Quasi-solid: Difference between revisions
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'''Quasi-solid''' is the physical term for a semi-[[solid]]. While similar to a solid in some respects (it can support its own weight and hold its shape), a quasi-solid also shares some properties of [[liquid]]s, such as shape conformity to something applying pressure to it, or the ability to flow under pressure. Quasi-solids are also known as [[amorphous]] solids because at the microscopic scale they are disordered, unlike traditional [[crystalline]] solids. |
'''Quasi-solid''' is the physical term for a semi-[[solid]]. While similar to a solid in some respects (it can support its own weight and hold its shape), a quasi-solid also shares some properties of [[liquid]]s, such as shape conformity to something applying pressure to it, or the ability to flow under pressure. Quasi-solids are also known as [[amorphous]] solids because at the microscopic scale they are disordered, unlike traditional [[crystalline]] solids. For instance, common Glass is a semi-solid, because on the molecular level, its units, aligned in the crystal lattice, are octagonal in structure. When octagons are tiled together in the lattice, their eight-sided geometry forces spaces to be formed between units, which is the cause for Glass' existence as a quasi-solid. |
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Revision as of 15:48, 10 June 2010
Quasi-solid is the physical term for a semi-solid. While similar to a solid in some respects (it can support its own weight and hold its shape), a quasi-solid also shares some properties of liquids, such as shape conformity to something applying pressure to it, or the ability to flow under pressure. Quasi-solids are also known as amorphous solids because at the microscopic scale they are disordered, unlike traditional crystalline solids. For instance, common Glass is a semi-solid, because on the molecular level, its units, aligned in the crystal lattice, are octagonal in structure. When octagons are tiled together in the lattice, their eight-sided geometry forces spaces to be formed between units, which is the cause for Glass' existence as a quasi-solid.