Inhaltsverzeichnis
Hallo und Willkommen !
Eine sehr kurze Zusammenfassung:
Ein Tachymeter ist ein Gerät zur Vermessung der geografischen Lage
von Gebäuden, Grundstücken, Bergen, Tunneln usw, d.h. ein Werkzeug der Geodäsie.
Technisch ist das ein Theodolit kombiniert mit einem Entfernungsmesser.
Die Geräte werden auch als "Totalstationen" bezeichnet, da sie die Lage eines Punkts "total" bestimmen können, d.h. mit 2 Winkeln und einer
Streckenlänge (Kugel-Koordinaten).
Kurz&gut: Auf jeder Baustelle, von der PKW-Garage bis zum Gotthard-Basistunnel, werden Tachymeter verwendet, um Bauwerke dort hin stellen, wo sie hin sollen.
Viele traditionelle Aufgaben der Vermessung werden heute zwar von Satelliten-gestützter Technik (GNSS, mit dem Spezialfall GPS) erledigt. Das ist deutlich schneller, aber nicht überall einsetzbar: An Orten ohne Satelliten Empfang (in Häuserschluchten, Wäldern, Tunneln, oder Bergwerken) oder ohne einen notwendigen, zusätzlichen Mobiltelefon-Empfang für die genauen Echtzeit-Korrekturdaten, ist Satelliten-gestützte GNSS/GPS im Zentimeterbereich und darunter nicht anwendbar. Zudem sind Tachymeter meist genauer, zumindest die des oberen Preis-Segments.
Bevor es Geräte ohne eingebauten elektronischen Entfernungsmesser gab, also etwa vor 1950, war die Bestimmung von Längen und Entfernungen in
der Geodäsie außerordentlich mühsam: Der einzig genaue Weg war das Aneinanderlegen von genauen, temperatur-stabilen Messlatten auf einer
horizontalen Referenz-Strecke. Das ist zwar machbar, aber sehr aufwendig, unter anderem deshalb, weil erstmal eine horizontal Schneise
zwischen zwei Punkten erstellt werden musste. Das Britische Empire hat von 1802 bis 1852 in dieser Art
ganz Indien vermessen. Das gleiche war zuvor in Europa erfolgt.
Die Vermessung der USA verlief ähnlich. In allen Fällen übrigens mit auch heute noch beeindruckender Genauigkeit.
Die ersten opto-elektronische Entfernungsmesser nach 1960 waren bahnbrechend im Vermessungswesen, da sie genau und schnell waren,
zudem einfacher in der Anwendung. Die ersten Vorläufer, nach 1950, verwendeten noch
Radiowellen im Mikrowellenbereich, und waren daher schwerer und unhandlicher. Die heutigen (2021) Laserentfernungsmesser, nun
erhältlich in jedem Baumarkt, sind deren Urenkel.
Der Fokus dieser Webseite liegt auf Instrumenten der Firma Carl Zeiss in Oberkochen, mit Herstellungsjahr etwa von 1960 bis 2000.
Damit umfasst sie zeitlich die ersten Geräte der westdeutschen Zeiss Werke bis zur Abgabe des Geschäftsbereiches Geodäsie an die Firma Trimble.
Die meisten Tachymeter dieser kleinen Sammlung sind in funktionsfähigem Zustand und getestet.
Links zu einigen anderen Sammlungen Geodätischer Instrumente, die allerdings einen anderen Fokus haben, sind unter "Verschiedenes" aufgeführt.
Diese Webseite ist mittlerweile etwas umfangreicher geworden und wurde daher unterteilt. Ein click auf das Inhaltsverzeichnis auf der linken
Seite wählt einzelne Rubriken.
Inhaltlich Anmerkung: Der Seiteninhalt wurde ursprünglich von mir in Englisch geschrieben, und erst nach-und-nach gibt es die Rubriken auch
in Deutsch. Mea culpa.
Technische Anmerkung: Die Auswahl-Funktion benötigt derzeit Javascript.
