This
appears to be borne out within the evidence of the sedimentary records. There
seems to be wide recognition of distinct pulses in the rates and forms of sedimentary
deposition that have occurred over wide geographical areas. Deep-sea drilling
in both the Atlantic and Pacific have penetrating into distinct Mesozoic (circa
65 - 250Mbp‡) sequences to reveal correlated stratigraphic
units,
Jansa et al (1979), which seem to closely resemble those typical of the
Tethyan, Wezel (1985). At around 110Mbp a dramatic change in the nature of
the sediments occurred. This saw the ending of the limestone formations and the
sudden increase in clay and quartzose beds. At this time deposition rates are
seen to accelerate and be accompanied by tectonic changes at large numbers of the
world’s passive margins, De Graciansky et al (1987), involving widespread
regional subsidence and tectonic mobility at the margins, Kent (1977) and Wezel
(1985).
Recording
time-stratigraphic relationships of sequences in the North American craton, in
which certain geological periods display non-depositional hiatuses while others
show rapid and widespread deposition, Sloss (1964) commented that “in other
words, let us not here argue the validity of the sequence concept, but, rather,
proceed to a consideration of the alternation between depositional and non-depositional
episodes of the craton and the significance of these events. Are the successive
episodes repetitions of the same behavior? If differences exist, is there a
systematic pat tern of recurrence?
What relationship, if any, appears to exist between cratonic events and those
occurring in neighboring mobile belts?” He went on to conclude from his earlier
work, Sloss (1963), that it should be “reiterated … that the stratigraphic
record of the North American craton (late Precambrian to the present) is
punctuated by six interregional, cratonwide unconformities. The unconformities
are recognizable surfaces which subdivide the cratonic stratigraphic column
into six vertically successive groupings of rocks, each identified by a
geographic term in the manner of other lithostratigraphic units. These units
are defined and described in the aforementioned paper, and their
time-stratigraphic limits are indicated” very graphically in Figure 2 (Sloss,
1964).
There
is other evidence to suggest that the pulses in epeirogeny, often triggering
periods of mountain building activity, also occur over quite distinct periods
of geological time. Synchronous periods of mountain building have been compared
with paleoclimate temperature estimates over the Phanerozoic (Post & Illis,
2009) and noted by Kalander et alia (2011) to have a close correspondence with
the geological evidence for the occurrence of ice ages, supporting the model outlined by Croll (2007). Ollier (2006b) has made
detailed analysis of the spurt in epeirogenic events during the so called
“neotectonic” period of the late Cenozoic. And evidence of such regional uplift
in Plio-Pleistocene and its possible thermochronology has been very clearly
identified as a global process from the study of marine and fluvial terrace
structures (see for example Bridgeland (1988, 2010) and Westaway (2002, 2010)*.
None of this seems compatible with the PT or EE models.
Over the next few postings I will examine each of these aspects of the dynamic processes of tectonic evolution. These postings will attempt to demonstrate that the phasing of periods of rapid build-up of sedimentary deposits followed by periods during which vast areas of continental landmass uplift or subside, are no accident. It will suggest to the extent consistent with the far from universally accepted data, that this phasing of tectonic activity is driven by forces derived from Earth’s interactions with our galaxy, solar system, and especially the Sun. Specifically, it will attempt to demonstrate that over deep geological timescales the phases during which continents undergo maximum rates of erosion and synchronously marine sedimentation experiences its greatest rates of build-up are closely locked-in to the periodicity of warm-ages. Furthermore, the thermal-mechanical model used to explain this locking-in process will also be suggested to account for the periods during which the Earth’s crust experiences its greatest rates of epeirogenic rise and fall.
‡ Experienced geologists will of course not need my numerical interpretations of the conventionally used geological periods, but as someone not trained in the nomenclature I find it very frustrating reading geological works where numerical values are not given. It means a chart is required to translate to real time – would it not be easier to include real time translations as a matter of course?
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