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Beams, Frames and Rings

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Solid Mechanics

Abstract

In the previous chapter, while developing as the primary effort certain variational principles of mechanics, we entered into a discussion of trusses in order both to illustrate certain aspects of the theory and to present a discussion of the most simple class of structures. We could take on this dual task at this stage because the stress and deformation of any one single member of a truss is a very simple affair. That is, the only stress on any section (away from the ends)

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Notes

  1. 1.

    At the ends, in reality, due to friction of the supports and complicated boundaries of the member it is unlikely that simple uniaxial tension or compression will exist.

  2. 2.

    Note because we are neglecting the shear deformation associated with Ï„ xz , w(x) represents deflection due only to bending.

  3. 3.

    You will be asked as an exercise (Problem 4.1) to find these results using the Δ operator.

  4. 4.

    The shear stress must then be zero at the upper and lower boundary surfaces.

  5. 5.

    Among the many definitions are those stemming from relating the maximum shear stress through the thickness, as developed from a more exact solution, to the approximation (4.35), or those from matching of certain wave speeds from the dynamics of a Timoshenko beam to more accurate results of elasticity theory.

  6. 6.

    Journal of Applied Mechanics, June 1966, p. 335.

  7. 7.

    As an exercise you will be asked to verify the following results by carrying out the extremization process.

  8. 8.

    Note before proceeding further that solutions of the uncoupled equations must be checked in the coupled form since the uncoupled equations form a higher-order set of equations having thus as an outcome, extraneous solutions.

  9. 9.

    The coefficients 3 and 4 have been chosen so as to give w 1 a zero slope at x = L/2 as is required of a beam with a continuous slope and symmetry about x = L/2.

  10. 10.

    We shall consider eigenfunctions in Chap. 7.

  11. 11.

    Note that origin of coordinates is at left end of beam (see Fig. 4.11).

  12. 12.

    Constraints not needed for equilibrium.

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Dym, C.L., Shames, I.H. (2013). Beams, Frames and Rings. In: Solid Mechanics. Springer, New York, NY. https://doi.org/10.1007/978-1-4614-6034-3_4

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  • DOI: https://doi.org/10.1007/978-1-4614-6034-3_4

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  • Publisher Name: Springer, New York, NY

  • Print ISBN: 978-1-4614-6033-6

  • Online ISBN: 978-1-4614-6034-3

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