| type | Reg Elta 14 | SM4 | Elta 2 | Elta 42 | Elta 3 | Elta 4 | Rec Elta RL | Rec Elta 13 | Rec Elta 15 | Elta S10 | Elta S20 | Trimble 5603 DRE200+ with Zeiss interface unit | |
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| series | 1st | 2nd | 3rd | economy branch | "E series" | "Rec-Elta series" | "S series" | ? | |||||
| manufacturer | Zeiss (West, Oberkochen) | Zeiss (unified, Jena) | Zeiss/Trimble (Jena) | Spectra-Precision/Trimble (Sweden) and Zeiss (UI) | |||||||||
| approximate year of production | 1968+ | mid 1970 | 1978+ | early 1980 ? | 1985+ | 1985+ | 1990+ | 1990+ | 1993+ | 1998 - 2000 ? | 2001+ | ||
| nominal angular precision | 1 mgon (3.2″) | 1 mgon (3.2″) | 0.2 mgon (0.6″) | 5″ | 1.5″ | 3″ | 1.5″ V, 2″ H | 1.5″ | 3.0″ | 1″ | 3″ | 3″ | |
| angular compensator | one axis | ? | at least one axis | -none- | two axes | one axis | ? | two axis | two axes | two axes | |||
| distance precision | ? | ? | 5-10 mm + 2ppm | 5-10 mm + 2ppm | 3mm + 2ppm | 3mm + 3ppm | 5mm + 2ppm | 2mm + 2ppm | 3mm + 2ppm | 1mm + 2ppm | 2mm + 2ppm | 3mm + 3ppm | |
| telescope magnification | 25x | 25x | 30x | 28x | 30x | 30x | ? | 30x | 22x | 30x | 30x | 26x (30x optional) | |
| options | - | - | pluggable firmware and storage modules | - | external laser pointer | - | CM/CMS version with motorised axes, slip-ring |
Track (co-axial CCD for prism lock/track), Arc (wireless), Space (extra sensor to find prism) | wireless control, laser pointer, tracker (both not co-axial) | ||||
| optical sighting indicator for stake-out work | no | red/green: left/right blink frequency: distance | yes | ||||||||||
| reflector-less | no | yes (prism not recommended under 50m) | no | yes | |||||||||
| built-in optical plummet | no | yes | no | ||||||||||
| angular encoder type | relative | absolute | |||||||||||
| motorised axes "robotic" | no | CMS version | yes | ||||||||||
| user interface (hardware) | rotary/dip switches Nixie tubes | rotary/dip switches LED 7-segment | rotary/dip switches LED 7-segment | rotary/dip switches 3x LCD | two 4 line x 9 character alpha-numeric LCDs 3 buttons | 240 x 38 pixel, 4 line alpha-numeric LCD 24 keys | 320 x 80 pixel LCD, QWERTY keyboard | 320 x 80 pixel LCD, QWERTY keyboard (detachable) | |||||
| op-sys | Zeiss firmware | MS-DOS | |||||||||||
| internal storage of points | no | yes MEM200,MEM800 | ? | no | yes | ||||||||
| PC interface (hardware) | 5bit tape puncher | none | MEM modules, RS232 | RS232 , 1200,2stop,7bit+odd | RS232 , 1200,2stop,7bit+odd | RS232 , configurable | RS232 , configurable
PCMCIA flash card, optional wireless | RS232 , configurable
PCMCIA flash card | |||||
| original battery pack | external NiCd 12.5V 17Ah "Ramert DEAC 12 Z D19" | Zeiss 708110 7.2V, 700911 7.2V | Zeiss 708152 4.8V 1800mAh NiCd, 705351-9020 4.8V 2400mAh | Zeiss 702710-9030, 6V 3500mAh NiMh | ? | ||||||||
| original charger | ? | Zeiss LG 4, LG 7, (?) | Zeiss LG 9 | Zeiss LG 20 | ? | ||||||||
| replacement cells | probably any 12V source with suitable current | 6x 1.2V NiCd size C | 4x NiCd, diameter 26mm, height 50mm, e.g.: Sanyo/Panasonic KR-CH(2.5) 2500mAh or N-3000CR 3000mAh | 5x NiMh e.g. Panasonic HHR380A-LF 1.2V 3800mAh | 12V gel/AGM Pb-battery | ||||||||
| case L x W x H [cm] | Al - | dark grey plastic 46 x 38 x 25 | yellow plastic 55 x 40 x27 | yellow plastic 41 x 22 x 29 | light grey plastic/Al 50 x 37 x 25 or yellow plastic | yellow plastic 47 x 42 x 28 | yellow plastic 38 x 30 x 50 | ||||||
Zeiss (West) had built a lot more models: For example the early S11 (Elta14 w/o electronic angular reading), the Eth 2/3/4 (on the market at the same time as Elta2/3/4 "E-Series", with a different display, the same type of chassis shape, but without distance measurement), Elta 13, Elta 6, Elta 40, Elta 46, RecElta14, C30 (successor of the S20 ?, no QWERTY keyboard), or the "R" (Routine) family, R45,R55,R50, an economic newer series, already built in partnership with Spectra Precision.
The names of the instruments by Zeiss Oberkochen can be a bit confusing:
The names "Elta 2", "Elta 3" and "Elta 4" may refer to instruments in different series: There are "Elta 2,3" in the first series, after the
initial Elta14 , and the newer "Elta 2,3,4" models of the "E-Series", as shown in table above. They have radically different internal
electronics, battery voltages and user-interfaces. With both series, the lower number has better angular resolution and a higher price.
Similar, a fellow-up to the "SM4" was, according to a Zeiss publication of 1978, named "Elta 4" too at the time. Additionally to the "SM4" it
had electronic angular read-out and was marketed as the low-precision version of the then "Elta 2". So the name "Elta 4" may refer to one of three
completely different instruments, depending on the decade of its manufacturing.
The rather coarse "Elta 42" (and "Elta 46" ?) had been a short-lived low-cost branch in the Zeiss product spectrum, - I have to update this description here with some new information ASAP.
And furthermore, in parallel to Zeiss Oberkochen (West Germany, BRD, ''Federal Republic of Germany''), there had been a product range of Zeiss Jena (East Germany, DDR, ''German Democratic Republic'') between 1946 and 1999 as well. Zeiss Oberkochen and Zeiss Jena had been fierce competitors on the world market during the era of the "Cold War". There are a couple of symmetries: Zeiss West supplied the Elta14 to the Olympics (distance measurements in javelin throw, etc) in Munich 1972 and Zeiss Jena had their tachymeters at the Olympics in Moscow 1980. In their time, both had been at the high-end of electro-optics.
For older S10/S20 with "PC-Version 1" hardware, there are issues with CFCARD-to-PCMCIA adapters (see section on PCMCIA). And the older "PC-Version 1" hardware is terribly slow, likely due to a very slow 86286 CPU: A lot of patience is required when operating an S10/S20 with "PC-Version 1" in the field.
