Full text: XIXth congress (Part B5,1)

Bas, Hüseyin Gazi 
  
  
8.94x10-6 |9.02x10-6 | 1.79x10-6 | 2.19x10^5 
  
10 | 15 6 6 
1.37x105 |1,42x10-5 [| 2.73x 105 [3:37x 105 
  
15 | 25 10| 10 
2.35x105 \2.70x10-5 |4.70x10-5 |5.91x10-5 
  
20 | 35 14] 14 
3.44x105 |4.66x10-5 |6.88x10-5 | 8.99x10-5 
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
30 12] 12 
30 3.36x105 |4.14x10516.72x105 |8.57x105 
25] 10] 10 
40 3.39x10-5 |3.68x10-5 | 6.79x10-5 | 8.43x10-5 
40 | 16| 16 
50 7.11x105 19.99x10-5 | 1.42x10-* 11.88x104 
20 8 8 
60 5.14x10° 14. 20x10" 1.03x10* |1,22x10* 
30 | 12 
70 12 11.29x10* l'1.17x10*|2.59x10" |3.13x10° 
23 |. 10 
85 10 ]4.08x10^ [2.34x10418.15x104^ [9.41x10^4 
© 
The results of the calculations have been shown that while the increase in mx, my and mz is In cl 
very slow for the different values of a and p between 0-45 degrees, this increase is fast for the coorc 
values between 45-90 degrees (see Table 2). If it is taken into account that the change in the the t 
object distance from point to point is negligible in close range measurement, for the same system, objec 
the errors in the object space coordinates depend on angles a and ß. Base-Object distance ratio appr« 
is an important criterion in terrestrial photogrammetry and the convergent case is preferred to the can t 
normal case of photogrammetry to increase the base length in the analytical method. Because the of ho 
horizontal angle will increase with a longer base length and a shorter object distance, an optimal certo: 
base-object distance ratio should be considered (for example B/Z-2/1) in close range 
measurements with theodolite. 
REFE 
Abdel 
Photo 
Bas, | 
Theoc 
Brown 
i i Digits 
Table 2. Object Space Coordinates Errors for the same system (Z=6.0 meter, 
constant) Ghosl 
a Z mx my mz Grist, 
Photo 
0 6 1.37 2.67 
1.33x105.. x105 x105 
  
  
  
  
  
  
  
  
50 International Archives of Photogrammetry and Remote Sensing. Vol. XXXIII, Part B5. Amsterdam 2000. 
 
	        
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