Thermal strains

Temperature change can also cause strain. In an isotropic material the thermally induced extensional strains are equal in all directions, and there are no shear strains. In the simplest cases,…

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Stress-strain relations

Linear elastic isotropic solid The simplest type of stress-strain relation is that of the linear elastic solid, considered in circumstances for which |∂ui/∂Xj|<< 1 and for isotropic materials, whose mechanical…

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What are Hole Basis System and Shaft Basis system?

Hole Basis System and Shaft Basis system – In the Machine design process there are different components are mated together to make the machine. These components will have a different function. Base on…

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Finite deformation and strain tensors

In the theory of finite deformations, extension and rotations of line elements are unrestricted as to size. For an infinitesimal fibre that deforms from an initial point given by the…

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Small-strain tensor

The small strains, or infinitesimal strains, εij are appropriate for situations with |∂uk/∂Xl|<< 1 for all k and l. Two infinitesimal material fibres, one initially in the 1 direction and…

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Types of fit

The three types of fit are: 1.     Clearance: The hole is larger than the shaft, enabling the two parts to slide and / or rotate when assembled. 2.     Location / transition: The…

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Geometry of deformation

Strain and strain-displacement relations The shape of a solid or structure changes with time during a deformation process. To characterize deformation, or strain, a certain reference configuration is adopted and…

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Equations of motion

Now the linear momentum principle may be applied to an arbitrary finite body. Using the expression for Tj above and the divergence theorem of multivariable calculus, which states that integrals…

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Stress

Assume that F and M derive from two types of forces, namely, body forces f, such as gravitational attractions—defined such that force fdV acts on volume element dV (see Figure…

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Linear and angular momentum principles: stress and equations of motion

Let x denote the position vector of a point in space as measured relative to the origin of a Newtonian reference frame; x has the components (x1, x2, x3) relative…

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