Update: Most instruments of my collection have been donated to the archive of Zeiss Jena in May 2022.
source: Zeiss manual Rec-Elta
The Trimble 5603 is the odd one on this list: The base unit was made by Spectra Precision AB, Sweden, and has, as far as I know, nothing to do with Zeiss. Notably, some details and concepts differ: e.g. the motor drive of both axis are different to the S20 (worm-gear with slip clutch at 5603, radial tooth gears on S20), the 5603 doesn't have a built-in optical plummet, it lacks removable batteries (when using the track option), the ocular is off-centre indicating a different internal beam path, etc.
The Series 5600 by Spectra Precision (later Trimble) featured a modular design and it offered four different detachable user interfaces units. One type of these units was marketed as Zeiss Elta / Open System Control Unit (Elta-CU), carries a Zeiss logo and looks the same as on the S20. Available programs on this unit either have a look&feel of Zeiss Elta or of Trimble. Users of an Elta S10/S20 will find this identical to operate. A nifty idea to separate the software look&feel from the underlying hardware. The Zeiss-CU is "Made in Sweden".
My 5603 came "naked", without batteries, cables or remote control, hence it needed some background research:
The type of push-pull-4-pin connector used on the Trimble 5603 and its Zeiss user-interface is Hirose HR10A-7P-4P (low-cost version) or
Hirose HR10-7P-4P , e.g. available from
Digikey.
The socket at the 5603 dismounts easily and reveals a little PCB with a 3.5A SMD fuse, from which the pin functions can be deduced.
Note that the number on the PCB close to the socket is not the pin number of the Hirose socket.
This wiring, shown in the image, works for me (see photo), but no warranty for the pin numbers (see Hirose HR10_catalog.pdf):
pin4: GND green/blue; pin3: 12V yellow/red; pins 1,2 are likely the RS232 interface.
This type of socket is, IMHO, mechanically a little frail for this task and it may break if the cable is pulled strongly by accident. This specific socket showed a crack already, when viewed under a microscope. It is a good idea to add a strain relief at the tripod close to the 5603. But of course, that depends on where the battery is placed.
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Power consumption was found to be 1A to 1.4A at 12V DC (12-17W). The 5603 is sensitive to under-voltage and draws a surge at power-on:
It required at least 12.4V to boot when connected via a 1.5m cable of 0.14mm cross-section, powered by a professional power-supply.
Booting did fail on a consumer-grade lab power-supply, which couldn't balance the initial power surge, although it is rated to drive 3A maximum.
If an Elta-CU does boot when powered directly, but does not boot when powered by the Trimble main connector, it could be a problem with
the initial current surge. The maximum cable outer diameter of the Hirose plug is 5mm, which limits the wire diameters and hence the cable
length.
For those not happy to do soldering themselves, - there's a market out there offering ready-made cables and custom batteries.
The Elta-CU has one internal NiMH back-up battery, 5x AAA-size, 6V , and 2x 3V Li coin-cells, soldered on-board. The correct procedure for replacement is yet unclear, - disconnecting them may void RAM-stored programs or parameters, and may brick the 5603.
| station name | LG4 | LG6 | LG7 | LG9 | LG10 | LG20 |
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| number | 708105 | 708112 | 708107-9901 | 708150 | 708100 | |
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| charger for REC500, according to Zeiss list | 
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| fitting battery type number | 708110 | 708111 | 708110,700911 | 708151,708152 | - | 702710-9030 |
| cell type | NiCd | NiMh | ||||
| number of cells | 6 C-size | 5 AA-size | 6 C-size | 4 C-size | 4 AA-size | 5 |
| nominal voltage [V] | 7.2 | 6 | 7.2 | 4.8 | 4.8 | 6 |
| photo of battery pack | 
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The following internal batteries have been found in an Elta-3, presumably they power the SRAM with the calibration data. Loss of the Lithium power could mean that the instrument is "bricked". They are located on the inner side of the PCB that is mounted underneath the socket of the main external battery. Exchanging them requires de-soldering the contacts and may need an auxiliary power supply while doing so.
The two internal CR2430 Li 3V batteries were found at 0.2V each, and replaced by new batteries of the same type.
Note that there are different types of soldering lugs available with this type of battery (pins, dual pins, lug).
The exact purpose of these batteries remain unclear: RT-clock, SRAM, ''NVRAM'' ?
At least the system was bootable with the old batteries, and after replacing one-at-a-time, it still booted OK.
Exchanging them was relatively straight-forward, using a vacuum de-soldering equipment is a plus.
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Keeping a legacy electronic tachymeter in working condition becomes increasingly problematic. Compared to their non-electronic forerunners they pose a few extra problems:
This situation with legacy Zeiss-West instruments is worse than the one with Swiss-made legacy Kern instruments, where enthusiasts run a detailed and open archive.
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Work is currently (2016) under way here on a mechanical replacement for the original 4.8V battery packs.
The original packs consist of two extrusion molded halves, glued together. Their shape is deteriorating after opening and re-sealing
multiple times for exchanging expired cells.
This replacement uses screws to mount the two halves, which makes the upcoming (?) replacement of cells easier. That said, the
availability of NiCd cells is probably ending at some time in the near future. NiMh cells could be a replacement,
but require a different charging technique, and hence a different charger.
Using USB power-packs to supply E-Serie and S10 instruments may work. The voltage level is 4.8V to 5V in both cases. Care must be taken not to reverse polarity. It would be unwise to assume built-in protection circuits. No experience on my side with this, so I can't advise on it.
