Physics, asked by Yogesh1305, 27 days ago

For an amorphous solid, the essential aspect with which its structure differs with respect to that of crystalline solid is the absence of long-range order and translational periodicity. Elaborate on this statement by explaining with the aid of a diagram the situation prevailing in the gaseous –state of a given material.

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Answered by avtash948
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Answered by s18677apaulom409761
2

Answer:

Amorphous solid, any noncrystalline solid in which the atoms and molecules are not organized in a definite lattice pattern. Such solids include glass, plastic, and gelSolids and liquids are both forms of condensed matter; both are composed of atoms in close proximity to each other. But their properties are, of course, enormously different. While a solid material has both a well-defined volume and a well-defined shape, a liquid has a well-defined volume but a shape that depends on the shape of the container. Stated differently, a solid exhibits resistance to shear stress while a liquid does not. Externally applied forces can twist or bend or distort a solid’s shape, but (provided the forces have not exceeded the solid’s elastic limit) it “springs back” to its original shape when the forces are removed. A liquid flows under the action of an external force; it does not hold its shape. These macroscopic characteristics constitute the essential distinctions: a liquid flows, lacks a definite shape (though its volume is definite), and cannot withstand a shear stress; a solid does not flow, has a definite shape, and exhibits elastic stiffness against shear stress.

On an atomic level, these macroscopic distinctions arise from a basic difference in the nature of the atomic motion. Figure 1 contains schematic representations of atomic movements in a liquid and a solid. Atoms in a solid are not mobile. Each atom stays close to one point in space, although the atom is not stationary but instead oscillates rapidly about this fixed point (the higher the temperature, the faster it oscillates). The fixed point can be viewed as a time-averaged centre of g

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