How to measure Baseline
In surveying procedures such as traversing, triangulation, trilateration, and setting out, baseline measurement is critical. Prior to the invention of the Electromagnetic Distance Measuring Instrument, baseline measurements were made with equipment such as tapes, chains, and bands (EDM).
The method of measuring baseline with early instruments has largely been replaced by distance measurements using electromagnetic means. So, basically there are two methods to measure the base line.
1)Conventional method
i) Wheeler’s method ii) Jadrein’s method
2)Electronic Distance Measurement
1). Conventional Method:
Theodolite
To use these methods, first field work is executed by two groups of surveyors. One is called setting out group consists of two surveyors and several porters, is responsible for aligning the measuring tripods prior to the measurement and at the proper intervals and the second group is called the measuring party, consisting of two observers, leveler, recorder and staff man, for actual measurements.
The obstructions are removed from the base line, which is then split into reasonable segments of up to one kilometer in length and is accurately aligned using theodolite.
Stout posts or marking stakes are driven firmly into the ground whenever the alignment changes. The setting out party then aligns the measuring tripods in preparation for the measurement, which can be accomplished in two ways:
i) Wheeler’s Method:
In this method the marking stakes are driven into the ground at regular intervals (less than the length of one tape) on the base line in such a way that their tops are 50 cm above the ground.
ii) Jaderin’s Method:
In this method, instead of straining poles, trestles (straining tripods) are used and measuring tripods are used in place of marking stakes.
Corrections:
Jaderin introduced some corrections for more accurate measurements. These are as follow:
Corrections in Taping:
i)Correction for Absolute Length
Absolute length = Nominal Length ± Ca
Ca = L (l’ – l)/L
where:
L = Measured or Recorded Length
l = Nominal Length of a tape
l’ = Actual Length of a tape
Ca = Correction for Absolute Length
The sign of the correction is determined by l and l’ values. However, because l’ is typically more than l, this adjustment is usually positive, indicating that when a tape is stretched and is too long, it reads too short.
ii)Correction for Temperature
Ct = α(Tm-To)L
Where:
α = Coefficient of Thermal Expansion
Tm = Mean Temperature during Measurement
To = Temperature of calibration Measured Length
iii)Correction for Pull/Tension
Cp = (P – Po)L/AE
Where
P = Pull applied during
Po = Pull under which the tape was calibrated
L = Measured Length
A = Cross sectional Area of the tape
E = Modulus of Elasticity of Tape Material
iv)Correction for Sag:
Cs = w2 L3 cos2φ/(24P²)
where
P = Pull applied during measurement
φ = Angle of slope between tape supports
w = Weight of tape per unit length
W = Total Weight of Tape
v)Correction for Slope
C = L (1 – cosφ )
OR
C = L – √(L² – h²)
C = h²/(2 L)
All these corrections are applied to the measured length in order to get accurate results.
2). Electronic Distance Measurement
EDM total station
Only in the early 1950s the first electronic distance measuring equipment were developed. These primarily consisted of Electro-optical and electromagnetic instruments. They were bulky heavy and expensive. The typical EDM today uses the Electro-optical principle. They are small reasonably lightweight highly accurate but still expensive.
The use of EDM technology removes the requirement for extensive baseline preparation. The use of EDM greatly simplifies the baseline measurement process. Since 1950, baseline measurement using invar wires has been replaced by a far more convenient form of measurement, namely the use of Electro Magnetic Distance Measurement (EDM).
EDM reduces the requirement for time-consuming baseline preparations. The length of the baseline has no bearing on the time it takes to take the requisite instrument reading during the actual measuring procedure.