The Elta 10, 20 and Trimble 5603 with Elta CU use PCMCIA storage cards. New PCMCIA cards became somewhat rare around the year 2010.
For the PCMCIA slot (aka "PC card"), a CF-card-to-PCMCIA adapter is an alternative. New storage cards in Compact Flash format (CF cards) are still available today (2018), while new PCMCIA memory cards (SRAM) are exotic (yet still used in some automation systems), rare and expensive.
However, a CF-card with a PCMCIA adapter works only on an S10/S20 with "PC-Version 2". Although both "PC-Versions" list Zeiss "SW version 1.43" , the older "PC-Version 1" hardware does not work with adapted CF cards and seems to accept PCMCIA SRAM cards only. Booting an older model with a CF-card was found to stall sometimes, while an original 1MB SRAM card worked. As a rough indicator, the update to hardware "PC-Version 2" may have happened around serial number 110000. Apart from the issue with the PCMCIA adapters, the older "PC-Version 1" hardware is in fact terribly slow, likely due to the slow 86286 CPU. Patience is required when operating an S10 with "PC-Version 1".
As said, PCMCIA/PC-card SRAM cards (e.g. 1MB) behave differently and can be difficult to read/write on Linux, even if you happen to own an
older laptop with a PCMCIA/PC-card slot. Industrial USB-to-PCcard converters do exist, e.g. by
CSM, since
some legacy industrial controls still rely on PC-cards. However, they are expensive.
Serial communication is an alternative way to upload/download data to/form an S10/S20 instrument with "PC-Version 1" hardware.
Good news: The CF-to-PCMCIA adapter does work on the newer Trimble 5603 as well.
| PC version 1 | PC version 2 |
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Formatting of CF-cards on Linux for acceptance by the MS-DOS in the S20 needs fiddling of parameters for "mkfs". These were found to work with
version 3.0.13 of mkfs.vfat, for an S20 with a "PC-Version 2" board:
mkfs.vfat -n tachy3 -F 16 -h 32 -s 16 -R 1 /dev/first_partition_on_cfcard
The "-h 32 -s 16" parameters are the critical ones.
Following the tape-puncher of the Elta 14 and prior to affordable laptops, Zeiss offered exchangeable memory moduls for data storage in the field. A second way for storage were external storage units that interfaced with the tachymeters through RS232:
The main reason for an in-the-field automated data storage is to avoid errors when communicating and writing down numbers manually. Faster speed is a benefit as well. Hence, once electronic reading of angular and distance values became technically feasible, their automatic storage was the next logical thing and constituted a big push forward in practical surveying.
The first in-the-field storage system of the then Elta-14 consisted of a 'portable', battery powered, 5bit tape puncher. The storage technology of the outgoing 1960-ties, used extensively in teletypers of the period.
These memory modules followed and offered an intermediate, optionally per-project, data storage between the tachymeter in the field and the computer at the office, without the need to carry the bulky computer equipment of the time (or a tape-puncher) into the field. They were sort of the "memory card" of the period. Later the REC500 offered a compact "tablet-like" solution with an enhanced user interface, and the need for these memory models declined. Note that the later E-Serie generation (see images above) doesn't have this memory slot.
According to a publication of Zeiss Canada from 1981, there had been a MEM100 module as well, supposedly a predecessor or low-capacity variant of the MEM200. The text states the capacity as "200 and 400 data-sets", and life of the buffer battery as "1 week" between charging.
The Zeiss MEM200 was a pluggable memory module for the second-generation Elta2. It features 12x TC5504P-1 Toshiba CMOS static RAM, 4kx1 bit each (roughly made around 1981) and an internal backup battery. Also included are 2 EPROMS and a Harris M3-6100-9 CPU, which, according to the web, runs 12bit @ 4MHz. On-board quartz is 2MHz. Plus some DIL ICs. Interestingly, on this MEM200, one TC5504P-1 had been replaced during its active time of duty. The 14-pin "Centronics"-style connector (similar to IEEE 1284) has the 2 rows connected in parallel, hence 7 lines for signal and power. Likely a multiplexed data-transfer. - ?
The Zeiss MEM800 was a pluggable memory module and supposedly the successor of the MEM200. It features unlabelled RAM chips on an extra PCB, and an internal backup battery, likely the same Varta 4-60DK @4.8V as the MEM200. One EPROM, an Texas-Instruments TMS70C00BNA CPU, plus 4 SMD latches, drivers and bus multiplexers. The TMS7000 had been an 8bit architecture released in 1981, featuring optional microcode customisations stored in CPU ROM. The I/O connector of a MEM800 is the same as on a MEM200.
| MEM200 | MEM200 internals | MEM800 | MEM800 internals |
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The Zeiss DAC100 was, according to a Zeiss publication of 1978, the first data conversion unit to read MEM memory modules, primarily intended to be used at the office. It interfaced to computers or printers via a RS232 serial connection. According to a picture in that Zeiss publication, it looked like an early desktop calculator, there's no actual unit in this collection (yet?).
The Zeiss REC200 was a follow-on data conversion unit to transfer from/to MEM modules. and charge their internal back-up battery. It can either log data from Zeiss tachymeters via RS232 in the field, or transfer the data to computers at the office. Powered by battery type Zeiss 70811 or a 12V DC input. The 70811 battery type fits in the Zeiss LG6 charger. Display consisted of a 16 character, single line LCD, with user input via 9 function-buttons and a numeric keypad. Getting it to work is somewhat cryptic without consulting the manual. The RS232 interface uses the same DIN 41524 connector as on the tachymeters (see above for a pin list).
