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STAR*NET V6 - Circe

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Appendix C Additional Technical Information<br />

Since slope distances and zenith angles are both “sloped” observations, their total<br />

standard errors are each inflated by both horizontal and vertical centering errors.<br />

In the following formulas:<br />

d = Horizontal distance from instrument to target<br />

s = Slope distance from instrument to target<br />

e = Elevation difference from instrument to target<br />

Slope Distances: The total standard error is equal to:<br />

Total Dist StdErr = Sqrt( DistStdErr 2 + (d/s) 2 * (I 2 + T 2 ) + 2*(e/s) 2 * V 2 )<br />

Zenith Angles: The total standard error is equal to:<br />

Notes:<br />

Total Zenith StdErr = Sqrt( ZenithStdErr 2 + (e/s) 2 * (I 2 + T 2 ) + 2*(d/s) 2 * V 2 )<br />

1. The calculations for angle and direction centering error in the formulas shown on<br />

this page and the previous page are carried out in radians.<br />

2. In any formula shown above for a linear observation (slope distance, horizontal<br />

distance or delta elevation), the resulting “total” standard error is calculated from the<br />

entered standard error of the observation plus any given centering errors. It should be<br />

noted that the “entered standard error” for any linear observation is made up of a<br />

constant part and PPM.. See the discussion of the PPM (Parts per Million) settings<br />

starting on page 23 of Chapter 4, “Options.”<br />

3. When standard errors are explicitly entered on an observation data line, these values<br />

are by default used as the “total” standard error value that will be used during the<br />

network adjustment. They will not be inflated by centering error.<br />

If there are situations where you would like explicitly entered standard errors to be<br />

inflated by entered centering errors, you can use the “.ADDCENTERING” inline<br />

option as described on page 91 in Chapter 5, “Preparing Data.”<br />

4. Centering errors are not applied to differentially leveled elevation differences.<br />

194

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