Deformation of single and polycrystals

Deformation of single and polycrystals

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  DEFORMATION OF SINGLECRYSTALS AND POLY-CRYSTALLINE MATERIALS BATCH 7
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  DEFORMATION OF SINGLECRYSTALS • When a single crystal is deformed under a tensile stress, it is observed that plastic deformation occurs by slip on well‐defined parallel crystal planes. • Slip always occurs on a particular set of crystallographic planes, known as slip planes. • Slip always takes place along a consistent set of directions within these planes. These are called slip directions. • Slip occurs most readily on the plane of greatest atomic density.
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  • The combinationof slip plane and slip direction together makes up a slip system. Tensile deformation of single crystal without constraint
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  SCHMID’S LAW • Tomove dislocations, a certain stress must be applied to overcome the resistance to dislocation motion. • Slip occurs when the shear stress acting in the slip direction on the slip plane reaches a critical value known as critical resolved shear stress. • is the minimum shear stress required to initiate slip. • Condition for dislocation motion: CRSS RCRSS  
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      coscoscoscos cos/ cos  A P A P R • Thisis called schmid’s law.
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  • The quantityCosφ Cosλ is known as the Schmid Factor (M) . • The tensile stress at which the material start to slip is the yield strength of the material. • In a given crystal, there may be many available slip systems. • As the tensile load is increased, the resolved shear stress on each system increases until eventually is reached on one system. • The crystal begins to plastically deform by slip on this system, known as the primary slip system. CRSS
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  • The stressrequired to cause slip on the primary slip system is the yield stress of the single crystal. • From Schmid's Law, it is apparent that the primary slip system will be the system with the greatest Schmid factor (M). MYCRSS  
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  Plastic Deformation ofpolycrystalline materials • Deformation and slip is more complex in polycrystalline materials . • Due to the random crystallographic orientations of the numerous grains and the effect of neighbouring atoms, the direction of slip varies from one grain to another. • These materials are made up of a number of small crystals or grains. • For each crystal, slip occurs along the slip system that has the most favourable orientation.
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  • During deformation,each individual grain is constrained to some degree in shape it may assume by its neighbouring grains. • Prior to deformation the grains are equiaxed. • After deformation, the grains become elongated along the direction in which specimen was extended. • Dislocation motion occurs along slip systems with favourable orientation (i.e. highest resolved shear stress). • The grain boundaries exert repulsive force on the successive dislocations coming down the slip plane. • Thus the grain boundaries cause dislocation pile-up.
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  • Since grainboundaries diminish dislocation mobility, polycrystalline materials are stronger than single crystals. • Larger plastic deformation corresponds to elongation of grains along direction of applied stress. Before After
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  • When acrystal is surrounded by other crystals of different crystallographic orientation, deformation of the crystal cannot start at the primary system as the strain taking place need to be compatible with the strain at the boundary in the other crystals. • Because strains along grain boundaries must be the same for each grain, the grains will deform in a cooperative manner. • Since plastic deformation of a single grain is restrained by its neighboring grain, a polycrystalline material will have an intrinsically greater resistance to plastic flow than would a single crystal.
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  REFERENCES 1. George EDieter, “Mechanical metallurgy”, Mc Graw Hill, Singapore, 1995. 2. M.N. Shetty, “Dislocations and Mechanical Behaviour of Materials”, PHI Learning Private Ltd,2013.
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