According to a publication of Zeiss Canada from 1981, the Zeiss REC100 was similar to the REC200, but without the LCD display.
The Zeiss REC500 was a newer, portable, ruggedised hand-held computer, used for data storage and management with Elta models
that did not have on-board data storage, but an RS232 serial port. Effectively it replaced the storage function of the older MEM modules
with a much nicer and more powerful storage and user-interface.
Two hardware were used: The older model "Husky 352KEL", model 114K or newer "Husky Hunter", model H-2922, both manufactured by "Husky
Computers Ltd" in Coventry, UK.
The newer features a graphics-capable LCD display, QWERTY keyboard, one 25-pin sub-d RS232 port and a 4pin Lemo
socket for power supply and charging.
According to its manual of 1986, it runs CP/M on a Z80 CPU and a BASIC interpreter,
Other internal parameters (CPU,RAM,NVRAM,etc) not (yet) known to author. The manual mentions an additional internal NiCd battery and
seal dimensions of 1.5mm x 30mm for the AA battery compartment.
Wikipedia article on Husky computers
| REC200 | REC500 | |
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| earlier version | later version | |
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| Tachytop (Bussole) | Th 3 | Th 2 | Th 42 | Th 42 + Eldi2 | Rta 4 | |
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| coordinate display | coming soon | 
| coming soon |  111.17 GON vertical, 136.645 GON horizontal | 
|  (image quality and field-of-view limited by camera.) Reads 98.815 GON vertical, 326.735 GON horizontal precise for a layman's eye to 0.002GON, about 6″ |
| manufacturer | Zeiss (Jena) | Zeiss-Opton (Oberkochen) | Zeiss (Oberkochen) | Zeiss (Oberkochen) | ||
| approximate year of production | ca 1930-1950 ? | ca 1953-1969 | ca 1960-1970 | ca 1960 | ca 1960 ? | ca 1960-? |
| nominal angular precision | 0.1g | 1' (0.1' with micrometer) | <1" | ? | ? | 3″ |
| angular compensator | - | - | one axis | one axis | one axis | one axis |
| angular reading [GON] | 1.0g | 0.1g 0.01g micrometer | 0.0001g (0.3") | 0.01g | 0.01g | 0.01g |
| angular estimate [GON] | 0.1g | 0.01g 0.001g micrometer | - | 0.001g | 0.001g | 0.001g |
| distance precision | - | - | - | - | Eldi2 ± 5mm, ± 20mm | 5-20cm / 100m (500ppm) |
| telescope magnification | 12x | 25x Apochromat, coated, inverted image | 30x | 25x ? | 25x ? | 25x Apochromat, coated |
In order to show the vertical and horizontal scales in one display, the theodolites used an impressively complex optical path within the
instrument. Sub-second theodolites like the "Th 2" also have a rather fascinating ''vernier scale'' method for adjusting and reading
sub-second angles.
One way of distance measurement is to use the view-angle that a distant vertical rod subtends in the view finder of the theodolite. This is
easy, but is limited to a ''few dozen meters'', beyond that it becomes increasingly difficult to read the rod markings and the required rod length
becomes too large. For non-horizontal view directions (''down-hill'' or ''up-hill'') correctional factors have to be applied.
The principle is mostly used for construction work in domestic-house-size building projects.
Some theodolites (e.g. the Zeiss Rta4) do have a very clever mechanical automatic adjustment to measure horizontal distances even when
viewing the vertical rod up-hill or down-hill (the so called ''reduction'' of distances).
A "bussole" theodolite is effectively a precision compass plus an additional vertical angle reading. It is used if no second point is in sight as horizontal reference. Azimuth readings are comparatively coarse and relative to Magnetic North. The angular offset to "True North", the Magnetic Declination, depends on the location on the Earth and is not constant over years. All magnetic materials (e.g. steel) must be kept well clear of the bussole while taking readings. A Gyrocompass is an alternative that orients itself to "True North" automatically.
Parameters of Eldi 2:
910nm, 15MHz/150kHz (two ranges, 700m, 1000m), 6-9V DC, 5W
Nominal error: ± 5mm @ 700m range (7ppm), ± 20mm @ 1000m range (20ppm)
Due to the modulation frequencies, the measured and displayed distance is correct up to 1000m, for longer distances there's a manual correctional
procedure.
Source: Zeiss manual G70-165-d, 1977
| Hersteller | Zeiss West | Zeiss Jena | Nestle | ||
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| Ni 2 | Koni 007 | Ni 007 | Nan 2024 | ||
| Bilder |
 
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| Fernrohr Vergrößerung | 31x | ||||
| Pendel-Kompensator | ja, mit Wirbelstrom-Bremse | ||||
| Fernrohrbild | aufrecht | ||||
| Instrumenten Präzision | 0.5mm/km | 0.8mm/km 0.5mm/km nach Tests von Zeiss Oberkochen (!) | 3mm/km | ||
| Extras | Nonius (20′) am horizontalen Teilkreis | Planplatten Mikrometer | |||
| Markt Einführung | 1959 | ||||
| AGA Model 6A | HP 3800B | |
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| instrument precision | ? | 5mm + 7mm/km |
| instrument range | ? | max 3km (triple prism) |
| readings | potentiometer | numerical decade knobs |
| approximate year of production | 1950-1960 ? | 1965-1974 ? |
Correction for air pressure and temperature is done externally. The HP3800B offers an external potentiometer located at the battery
pack to set a correction factor for both. Parameters from HP's "3800B/3801B Operating Manual", Part No 03800-90004, printed ca 1972.
