,<br />

transverse to the line of sight.<br />

The vertical angle is corrected by the amount of the<br />

stored index error and by the component of the<br />

vertical-axis tilt in the direction of the line of sight. A<br />

tilt sensor monitors both components of the verticalaxis<br />

tilt. Fig. 3 shows the principle of a tilt sensor, in<br />

which a liquid mirror forms the reference horizon.<br />

<br />

1 - Reticle on prism<br />

2 - Oil surface<br />

3 - Deviating prism<br />

4 - Imaging lens<br />

Fig. 3: Tilt sensor<br />

<br />

<br />

<br />

<br />

<br />

5 - Image of the reticle<br />

6 - CCD linear array<br />

7 - Illuminator (LED)<br />

The reticle (1) located on the prism is illuminated (7),<br />

and is imaged (5) on the linear CCD array (6) by way<br />

of the imaging lens (4) after double reflection at the<br />

liquid surface (2). The triangular line pattern of the<br />

reticle makes it possible to capture both tilt components<br />

by means of just one unidimensional receiver.<br />

Longitudinal tilt alters the spacing between the differently-oriented<br />

lines; transverse tilt shifts the centre of<br />

the entire line pattern along the CCD array.<br />

This arrangement enables the tilt sensor to be made<br />

so small that ideally it could be placed centrally over<br />

the vertical axis. The liquid mirror would then be<br />

displaced from its horizontal position only very<br />

slightly, even during rapid rotation of the alidade.<br />

Also, the tilt measurement can no longer be affected<br />

by other factors such as the temperature-related<br />

deformation of the theodolite standard.<br />

<br />

3


3. Measuring Distance<br />

Two coaxially-measuring distancers are incorporated<br />

into the TCR instruments (fig. 4). Both distancers<br />

operate on the well-known phase measurement<br />

principle.<br />

The infrared laser beam for measuring distances to<br />

prisms and reflector tapes has a wavelength of<br />

780nm, a range of 3000 metres with a single prism,<br />

and an accuracy of 2mm + 2ppm. The visible red laser<br />

beam has a wavelength of 670nm and measures<br />

distances of up to 80 metres with an accuracy of 3mm<br />

+ 2ppm without using a reflector.<br />

Fig. 4: Optical design of a total station measuring without reflector<br />

The unambiguity of the distance measurement up to<br />

12km is assured by a special frequency system. Its<br />

base is a frequency of 100MHz, corresponding to a<br />

measuring scale of 1.5m.<br />

The “Long Range“ measuring mode can be engaged<br />

for long distances. With it, the red laser beam can<br />

also be used to measure to prisms at a distance of<br />

between 1000 metres and 5000 metres.<br />

A keystroke will switch between the two distancers<br />

immediately and at any time. The correct zero-point<br />

correction (additive constant) is set automatically.<br />

This combination of two distancers in a single total<br />

station, achieved now for the first time, offers great<br />

advantages where the points to be measured are<br />

4<br />

Reflector, target<br />

Laser for<br />

reflectorless<br />

measurement<br />

Laser for<br />

reflectorsupported<br />

measurement<br />

accessible only with difficulty or not at all, for example<br />

on frontages, during control measurements on<br />

steel constructions, and in determining lengths of<br />

conduits. The visible red laser beam can also be<br />

switched on permanently for marking target points,<br />

e.g. for profile surveys in tunnels or for indoor surveys.<br />

At a distance of 50 metres the laser dot has a<br />

size of approximately 1cm x 2cm.<br />

Receiver<br />

diode<br />

Motor<br />

Graded filter / internal light path<br />

Telescope of total station


4. Automatic target recognition<br />

4.1 The Principle<br />

Automatic target recognition (ATR) is incorporated<br />

into the telescope in the same manner as is the EDM.<br />

An infrared laser beam is projected coaxially into the<br />

telescope axis by means of optical components and<br />

emerges from the main objective. A beam splitter<br />

separates the reflected beam of the ATR from the<br />

EDM beam and from the visible light, and guides it to<br />

the receiver (the video sensor).<br />

Special hardware adds the intensities of the elements<br />

of the video sensor in rows and in columns, resulting<br />

in two “projections”. The centres of these are determined<br />

by a processor and are then transformed into a<br />

horizontal and a vertical angle of correction with<br />

regard to the visual line of sight. These angle corrections<br />

are used to correct the values relating to the<br />

visual line of sight, as measured by the circle-scanning<br />

system.<br />

4.2 Fine pointing<br />

Three sequentially-running processes characterize the<br />

