Skip to main content

Affine Dynamics

  • Chapter
  • First Online:
Shapes and Dynamics of Granular Minor Planets
  • 368 Accesses

Abstract

In this chapter, we obtain the equations of motion that govern the simplest, non-trivial, deformable dynamics of an ellipsoidal body. We will employ volume averaging (also known as the method of moments or the virial method) to this end.

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

Access this chapter

eBook
USD 16.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 109.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 109.99
Price excludes VAT (USA)
  • Durable hardcover 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.

    Further support for analyses that assume that granular minor planets deform in an affine manner will be found from results in plasticity theory (Sect. 4.4), and when comparing the predictions of such investigations with simulations and observation in the coming chapters.

  2. 2.

    In fact, if we had retained \({\mathsf {B}}_S\) and \({\mathsf {B}}_P\) in their entirety when computing \({\mathbf {F}}_S\) and \({\mathbf {F}}_P\), then the formulae derived in Sect. 3.4 for \({\mathbf {F}}_S\) and \({\mathbf {F}}_P\) obey Newton’s third law, i.e., yield forces that are equal and opposite. This is proved as follows. From Maciejewski (1995), the total force exerted by the primary on the secondary, \({\mathbf {F}}_S = -\rho ''\rho 'G\int _{V''}\int _{V'}\frac{\overline{\mathbf {x}}_S - \overline{\mathbf {x}}_P}{\left| \overline{\mathbf {x}}_S - \overline{\mathbf {x}}_P\right| ^3}\mathrm{{d}}V' \mathrm{{d}}V''\), where \(\overline{\mathbf {x}}_S = {\mathbf {r}}_S + {\mathbf {x}}_S\) and \(\overline{\mathbf {x}}_P= {\mathbf {r}}_P + {\mathbf {x}}_P\) locate with respect to the mass center C material points in the primary and the secondary, respectively; see Fig. 3.1. The force \({\mathbf {F}}_P\) has the same formula, but with minus sign, so that \({\mathbf {F}}_S = -{\mathbf {F}}_P\). From Chandrasekhar (1969, p. 48, Theorem 7), \(-\rho 'G\int _{V'}\frac{\overline{\mathbf {x}}_S - \overline{\mathbf {x}}_P}{\left| \overline{\mathbf {x}}_S - \overline{\mathbf {x}}_P\right| ^3}\mathrm{{d}}V' = -2\pi \rho 'G{\mathsf {B}}_P\cdot {\mathbf {d}}_S\) , as it is the force per unit mass exerted at \({\mathbf {d}}_S\) by the primary; see Fig. 3.1. Similarly, \(-\rho ''G\int _{V''}\frac{\overline{\mathbf {x}}_P - \overline{\mathbf {x}}_S}{\left| \overline{\mathbf {x}}_P - \overline{\mathbf {x}}_S\right| ^3}\mathrm{{d}}V'' = -2\pi \rho ''G{\mathsf {B}}_S\cdot {\mathbf {d}}_P\). Thus, \({\mathbf {F}}_S = \rho ''\int _{V''}\left( -2\pi \rho 'G{\mathsf {B}}_P\cdot {\mathbf {d}}_S\right) \mathrm{{d}}V'' \) and \({\mathbf {F}}_P = \rho '\int _{V'}\left( -2\pi \rho ''G{\mathsf {B}}_S\cdot {\mathbf {d}}_P\right) \mathrm{{d}}V'\), which are exactly the formulae obtained in Sect. 3.4; see equations before (3.39) and (3.44). Clearly, \({\mathbf {F}}_S = -{\mathbf {F}}_P\).

  3. 3.

    In a contact binary, the primary and the secondary touch each other. There may or may not be significant contact forces present. In this book, we will assume that the contact forces, if any, are insignificant compared to other forces present. The extent to which this assumption is valid will often be revealed by the mismatch of our predictions with observations; see, e.g., applications to binary near-Earth binaries in Sect. 10.8.