Both are non-coaxial instruments, the telescope and the range finder are not at the same vertical position. Therefore, HP offered a prism
with a vertical post and instructions to aim the telescope above the prism.
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| instrument precision | reading approx 3 mGON |
| telescope magnification | 12x (inverted image) |
| distance factor | 100 |
| approximate year of production | 1950 - 1970 |
This type of compass theodolite was built by Ertel in Puchheim, Bavaria. Its telescope image is inverted with horizontal
stadia lines, optionally with a right angle prism at the ocular. According to a very helpful guy who had worked at Ertel, two variants had
been manufactured: A grey painted standard model, and an identical, but dark-green painted one for the military. Some serial number start
with the prefix "FB" for "Forst-Bussole", ("forestry theodolite"), although this prefix is found in the serial number for some dark-green models
as well. On some models, the horizontal scale can be shifted ±15GON relative to the telescope axis, to allow setting of the local
value of the
magnetic declination, thus giving horizontal readings relative to
True North directly.
Due to the inverted telescope image, the instrument is best used with levelling rods that have the numbers at the stadia lines printed
up-side-down.
Apart from a serial number, there's no model name or type mentioned on the instruments.
These particular examples had been used extensively in forest management and building of forest infrastructure in Northern Germany,
and in training classes.
The swiveling interface to the head of the accompanying special, non-ferrous, tripod allows levelling the theodolite. The non-ferrous material ensures low or zero magnetic deviation. Notable is the non-standard screw between tripod and theodolite, featuring a metric fine-pitch M15x1.5 thread. The screw and the non-flat head of the tripod make these Ertel tripods incompatible with other theodolites.
Note: The GON values on the horizontal circle increase anti-clockwise, with the East "E" label printed to the "left" of North. This may be counter-intuitive at a first glance, since compasses scales show angular values increasing clockwise, and West to the "left" of North. However, both work correctly, and read the correct value. For example, 90°, 100GON, when pointed to the Magnetic East. Two positions of the telescope are possible, see below.
| left-hand position | right-hand position | |
|---|---|---|
| sighting centred on church lighting rod |
|
|
| top view |
|
|
| detail of North end of needle |
|
|
| horizontal reading North end of needle | 328.5 GON | 128.5 GON |
Most theodolites and tachymeters allow to focus on the distant target using either of two positions of the telescope. The main advantage is to intrinsically cross-check the instrument and get an estimate on its errors. Secondly, it can identify errors in manual reading or alignment. With manual reading, the advantage of the GON angular units becomes obvious: The difference between the two readings is 200GON, which is easier math than adding/subtracting a value of 180deg. Motorised tachymeters offer automatic measurements with both telescope positions and cross-check these automatically with pre-defined error-bounds.
The above example of an Ertel theodolite is slightly unusual, as the axis of its telescope is not centred above its vertical axis, but has an 8 cm offset. The parallax error caused by this in above example, with a target distance of roughly 360m, is atan(0.08m/360m) = 14 mGON , which is about a factor of 20 smaller than the estimated precision (300 mGON) of the visual reading of its scale. Hence the parallax error could be neglected anyway in this case. However, for objects closer, the average of the two telescope positions must be used to compensate for the parallax error.
For theodolites with the usual centred-mounted telescope, a remaining 'gap' between the telescope axis and vertical axis constitutes an instrument error which can be cross-checked by measurements in both telescope positions.
In general, with instruments where the full angular circle is readable, it is advised to read the angular value at opposite positions. In the case of the Ertel bussole, this means reading both the North and South end of the needle, to increase precision and cross-check for out-of-centre errors.
The use of modern metal theodolites for surveying and constructions goes back well over 100 years. A brilliant example was the surveying
that led to the successful cut of the first Gotthard Tunnel in 1881, when the
two tunnelling crews met quite nicely spot-on inside the mountain.
Instrument precision went up over the decades, size and weight went down, and the handling was greatly eased for the surveyor (e.g.
electronic reading the scales).
A major revolution came with electronic distance measurement (EDM), which is the only way to measure distances over 100m fast and
accurately. Measuring survey distances by timing electromagnetic waves became available in the field around 195x. First by microwave, then
in the infra-red spectrum. After the first infra-red and combined instruments (like the "Elta 14"), the route was set to develop faster and
more compact instruments, leading to the indoor and outdoor 3D scanners of today (2010+, "LIDAR").
Another milestone was the introduction of prism-less tachymeters around 2000, which work with the reflected light off most surfaces. First
tachymeters needed a retro-reflecting prism at any distance, todays instruments
require a prism only for very large distances. The reflected signal off a normal dark grey surface in, say 100m, distance, is extremely weak,
and it is a respectable feat of electronics that today's instruments work with whatever low signal they get. For distances in the order of a
kilometre and more, prisms are still useful. If not for signal strength, they define the measured point exactly.
They are also used in "stake-out" work, when 3D coordinates are mapped to a 3D-point in the field.
The reading of angular values went electronic too, with the advent of electronic tachymeters. That alone greatly simplifies the surveying
process: Manual tables and logs were replaced by electronic storage of measured coordinates. The two positions of a theodolite, used at all
times to cross-check alignment errors of the instrument, can now be handled electronically and hence done automatically.
