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Ch. 1: Introduction

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INTRODUCTION
23
ZONES OF ROCK STRAIN
In the contraction, or assumed contraction, of the earth's crust, the stupendous strains developed will affect different rocks in a different way as they are brittle or tough, thickly bedded or in thin layers, and it will also affect them differently as they are removed at comparatively great distances from the surface. Van Hise, who has developed this principle, assumes that at a depth of 30,000 feet below the earth's surface the overlying pressure is so great that the rocks cannot break or crack under compression, but that they How, that their particles adjust themselves to new positions of stability under the strain, by movement, that indeed they behave like soft or mobile bodies, like wax, for instance. Such movements must be in­finitesimal, but as every component molecule of the rock shifts its position to accommodate the stress, the whole mass of rock has been welded and moulded like a plastic body. This is called the Zone of Flowage.
Above this zone the pressure is relieved or diminished, and the stronger rock layers will break or crack when the thrusts of compression take place; they will not then How, while the weaker, less resistant rocks will flow, and the resultant mix­ture of effects, where some rocks yield without losing continu­ity, and other rocks break, represents the so-called Zone of Fracture and Flowage.
Above this zone again, and now in closer proximity to the surface, all the rocks break, and faults, joints, crevices, are formed, shatterings occur, crushings and the familiar results of smashing and even pulverization. This is the Zone of Fracture.
The rocks of New York Island suggest a complementary hypothesis. They have not been in the zone of flowage, per­haps very near it; they have participated in the strains of the zone of fracture, but they have been bent and folded, crumpled, and thrown into rippling undulations, which may be seen on
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