fine pointing: the search process, the targeting process<br />

and the measuring process.<br />

After the coarse manual pointing of a prism, the fine<br />

pointing with the help of ATR is completely automatic.<br />

ATR first checks whether the coarsely-targeted<br />

prism is located within the field of view of the telescope.<br />

If it cannot detect the prism, it commences a<br />

search procedure involving a continuous spiral movement<br />

of the telescope. The speed of this scan is<br />

selected so that there are no gaps between the individual<br />

images in the area scanned. The telescope<br />

stops moving as soon as the prism has been detected.<br />

When using the ATR measuring technique, it is not<br />

necessary to target the prism centrally in order to<br />

determine the horizontal direction and the vertical<br />

angle. Nevertheless Hz and V angle corrections are<br />

determined during the subsequent targeting process<br />

when the motor moves the telescope so that it points<br />

to the centre of the prism within the predetermined<br />

tolerance limits.<br />

There are two reasons for this: firstly, so that the user<br />

can confirm the correct automatic targeting by visual<br />

observation and secondly, so that a distance can be<br />

measured at the same time. ATR requires one prism<br />

for target identification and so, to simplify operation,<br />

the ATR angle measurement has been coupled to the<br />

triggering of a distance measurement.<br />

During the measuring procedure, angle corrections<br />

are redetermined, the horizontal and vertical angles<br />

are corrected appropriately, and the distance is<br />

measured or the target-point coordinates are calcu-<br />

lated. Fig. 5 shows the sequence of an ATR measurement<br />

procedure.<br />

The measuring accuracy of ATR in its standard setting<br />

corresponds to the angle-measuring accuracy of the<br />

corresponding instrument model. If a distancemeasuring<br />

mode different from the standard one is<br />

selected, the accuracy of the ATR measurement<br />

adapts to the accuracy class of this measuring mode.<br />

In, for example, the distance-measuring mode “Fast“,<br />

this shortens the measuring time and enables the<br />

measurement to be carried out on unstable, handheld<br />

reflectors at close range.<br />

When ATR is used for measuring, there is no need to<br />

focus the telescope or to fine-point the target, and so<br />

the speed of measurement is increased enormously<br />

and the precision, which is independent of the observer,<br />

remains constant.<br />

4.3 Tracking the target<br />

Tracking is essentially an automatic control system,<br />

or feedback loop (fig. 6). The theodolite drive, the<br />

control range, consists of two axes each with a servomotor,<br />

a transmission and a circle-scanning system.<br />

The ATR is a measuring system, which supplies not<br />

only the actual values, but also the deviation between<br />

actual and required values and the horizontal and<br />

vertical corrections from the electronic or optical line<br />

of sight. The automatic control system is intended to<br />

minimize the deviations, irrespective of the speed and<br />

acceleration of the target. The deviations are read off<br />

at the video rate; from them, the circuit determines<br />

the currents needed by the motor in order to attain<br />

the set goal.<br />

This procedure runs continuously throughout the<br />

tracking phase. If contact with the target is lost, e.g. if<br />

the reflector carrier passes behind an obstacle, the<br />

tracking process is interrupted. The values that then<br />

become effective instead of the deviation values are<br />

based on a movement model, which assumes the<br />

horizontal and vertical speeds of the reflector carrier<br />

to be constant. These speeds are derived from the<br />

filtered movement before loss of contact. Filtering<br />

serves to eliminate superimposed frequencies such<br />

as the vertical component of walking. Because the<br />

model is just an approximation of the movement, it is<br />

applied only for a period of a few seconds.<br />

If measurements are triggered parallel to the tracking<br />

process, the course of the moving target can be<br />

determined. The time synchronization of the individual<br />

sensors of the total station has a considerable<br />

influence in this application. The measuring systems<br />

are integrated for different periods, and so the true<br />

time at which they are determined has to be established<br />

and then interpolated or extrapolated to a<br />

common point in time.<br />

5


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Fig. 5: The sequence of an ATR measurement<br />

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Fig. 6: Feedback loop of target tracking<br />