The units of GON and DEGREE are selectable in one instrument by software, before that, an instrument had either a hardware scale in GON or
DEGREE. Furthermore, electronic processing of angles and distance allows a direct conversion to Cartesian XYZ coordinates in the field and
XYZ coordinates of points can be directly exchanged with 3D CAD systems.
However, the ease of using a modern tachymeter still depends, like with their mechanical predecessor, on the skill of its manufacturer and
matching the preferences in handling by the surveyor. There are excellent graphical-user-interfaces (GUI) and there are bad examples.
Another point is the readability of the display in bright light:
While the LCD of an 1990 "Elta-3" looks a bit dated at first, it is perfectly readable under
any light condition, while a newer (non-Zeiss) tachymeter with a 5" touch-screen using the Windows operating system, made around 2005, is
in fact unreadable outdoors.
Sadly, Zeiss in Oberkochen apparently decided to bail out around the time when the first non-prism tachymeters became available. - Although
their "Rec Elta-RL" was prism-less, the newer "S20" was not - a bit weird. They first merged with Zeiss Jena after German
unification, then, apparently, concentrated the surveying work at Jena and after a few years sold their whole survey product line to
Trimble.
Nevertheless, their instruments still work impeccable for actual surveying work, - what you should expect from a product with a "Zeiss" logo.
And, after all, a prism is both nice and required to define a point during "stake-out work" (transferring 3D points from CAD-model to landscape).
In any case, the distance measurements is primarily one of time. To convert to distance with usable precision, the speed-of-light in the atmosphere must be known with sufficient precision. And that depends on atmospheric pressure and humidity along the optical path. In most geodetic applications it is deemed safe to assume that atmospheric conditions at the point of the instrument are the same as along along the optical path. Hence atmospheric parameters must be recorded by the surveyor or the instrument, and then corrected for. This was done semi-manually with first-generation instruments and fully automatically with the newer ones (e.g. S20).
The speed of light is roughly 33cm (330mm) per nano-second (ns, 10-9 second).
Hence, to resolve 1mm with time-of-flight measurement, the electronics need a time resolution of 1/330 = 0.003ns, or 3 pico-seconds (ps, 10-12
second).
A sinus signal with 1 pico-second (ps, 10-12 second) period has a
frequency of 1000GHz (109 Hertz), so electronics
have to handle signals well in the high GHz range. And they must be stable, compact and reasonably priced.
Which easily explains that practical use of this technology required the invention and mass-production of
transistors and smaller
integrated circuits.
Technically there are two ways to get the timing: Either by directly measuring the time between sending a pulse and the returning echo
(time-of-flight, TOF). Or by modulating the emitted light with a few hundred MHz and measuring the phase shift between emitted and returned
signal. This requires a set of different modulation frequencies in order to get a non-ambiguous solution.
With the second method, measurements take longer, but electronics are supposedly easier.
In surveying, Satellite navigation ("SatNav") has replaced tachymeters for most
routine work. From a Physics point-of-view, SatNav is based on exactly the same principle of measuring time-of-flight: SatNav times
microwave signals and hence distance between the point on Earth and a collection of satellites about 20.000 to 25000km away.
SatNav can be precise down to 1cm, which is pretty good compared to the distance of 20000km. But it does require correctional real-time
information about the atmosphere to achieve this.
Hence, for surveying, it typically needs an usable SatNav signal from multiple satellites and a mobile phone connection. These are
not always available: The SatNav signal is impaired by high rise buildings in cities, foliage inside a forest or underground (mining,
tunnelling), while rural areas may not have mobile phone coverage. Which is why traditional tachymeters are still in use and relied upon.
| unit | symbol | units/revolution | unit for small angles | example |
|---|---|---|---|---|
| GON | g | 400 | mGON (1/1000 GON) | 50.1371g |
| DEG | ° | 360 | arcsec (1/3600°) | 45.1234° (decimal) or 45°07′24.24″ (DMS) |
| RAD | 2 π | mRAD (1/1000 RAD) | 0.78755rad |
Angles in DEG can either be given as decimal or as
degrees-minutes-seconds (DMS): A decimal value of 45.1234deg is roughly the same as 45°07′24″ .
NB: The German term "Grad" is the same as the English "degrees". GON is called "Grad", "Grade" or "gradian" in English. Hence most pocket
calculators allow a selection of "DEG,GRAD,RAD" for angular units.
The popularity of "GON" amongst surveyors is fraternised with rather quickly in the field when comparing readings of mechanical theodolites
in the two telescope positions: Adding or subtracting a value of "200" from the azimuth readings is quicker than dealing with "180". But
with the advance of electronic processing and data transfer, the choice of units became less relevant in practice. A second advantage is
that fractional GON values are always given in decimal notation, whereas fractional degrees can be given in decimal or in minutes/seconds,
leading to potential confusion. Outside surveying, the use of GON seems to have remained very rare.
One arc-second is also something of a watershed for the precision of an instrument: Theodolites used in average construction work have a
nominal precision of 3″-5″, while first-order country-wide surveying calls for ''sub-second'' precision.
Theodolites for astronomical observations and first-order surveying (e.g. Wild T4) have a precision of 0.1″ .
In comparison, a nautical hand-held sextant has a typical precision of a
few arc-minutes.
