Station 1 · A → B
+0.550m
Δh = w − p = 1.425 − 0.875
Geometric levelling · teaching model
The difference between two staff readings carries height from one benchmark to the next. Three stations lead from A through B and C back to A — and there the calculation should return the height it started from. Change a reading and see how far the loop opens.
starting benchmark — height given in the exercise
+0.550m
Δh = w − p = 1.425 − 0.875
matches the reference
−0.530m
Δh = w − p = 1.120 − 1.650
matches the reference
−0.020m
Δh = w − p = 0.950 − 0.970
the same benchmark A, height from the calculation after three stations
Return to A · gap fh
0mm
A′ = A: the calculation returned to the height of benchmark A.
Previous result: none — nothing has been changed yet.
Δh1+0.550m
Δh2−0.530m
Δh3−0.020m
Σ0.000m
Σw − Σp = 3.495 − 3.495 m
In a reading field the ↑ ↓ arrows change the value by 1 mm and the −5 and +5 buttons by 5 mm. Staff range in the exercise: 0.100–3.500 m. An empty reading is not zero — the calculation then pauses.
Exercise reference: we assume that B = H₀ + 0.550 m and C = H₀ + 0.020 m are true, so that you can see which point the measurement has shifted. In the field you do not know the truth — you have only the readings and the balance. The length of the gap on the left edge is schematic and linear up to 100 mm: a gap of 100 mm or more takes up 80% of the side length (the rest is shared between the two short segments of the mark).
Closure 0 mm — the calculation agrees.
The sum of the backsights equals the sum of the foresights, and points B and C agree with the exercise reference. This is agreement of the balance, not proof of a flawless measurement: mistakes of opposite signs also give zero (the “Errors cancel out” case).
One station
The level stands between the points and defines a horizontal line of sight. The backsight reading w measures the distance from the starting point to that line, the foresight reading p from the end point. The difference w − p is the height difference: a positive value means that the foresight point lies higher [2]. The height of the sight line drops out of the result: raise it by 100 mm and both readings grow by the same amount (the “Different sight-line height” scenario).
Limits of closure
The loop returns to A and says only how large the sum of the mistakes is. It does not say at which station they arose, and it does not rule out mistakes of opposite signs. That is why checks independent of the balance are added in the field, for example a second reading on the second graduation of the staff or a measurement in the opposite direction [2] [3]. Five cases from the exercise, calculated for T = 5 mm and any H₀:
The calculation matches the reference. Still only a balance.
Different readings, same difference. A different reading on the staff is not an error in itself.
Within the exercise threshold, but the loop does not show that station 3 is to blame.
Above the threshold. The balance says “somewhere”, the exercise reference shows “from C upwards”.
A perfect closure, yet point B is 10 cm lower. This very case is the reason not to read zero as proof.
LEVELLING LOG · TEACHING MODEL · loop A → B → C → A H(A) = 100.000 m · exercise threshold T = 5 mm stn 1 A→B w = 1.425 m p = 0.875 m Δh = +0.550 m H(B) = 100.550 m stn 2 B→C w = 1.120 m p = 1.650 m Δh = −0.530 m H(C) = 100.020 m stn 3 C→A w = 0.950 m p = 0.970 m Δh = −0.020 m H(A′) = 100.000 m Σw = 3.495 m · Σp = 3.495 m · f_h = Σw − Σp = 0 mm Invented data; conventional layout; this is not a measurement or surveying instructions.
Scope and uncertainties
Sources