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Горное право. Словарь. Термины, понятия, институты

Горное право. Словарь. Термины, понятия, институты

А.И. Перчик

Геология месторождений нефти, газа и конденсатов (1)

Физические основы технологии добычи нефти

Физические основы технологии добычи нефти

Морис Маскет

Методы поисков и разведки месторождений полезных ископаемых (1)

Гидрологические основы росительных мелиорации в бассейнах рек Чу и Талас

Гидрологические основы росительных мелиорации в бассейнах рек ...

К. В. Цыцещо & В. В. Сумарокова

Гидрогеология (1)

Interfacial friction-induced pressure and implications for the formation and preservation of intergranular coesite in metamorphic rocks

Interfacial friction-induced pressure and implications for the ...

Shaocheng Ji & Qian Wang

Mineralogy (1)

Category: mantle

Geophysical Continua: Deformation in the Earth’s Interior

Geophysical Continua: Deformation in the Earth’s Interior

Brian Kennett & Hans-Peter Bunge

Geological and geophysical studies of the deep structure of the Earth (1)

New Theory of the Earth

New Theory of the Earth

Don L. Anderson

Geochemistry (1)

Theory of the Earth

Theory of the Earth

Don L. Anderson

Geological and geophysical studies of the deep structure of the Earth (1)

Mantle Dynamics Past, Present, and Future: An Introduction and Overview

Mantle Dynamics Past, Present, and Future: An Introduction and ...

D. Bercovici

INTRODUCTION TO THE PHYSICS OF THE EARTH'S INTERIOR

INTRODUCTION TO THE PHYSICS OF THE EARTH'S INTERIOR

JEAN-PAUL POIRIER

A Scientific Journey to the Center of the Earth

A Scientific Journey to the Center of the Earth

P. Olson

Overview – Mineral Physics: Past, Present, and Future

Overview – Mineral Physics: Past, Present, and Future

Density of the Earth & by Williamson & Adams (1923). Here, elastic constants of various rock types ... & gravitational data. Their work was marked by taking into account ... & the longitudinal & shear seismic wave velocities Vp & Vs) & mineral properties (Ks, the adiabatic bulk modulus & density, x1a), via d x1aðr Þ = – gðr Þdr _jðr Þ, ½1Š ... & is given by j(r) = V2 p (r)–4_3V2 s (r) = Ks (r) x1a (r) ½2Š. ... (...)

Overview - Mineral Physics: Past, Present, and Future

Overview - Mineral Physics: Past, Present, and Future

G. D. Price

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