1 arc second (1″) corresponds to 4.8mm at 1km distance. Or while, we're at it, to 1.9km at 400000km, the approximate earth-lunar distance.
| deg | 1/1000 deg | arc-minute | arc-second | mrad | gon | mgon | object size at 1m | at 1km | ||
|---|---|---|---|---|---|---|---|---|---|---|
| 1 deg | = | 1° | 1000 | 60′ | 3600″ | 17.45 | 1.11g | 1111 | 17.45 mm | 1.7 m |
| 1/1000 deg | 0.001° | 1 | 0.06′ | 3.6″ | 0.017 | 0.0011g | 1.1 | 17.45 μm | 17 mm | |
| 1 arc-minute | 0.0167° | 16.67 | 1′ | 60″ | 0.29 | 0.0185g | 18.52 | 0.29 mm | 29 cm | |
| 1 arc-second | 0.00028° | 0.278 | 0.0167′ | 1″ | 0.0048 | 0.0003g | 0.3 | 4.8 μm | 4.8 mm | |
| 1 mrad | 0.057° | 57.3 | 3.44′ | 206″ | 1 | 0.0637g | 63.66 | 1 mm | 1 m | |
| 1 gon | 0.9° | 0.0009 | 54′ | 3240″ | 15.71 | 1g | 1000 | 15.7 mm | 1.6 m | |
| 1 mgon | 900° | 0.9 | 0.054′ | 3.24″ | 0.0157 | 0.001g | 1 | 15.7 μm | 15.7 mm |
|
Angular units of [mGON] versus [arc seconds] : 
|
Angular units of [mrad] versus [arc minutes] : 
|
Angular units of [urad] versus [arc seconds] : 
|
As with any measurement, the nominal precision of the instrument does not solely warrant the "trueness" of a measurement. Systematic internal errors may have been picked up since last calibration. Handling errors can be of simple nature:
Ways to reduce errors:
Cross-checking of results is highly advisable in any engineering or scientific work. Knowing the concept of Accuracy and Precision is considered most helpful.
For example, the nominal angular and distance errors of an Elta S20 are, according to the Zeiss manual:
Tripods used in surveying use larger screws than
photographic tripods. The larger screws allow a central bore for an
optical sight downwards ("optical plummet"). One standard screw type is commonly used, except for some exotic legacy theodolites
(see Ertel example in "other brands") and quick-lock systems.
Like photographic tripods, this screw type is "Unified Coarse" (UNC).
And as usual with UNC, their specification consists of the outer diameter in fractional Inch
and the threads-per-inch.
For example, 1/4-20 specifies a diameter of 1/4" (6.35mm) and 20 threads-per-inch (1.27mm pitch).
By the way - UNC 1/4-20 is thus slightly incompatible with metric M6 (diameter 6mm, pitch 1mm).
| thread type | outer diameter | pitch | drill size | tripod type |
|---|---|---|---|---|
| UNC 1/4-20 | 6.4 | 1.3 | 5.1 - 5.4 | consumer camera |
| UNC 3/8-16 | 9.5 | 1.6 | 8.0 - 8.3 | pro camera |
| UNC 5/8-11 | 15.9 | 2.3 | 13.5 - 14.0 | surveying equipment |
Worth to note: Unified Coarse (UNC) is not compatible with (British BSW) Whitworth thread, nor British Standard Pipe (BSP). Hence UNC 3/8 doesn't fit G3/8. A bit confusing, since all three systems use an "imperial" label based on fractions of an Inch. However, they differ in diameter, pitch and thread angle (UNC 60°, Whitworth, BSP 55°). ... Welcome the newer and systematic metric system.
Early (pre WW-II) theodolites had been screwed onto a tripod directly. Newer system use a
tribrach as an interface between instrument and tripod:
Quick-lock system between tribrach and tripod offer faster mounting and a reproducible position, both in height
and, with the Kern and Wild types, orientation: Note the two pins on the Kern flange and the gap in the Wild flange, both enforcing a
specific orientation of the instrument on the flange. Compared to this, Zeiss featured a cylindrical "Zeiss bolt" as mechanical interface
between tribrach and instrument, which had no reproducible orientation around the vertical axis .
Most quick-lock systems offer to swap the theodolite with a target. The reference point of the theodolite is then at the same position as
the centre of the target (prism or mark).
| Wild | Zeiss | Kern |
|---|---|---|
|
|
|
The Kern type was an unusual combination of tribrach and tripod. The Wild and Zeiss type use a standard UNC-5/8 screw between tribrach and tripod,
thereby allowing to mount it on any surveying tripod or flange.
The Kern had a unique positioning method: It used a vertical extensible rod to centre the tripod over the reference point while adjusting
the rod vertically over the point. This mechanical alignment has benefits and drawbacks over optical methods: With both the alignment over a
reference point is a two step procedure: Levelling the tripod and shifting it horizontally. The Kern method seems slightly faster and works
if the reference point can only be manually felt, but not seen, e.g. a reference dip in muddy water.
The Wild quick-lock is still used widely today (2024), it seems to be the de-facto standard. With reproducible orientation, it offered
advantages over the Zeiss mount, while its locking mechanism is mechanically more complex.
Although data was compiled with care and cross-checked where possible, all data and parameters are supplied "as-is" without any
warranty.
We're not responsible for the contents of other websites, even if we link to them.
Disclaimer: We're not responsible for the contents of external sites, whose contents may change after we checked and linked to them.
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Autor: Peter Apian-Bennewitz,
Stand vom: 10.1.2022 meine anderen technischen Notizen , home page |
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