Skip to main content

Small Oscillations

  • Chapter
  • First Online:
Classical Mechanics

Part of the book series: Undergraduate Lecture Notes in Physics ((ULNP))

  • 3396 Accesses

Abstract

Oscillatory or vibrational motion has applications in all of physics as well as in engineering. We begin with the one-dimensional harmonic oscillator, including friction and external excitation, and continue to study wave propagation along linear chains, which eventually leads us to normal mode analysis.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 49.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 64.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    Stokes, Sir George Gabriel, British mathematician and physicist, *Skreen (County Sligo, Ireland) 13.8.1819, †Cambridge 1.2.1903.

  2. 2.

    A justification for (6.8) in a special case is given on p. 276.

  3. 3.

    Notice that if \( \vec {F} = - \frac{\partial U}{ \partial \vec {r}} \equiv -\vec \nabla U \), then \( \oint \vec {F} \cdot d \vec {s} = - \oint \vec {\nabla } U \cdot d \vec {s} = - \oint d U = 0 \).

  4. 4.

    This means we take a snapshot, showing the oscillating chain at time \(t=0\).

  5. 5.

    Everything we just discussed also applies to the \(\sin \)-part.

  6. 6.

    The displacements \(u_s\) and \(v_s\) are real of course.

  7. 7.

    Notice that \( \overline{\sin ^2 ( \ldots )} = \frac{\omega }{2 \pi } \int _0^{2 \pi /\omega } \sin ^2 (\omega t + c) dt \), where the quantity c is independent of t. The substitution \( x = \omega t + c \) yields

    $$\begin{aligned} \overline{\sin ^2 ( \ldots )} = \frac{1}{2 \pi } \int _c^{2 \pi + c} \sin ^2 x d x = \frac{1}{2} \frac{1}{2 \pi } \int _c^{2 \pi + c} \underbrace{\left( \sin ^2 x + \cos ^2 x \right) }_{= 1} dx = \frac{1}{2} \;. \end{aligned}$$
  8. 8.

    E.g., \(\frac{K^{bb}}{2} \delta b_1 \delta b_2\).

References

  1. D.R. Lide (ed.), Handbook of Chemistry and Physics (CRC Press, Boca Raton, 2003)

    Google Scholar 

  2. W.D. Cornell, P. Cieplak, C.I. Bayly, I.R. Gould, K.M. Merz, D.M. Ferguson, D.C. Spellmeyer, T. Fox, J.W. Caldwell, P.A. Kollman, A second generation force field for the simulation of proteins, nucleic acids, and organic molecules. J. Am. Chem. Soc. 117, 5179 (1995)

    Article  Google Scholar 

  3. U. Burkert, N.L. Allinger, Molecular Mechanics, vol. 177, ACS Monograph (American Chemical Society, Washington D.C., 1982)

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Reinhard Hentschke .

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing AG

About this chapter

Cite this chapter

Hentschke, R. (2017). Small Oscillations. In: Classical Mechanics. Undergraduate Lecture Notes in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-48710-6_6

Download citation

Publish with us

Policies and ethics