References

  • M. Abramowitz, I.A. Stegun, Handbook of Mathematical Functions (Dover, New York, 1965)

    Google Scholar 

  • J.P. Boyd, Chebyshev and Fourier Spectral Methods, 2nd edn. (Dover, New York, 2001)

    Google Scholar 

  • S. Chandrasekhar, Ellipsoidal Figures of Equilibrium (Yale University Press, New Haven, 1969)

    Google Scholar 

  • C. Chree, Further applications of a new solution of the equations of an isotropic elastic solid, mainly to various cases of rotating bodies. Quart. J. Math 23, 11–33 (1889)

    Google Scholar 

  • D.T. Greenwood, Principles of Dynamics (Prentice-Hall, Englewood Cliffs, 1988)

    Google Scholar 

  • O.D. Kellogg, Foundations of Potential Theory (Dover, New York, 1953)

    Google Scholar 

  • Z. Kopal, Dynamics of Close Binary Systems (D. Reidel Publishing Company, Dordrecht, 1978)

    Book  Google Scholar 

  • D. Lai, F. Rasio, S.L. Shapiro, Ellipsoidal figures of equilibrium: compressible models. Astrophys. J. Suppl. S. 88, 205–252 (1993)

    Google Scholar 

  • D. Lai, F. Rasio, S.L. Shapiro, Equilibrium, stability, and orbital evolution of close binary systems. Astrophys. J. 423, 344–370 (1994)

    Google Scholar 

  • A.E.H. Love, A Treatise on the Mathematical Theory of Elasticity, 4th edn. (Dover, New York, 1946)

    Google Scholar 

  • A.J. Maciejewski, Reduction, relative equilibria and potential in the two rigid bodies problem. Celest. Mech. Dyn. Astr. 63, 1–28 (1995)

    Article  Google Scholar 

  • C.D. Murray, S.F. Dermott, Solar System Dynamics (Cambridge University Press, Cambridge, 1999)

    Google Scholar 

  • D.J. Scheeres, Stability of relative equilibria in the full two-body problem. Ann. NY Acad. Sci. 81–94, 1017 (2004)

    Google Scholar 

  • D.J. Scheeres, Orbital Motion in Strongly Perturbed Environments: Applications to Asteroid, Comet and Planetary Satellite Orbiters (Springer, New York, 2012)

    Book  Google Scholar 

  • I. Sharma, The equilibrium of rubble-pile satellites: The Darwin and Roche ellipsoids for gravitationally held granular aggregates. Icarus 200, 636–654 (2009)

    Google Scholar 

  • I. Sharma, Equilibrium shapes of rubble-pile binaries: the Darwin ellipsoids for gravitationally held granular aggregates. Icarus 205, 638–657 (2010)

    Article  Google Scholar 

  • I. Sharma, J.T. Jenkins, J.A. Burns, Tidal encounters of ellipsoidal granular asteroids with planets. Icarus 183, 312–330 (2006)

    Google Scholar 

  • I. Sharma, J.T. Jenkins, J.A. Burns, Dynamical passage to approximate equilibrium shapes for spinning, gravitating rubble asteroids. Icarus 200, 304–322 (2009)

    Google Scholar 

  • S. Sridhar, S. Tremaine, Tidal disruption of viscous bodies. Icarus 95, 86–99 (1992)

    Article  Google Scholar 

  • S.P. Timoshenko, J.N. Goodier, Theory of Elasticity, 3rd edn. (Mc-Graw Hill, New York, 1970)

    Google Scholar 

  • C. Truesdell, R.A. Toupin, The Classical Field Theories, in Encyclopedia of Physics Vol. III/I: Principles of Classical Mechanics and Field Theory, ed. by S. Flügge (Springer, Berlin, 1960), pp. 226–793

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Ishan Sharma .

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing Switzerland

About this chapter

Cite this chapter

Sharma, I. (2017). Affine Dynamics. In: Shapes and Dynamics of Granular Minor Planets. Advances in Geophysical and Environmental Mechanics and Mathematics. Springer, Cham. https://doi.org/10.1007/978-3-319-40490-5_3

Download citation

Publish with us

Policies and ethics