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The Modeling of Single-dof Mechanical Systems

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Dynamic Response of Linear Mechanical Systems

Part of the book series: Mechanical Engineering Series ((MES))

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Abstract

The need of dynamics models in engineering, objectives, scope, and limitations of mechanical analysis in general and of elements of systems (masses, springs, dashpots, energy sources and energy sinks); system; mechanical system; viscous, hysteretic and Coulomb friction.

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Notes

  1. 1.

    http://varan_bhaath.tripod.com/Pages/Saptapadi.htm.

  2. 2.

    Sometimes, dynamical systems are described by difference equations (case of discrete-time systems), integral equations and even by integro-differential equations.

  3. 3.

    These systems “forget” the history of their excitation.

  4. 4.

    Engineering systems are invariablymultibody systems, i.e., systems of rigid and deformable bodies. When a rigid body is constrained to move in one single direction, it can be modeled as a particle, but modern software for mechanical analysis regards all elements as bodies, their constraints being included explicitly in the form of algebraic relations in the mathematical model.

  5. 5.

    a.k.a parallel-axis theorem.

  6. 6.

    For brevity, translational springs and their corresponding stiffness are referred to as “springs” and “stiffness” when no confusion is possible.

  7. 7.

    FBD is the abbreviation of free-body diagram.

  8. 8.

    Henceforth, vectors are represented with lower-case boldfaces, matrices with upper-case boldfaces, scalars with math italics. Thus, while ω is a vector, ω is a scalar.

  9. 9.

    The scalar product of two vectors a and b, of the same dimension, also termed thedot product, is represented by the two alternative expressions ab and a T b.

  10. 10.

    See a textbook on kinematics of mechanisms.

  11. 11.

    The formal derivation of the Lagrange equations lying beyond the scope of the book, the reader is invited to review this derivation, as pertaining to systems of particles in a mechanics book, e.g., [3].

  12. 12.

    Erroneously, translational springs are sometimes referred to as “linear.”

  13. 13.

    Again, translational dashpots are sometimes erroneously referred to as “linear.”

  14. 14.

    Actually, friction force between pin and plate is present, but it develops no work because the point of application Q of this force is stationary. The sole role of the friction force here is to prevent sliding.

  15. 15.

    The expressions (1.49a–c) are said to be “first-order” because all variations δq and \(\delta \dot{q}\) appear linearly therein.

  16. 16.

    One equilibrium configuration can be obtained from the other by looking at the latter with the aid of a mirror. Mirror-imaging, of course, shouldn’t affect the intrinsic properties of the system.

  17. 17.

    For ease of visualization, δθ and δψ are exaggerated in the figure, but they are both assumed to be “small”.

References

  1. Almen J, László A (1936) The uniform-section disk spring. Trans ASME 58:305–314

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  2. Di Benedetto A and Pennestrì E (1993) Introduzione alla cinematica dei meccanismi. Moti infinitesimi. Casa Editrice Ambrosiana, Milan

    Google Scholar 

  3. Meriam JL, Kraige LG (1992) Engineering mechanics. Dynamics, vol 2, 5th edn. Wiley, New York

    Google Scholar 

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Correspondence to Jorge Angeles .

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Angeles, J. (2011). The Modeling of Single-dof Mechanical Systems. In: Dynamic Response of Linear Mechanical Systems. Mechanical Engineering Series. Springer, Boston, MA. https://doi.org/10.1007/978-1-4419-1027-1_1

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  • DOI: https://doi.org/10.1007/978-1-4419-1027-1_1

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  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4419-1026-4

  • Online ISBN: 978-1-4419-1027-1

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