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5. Remote control<br />

The remote-control system RCS1100 is an additional<br />

option for all Leica total stations. It is particularly<br />

efficient in conjunction with instruments that have<br />

automatic target recognition. The controller, battery,<br />

radio modem and antenna of the RCS1100 form a<br />

compact unit, which fits easily to a reflector pole (fig.<br />

7). The display and keyboard of the controller are<br />

identical to those of the total station, and so all instrument<br />

functions, including the applications programs,<br />

can be called up from the target area.<br />

Fig. 7: RCS1100 remote control system<br />

The remote control system makes it easier to capture<br />

important additional information at the target area in<br />

particular, and offers great advantages during stakeout.<br />

After a measurement, the path difference from<br />

the reflector to the point to be set out is calculated<br />

and is displayed on the controller. This facilitates and<br />

accelerates the stakeout procedure, and also enables<br />

the accuracy of the stakeout to be inspected directly<br />

from the target area.<br />

The EGL electronic guide light provides additional<br />

help during stakeout; it is a flashing light source,<br />

which can be built into any telescope housing (fig. 1),<br />

and enables the reflector carrier to be aligned with the<br />

line of sight of the instrument.<br />

6. Software<br />

The entire software for the <strong>TPS1100</strong> instruments can<br />

be roughly divided into three groups:<br />

- The systems software for controlling all basic<br />

functions of the total station<br />

- The comprehensive library of applications programs<br />

- The LEICA SurveyOffice, PC programs package for<br />

communication between instrument and computer.<br />

6.1. System software<br />

The system software controls all measurement<br />

functions, the display and the recording. For each<br />

dialogue in the display (e.g. measuring, data management,<br />

calibration etc.), the function keys are occupied<br />

by the appropriate relevant function. This ensures<br />

ideal user guidance along with quick and easy operation.<br />

All measurement sequences, and the functions which<br />

can be called from the various dialogues, are logically<br />

arranged. They can also be configured and so<br />

matched to individual user requirements.<br />

In the measuring dialogue, three different display<br />

templates can be defined; a keystroke switches<br />

between them so that the user has an overview of all<br />

important data.<br />

Five different recording templates can be defined<br />

quite independently of the display templates. 12<br />

items of data in any sequence can be recorded in any<br />

one measuring block. There is a choice between data<br />

formats containing either 8 or 16 characters per data<br />

word.<br />

All data can be stored on PCMCIA memory cards in<br />

various files, or can be exported via the RS232 interface<br />

to an external computer. Up to 60 files can be<br />

managed; they can be given any name. A distinction<br />

is made between measurement files for storing<br />

measurements, files with fixed-point coordinates,<br />

and code lists.<br />

Code lists with additional information for the postprocessing<br />

of measurement data can be imported<br />

directly through the keyboard into the instrument, but<br />

it is preferable to compile code lists on a PC with the<br />

program “Codelist Manager” from the Leica Survey<br />

Office and then to import this into the instrument.<br />

For standard coding, the appropriate code is selected<br />

from the list and then stored in a separate code block.<br />

A code block can contain a code and up to eight<br />

additional items of information. If no code list has<br />

been stored in the instrument, code blocks can also<br />

be entered manually via the keyboard and stored.<br />

7


Rapid coding (“Quick-Code”) is a special function<br />

with which a keystroke triggers a measurement, after<br />

which the measurement block and the corresponding<br />

code block are recorded automatically. To do this, a<br />

single-digit or two-digit number must be allocated to<br />

each code as a quick-code abbreviation when the<br />

code list is compiled with the “Codelist Manager” PC<br />

program. After the point has been targeted, it is<br />

enough to enter this number using the numeric<br />

keyboard. This action triggers a distance measurement,<br />

and stores the complete measurement block in<br />

accordance with the recording template selected and<br />

with the associated code block from the code list. The<br />

user can decide whether the measurement block or<br />

the code block should be the first to be stored.<br />

Point-related codes, and also up to eight attributes,<br />

can also be recorded along with each measurementdata<br />

block. The input is directly through the measurement<br />

dialogue. The precondition for this is that the<br />

point code and the attribute are defined both in the<br />

display and in the recording template.<br />

6.2. Applications programs<br />

To deal with the most important tasks in surveying,<br />

the following applications programs are incorporated<br />

into all instruments:<br />

Horizontal-circle orientation and height transfer<br />

Resection<br />

Free-station survey<br />

Setting out (stakeout)<br />

Computation of tie distance<br />

Remote height<br />

The user can load the following optional programs at<br />

any time:<br />

Reference line<br />

Area computation<br />

Hidden points<br />

Sets of angles<br />

Traverse<br />

Local resection<br />

Road stakeout<br />

File Editor<br />

COGO functions<br />

Auto Record (acceleration of mass point surveys)<br />

Face Scan for TCRM instruments<br />

DTM stakeout<br />

Leica offers GEOBASIC, a modern development<br />

environment within which users can develop their<br />

own individual applications programs.<br />

Printed in Switzerland. Copyright Leica Geosystems AG, Heerbrugg, Switzerland, 1999<br />

712705en - V.99 - RVA<br />

8<br />

6.3. LEICA SurveyOffice<br />

The LEICA SurveyOffice is a PC software package<br />

with the following functions:<br />

- Exchange of data between instrument and PC<br />

- Creation of code lists universally usable in the<br />

TPS300 instruments, the <strong>TPS1100</strong> instruments and<br />

the new GPS500 system<br />

- Loading and deleting systems software and applications<br />

programs and related display texts in various<br />

languages.<br />

Leica Geosystems AG<br />

Geodesy<br />

Heinrich-Wild-Strasse<br />

CH-9435 Heerbrugg<br />

Switzerland<br />

Phone +41 71 727 3131<br />

Fax +41 71 727 4702<br />

www.leica-geosystems.com

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