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  2. Schmid's law - Wikipedia

    en.wikipedia.org/wiki/Schmid's_Law

    Schmid's Law states that the critically resolved shear stress (τ) is equal to the stress applied to the material (σ) multiplied by the cosine of the angle with the vector normal to the glide plane (φ) and the cosine of the angle with the glide direction (λ). Which can be expressed as: [2] =

  3. Slip (materials science) - Wikipedia

    en.wikipedia.org/wiki/Slip_(materials_science)

    Slip systems in zirconium alloys. 𝒃 and 𝒏 are the slip direction and plane, respectively, and 𝝎 is the rotation axis calculated in the present work, orthogonal to both the slip plane normal and slip direction. The crystal direction of the rotation axis vectors is labelled on the IPF colour key.

  4. Critical resolved shear stress - Wikipedia

    en.wikipedia.org/wiki/Critical_resolved_shear_stress

    The Schmid Factor for an axial applied stress in the [] direction, along the primary slip plane of (), with the critical applied shear stress acting in the [] direction can be calculated by quickly determining if any of the dot product between the axial applied stress and slip plane, or dot product of axial applied stress and shear stress ...

  5. Frank–Read source - Wikipedia

    en.wikipedia.org/wiki/Frank–Read_source

    Consider a straight dislocation in a crystal slip plane with its two ends, A and B, pinned. If a shear stress τ {\displaystyle \tau } is exerted on the slip plane then a force F = τ ⋅ b x {\displaystyle F=\tau \cdot bx} , where b is the Burgers vector of the dislocation and x is the distance between the pinning sites A and B, is exerted on ...

  6. Slip bands in metals - Wikipedia

    en.wikipedia.org/wiki/Slip_bands_in_metals

    Dislocations are generated on a single slip plane They point out that a dislocation segment (Frank–Read source), lying in a slip plane and pinned at both ends, is a source of an unlimited number of dislocation loops. In this way the grouping of dislocations into an avalanche of a thousand or so loops on a single slip plane can be understood. [19]

  7. Lomer–Cottrell junction - Wikipedia

    en.wikipedia.org/wiki/Lomer–Cottrell_junction

    When two perfect dislocations encounter along a slip plane, each perfect dislocation can split into two Shockley partial dislocations: a leading dislocation and a trailing dislocation. When the two leading Shockley partials combine, they form a separate dislocation with a burgers vector that is not in the slip plane. This is the Lomer ...

  8. How To Fill Out a W-4: A Complete Guide - AOL

    www.aol.com/news/fill-w-4-complete-guide...

    When you start a new job -- or change your name or marital status -- you will probably have to fill out a new W-4 tax form. Your completed form is used to determine how much of your income your...

  9. Geometrically necessary dislocations - Wikipedia

    en.wikipedia.org/wiki/Geometrically_necessary...

    Nye has introduced a set of tensor (so-called Nye's tensor) to calculate the geometrically necessary dislocation density. [4] For a three dimension dislocations in a crystal, considering a region where the effects of dislocations is averaged (i.e. the crystal is large enough). The dislocations can be determined by Burgers vectors.