Coupled nonlinear wave equations are obtained for the special case of wave motion in a thin rod with circular cross-section resulting from a large-amplitude torsional source. Lagrangian mechanics are employed to obtain the wave equations from expressions for the kinetic and potential energy densities in the rod due to an assumed displacement field. Longitudinal waves are generated at quadratic order in strain by the torsional wave through inertial (centrifugal) and elastic forces. Nonlinear effects on the torsional wave occur at cubic order in strain, due to both interaction with the longitudinal wave and strain-hardening shear nonlinearity. While the torsional wave propagates without dispersion, the longitudinal wave is subject to leading-order effects of geometrical dispersion when its wavelength is comparable to the rod radius. The case of weak nonlinearity is analyzed, for which the torsional wave propagates without nonlinear distortion while finite-amplitude effects generate a longitudinal wave. An analytical solution reveals that inertial and elastic forces resulting from a harmonic travelling torsional wave work against each other in the generation of the longitudinal second harmonic. Numerical solutions for transient source motion highlight interaction between the torsional and longitudinal modes near the source, and effects of geometrical dispersion on the longitudinal wave.
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