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Table Of Contents
Introduction
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Applications of deformation surveys include:
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Dam walls - earth and concrete
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Bridges
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Buildings
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Earth movements, for example continental drift, or subsidence
as a result of mining
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There can be considerable cost (human and $) for
failing to detect deformations, and/or interpret them accordingly.
Failure of the Teton dam in Idaho, 1977, killed 11, left 2500 homeless
and resulted in $400 million in claims.
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Besides the monitoring of engineering type structures
other deformations to be aware of include (Krakivsky, 1986):
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Tidal effects - the earth's crust can deform
by as much as 0.5m, although this happens uniformly over a large
area.
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Crustal loading - caused by natural phenomena
such as glacial advance and retreat, siltation in river basins,
or with human intervention the draining/filling of lakes.
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Plate tectonics - tectonic plate drift is of
the order of a few cm per annum, although violent earthquakes
can cause deformation of metres
- Ground consolidation - especially due to the extraction of
oil/gas or artesian water
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Measurements
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High precision networks use survey equipment such
as first order theodolites, precise levelling, Mekometer EDM and
GPS translocation in order to detect the movement of survey stations
or targets. Photogrammetry can be an effective tool for deformation
monitoring depending on the scale of the object being measured.
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Besides convention survey measurements other geotechnical measurements
can be made (Chrzanowski, 1986):
Instruments including extensometers, strainmeters,
laser rangers, and tiltmeters are used. These intruments are extremely
sensitive. Ideally all observations strutural/geotechnical/survey
should be incorporated into the one adjustment model.
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The gravity field may be considered in precise
engineering surveys (integrated geodesy/least squares collocation).
This is particularly important in large structural projects where
newly introduced loads significantly distort the gravity field locally.
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GPS is useful especially for long connections to
stable ground. It has been successfully used in deformation monitoring
of structures such as dams.
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GPS also does not require a clear line of sight
- In some cases, eg a steep dam wall, GPS may be unsuitable due to
poor satellite visibility/geometry, and multi-pathing.
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Processing
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The adjustment of such survey networks require
all the considerations with respect to elimination of errors and
the correct estimation of measurement precisions.
Any deformation survey must pay particular attention
to errors in the survey so that gross or systematic errors do not
contaminate the detection of movements and produce false results
(eg is the dam about to fail or did you forget to correct for the
EDM index error?)
Certain field techniques and procedures can be applied:
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Forced centring - eliminates errors from multiple
instrument/target setups, especially between epochs.
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Repeated measurements
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Simultaneous measurements
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Corrections for trunion axis tilt (in many
cases small zenith distances will be encountered)
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Advancing theodolite circles, etc.
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It is also important to determine in advance whether
absolute or relative movement is important as the former will require
an absolute datum to be defined outside the area of expected movement.
If only change in shape is important (eg bridge
sag) then a minimal constraint or free network solution can be used
to avoid any influence from external constraints. As in the diagram
there is no survey connection to stable control.

If a block shift or rotation is important as well
(eg dam deformation), then connections must be made to survey stations
which are sited in stable areas to provide the required absolute
datum. Often stable ground may be considerable distance away from
the area being surveyed for deformation.

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Surveys for deformation are generally repeated
at certain time intervals (measurement epochs). The time interval
depends on the expected movement / settlement of the structure and
the risk to life.
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Generally stations and targets are put in place
and suitable field procedures established. The established procedure
is repeated at each epoch to minimise systematic and gross errors
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Each of these repeated network surveys is known
as an epoch of measurement, so the comparison and analysis of the
results of the repeated surveys is commonly known as epoch testing
- Some structures deform at such a rate that the deformation must
be modelled during the time taken to perform a measurement epoch.
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Testing
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The essence of epoch testing is to determine whether
the differences between the coordinates from two different epochs
are statistically significant
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Epoch testing must take into account the precisions
of the coordinates, as well as the correlations between both the
coordinates of individual stations and coordinates of different
stations hence the full weight coefficient matrices from each epoch
contribute as follows :
Epoch 1:
x1 station coordinates vector
Q1 weight coefficient matrix
Epoch 2:
x2 station coordinates vector
Q2 weight coefficient matrix
and the differences in the coordinates and the associated weight
coefficients are:
d = x2 - x1
Qd = Q1 + Q2
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If free networks are employed then there should
be a 6 or 7 parameter transformation applied, to fit epoch 2 to
epoch 1, using all points in the network
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The first test conducted should always be the global
congruency test : analogous to the global test for a single network
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The quantity W = dt
Qd-1 d is tested against a Fisher statistic
at an appropriate confidence level, if W
passes then there has been no (statistically significant) movement
and the networks are congruent
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If W fails the global
congruency test then each point must be assessed by a local test
which compares the contribution to W
of the point against a Fisher critical value : analogous to the
local testing of residuals for a single network.
This test is done by recalculating W
without each point in turn
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The worst point (smallest W
value) is rejected and the entire testing
process repeated, including the transformation for free networks
(without the rejected points, which are now considered to have moved)
and the global congruency test
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Once the global congruency test passes, all those
points which have been rejected are considered to have moved whilst
those that are still contributing to W
are considered to be stable
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It is not unusual to test groups of points (eg
centre of the dam wall) and to amalgamate the survey data for stable
points over two or more epochs
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A good rule of thumb is that the point precisions
from the survey should be at least six times (preferably ten times!)
smaller than the expected magnitudes of the movement in order to
confidently detect the unstable points
- Where several epochs of data (usually > 3) are available a kinematic
or dynamic model for the epochs can be formed. A kinematic model only
considers the movements of the system without regard to their cause
- a dynamic model also models the movement, but considers the forces
causing the movement.
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Error Ellipses and Residuals
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Graphical representations of deformation analyses
are often shown as error ellipses (95% or some other confidence
interval - not the standard error ellipse) with vectors of movement
- differences between measurement epochs. Example.
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The visual representation is useful for empirical
checking and for the identification of the characteristics of any
movement. Examples with trends in residuals.
- 3D and multi-epoch representations are possible with CAD systems.
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References
Chrzanowski, A., 1986. Geotechnical and other Non_Geodetic
Methods in Deformation Measurements. Proceedings Deformation Measurements
Workshop Modern Methodology in Precise Engineering and Deformation Surveys
II. Bock, Y. (Ed.), Massachusetts, U.S.A., October 31 - November
1, 1986. Department of Earth, Atmospheric, and Planetary Sciences, Massachusetts
Institute of Technology, Massachusetts, U.S.A., pp. 112 - 153.
Krakiwsky, E. J., 1986. An Overview of Deformations,
Measurement Technologies, and Mathematical Modelling and Analysis. Proceedings
Deformation Measurements Workshop Modern Methodology in Precise Engineering
and Deformation Surveys II. Bock, Y. (Ed.), Massachusetts, U.S.A.,
October 31 - November 1, 1986. Department of Earth, Atmospheric, and
Planetary Sciences, Massachusetts Institute of Technology, Massachusetts,
U.S.A., pp. 7 - 33
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