2013
DOI: 10.1093/gji/ggt288
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Temperature-dependent transient creep and dynamics of cratonic lithosphere

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Cited by 12 publications
(3 citation statements)
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“…The application of Andrade's rheological model, which describes the transient creep, leads to oscillatory convective insta bility with a period of about 100 Ma, which corre sponds to the observed periodicity in the sedimenta tion (Birger, 1998;2012;2013). After the release of the compressive stresses, the linear creep deformations disappear, whereas the brittle deformations, which are irreversible, persist.…”
Section: The Stability Analysis Of the Flow Caused By Horizontal Compmentioning
confidence: 73%
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“…The application of Andrade's rheological model, which describes the transient creep, leads to oscillatory convective insta bility with a period of about 100 Ma, which corre sponds to the observed periodicity in the sedimenta tion (Birger, 1998;2012;2013). After the release of the compressive stresses, the linear creep deformations disappear, whereas the brittle deformations, which are irreversible, persist.…”
Section: The Stability Analysis Of the Flow Caused By Horizontal Compmentioning
confidence: 73%
“…For the slower processes characterized by the larger τ, inequality (18) gives a thinner elastic crust. For example, in the case of con vective oscillations of the lithosphere, which have a period of ~3 × 10 8 yr, the thickness of the elastic crust is at most 7 km (Birger, 2013). The lithosphere deter mined as a cold boundary layer formed by thermal convection in the mantle is much thicker than its upper elastic layer (elastic crust).…”
Section: The Rheology Of the Lithosphere And Its Depth Heterogeneitymentioning
confidence: 99%
“…В работе [Birger, 1998] реология, которая описывается интегральным уравнением, сводящимся к закону Андраде в случае постоянного напряжения, названа реологией Андраде. Реология Андраде применялась автором в предыдущих исследованиях [Birger, 1998;2000;2007;2012;2013;2016], где рассматривались такие геофизические процессы как затухание сейсмических волн, послеледниковые течения в мантии, малоамплитудные конвективные колебания в литосфере, происходящие при малых деформациях и переменных напряжениях. При исследовании этих процессов удобным математическим аппаратом является преобразование Лапласа по времени.…”
Section: Introductionunclassified