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Fig. 5.20 Part of a time section from a large-scale refraction profile, plotted in reduced time using a reduction velocity of 6 km s -1 .The
section was derived from the LISPB lithospheric seismic profile across Britain established in 1974. Phase a 1 : head wave arrivals from a
shallow crustal refractor with a velocity of about 6.3 km s -1 ; phases c and e: wide-angle reflections from lower crustal interfaces: phase d:
head wave arrivals from the uppermost mantle (the P n phase of earthquake seismology). (From Bamford et al. 1978.)
capable of detection and delineation by fan-shooting
include salt domes, buried valleys and backfilled mine
shafts.
An irregular, areal distribution of shots and detectors
(Fig. 5.22(a)) represents a completely generalized ap-
proach to refraction surveying and facilitates mapping
of the three-dimensional geometry of a subsurface
refractor using the time term method of interpretation
(Willmore & Bancroft 1960, Berry & West 1966).
Rather than being an intrinsic aspect of the survey de-
sign, however, an areal distribution of shot points and
recording sites may result simply from an opportunistic
approach to refraction surveying in which freely avail-
able sources of seismic energy such as quarry blasts are
used to derive subsurface information from seismic
recordings.
The time term method uses the form of the travel-time
equation containing delay times (equation (5.18)) and is
subject to the same underlying assumptions as other in-
terpretation methods using delay times. However, in the
time term method a statistical approach is adopted to
deal with a redundancy of data inherent in the method
and to derive the best estimate of the interpretation para-
meters. Introducing an error term into the travel-time
equation
D 1
D 2
D 3
D 4
D 5
D 6
s
D 7
S 1
D 8
Time leads
associated with
ray paths
through salt
D 9
Salt
dome
s
S 2
Fig. 5.21 Fan-shooting for the detection of localized zones of
anomalous velocity.
any ray path which encounters an anomalous velocity
zone will be subject to a time lead or time lag depending
upon the velocity of the zone relative to the velocity of
the surrounding medium. Localized anomalous zones
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