Abstract
I assume throughout this chapter that the underlying observer is inertial and the external body forces b and (hence) e and the external interface forces
and
are inertial. Then b has the form (7-1 ). I now characterize
through the equivalence of inertial force and temporal changes in momentum, and, knowing
,
is determined through the equivalence of inertial working and temporal changes in kinetic energy.1
Following a procedure of Podio-Guidugli [1997] as applied by Gurtin and Podio-Guidugli [1996a,b, 1997].
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© 2000 Springer-Verlag New York, Inc.
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(2000). Inertia. Basic Equations for the Interface. In: Configurational Forces as Basic Concepts of Continuum Physics. Applied Mathematical Sciences, vol 137. Springer, New York, NY. https://doi.org/10.1007/978-0-387-22656-9_12
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DOI: https://doi.org/10.1007/978-0-387-22656-9_12
Publisher Name: Springer, New York, NY
Print ISBN: 978-0-387-98667-8
Online ISBN: 978-0-387-22656-9
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