Ok, I found a variety of info. Ref. 1 & 2 came up with a (3D) solution to the problem. It produced a number of wave types: longitudinal, shear, Rayleigh, von Schmidt, Love, etc. Even looking at the stress outputs, it's not 100% clear how much wave production per type there is. What is clear is: for long periods of time the traditional 1D longitudinal wave theory is sufficient. For short times various other waves (especially von Schmidt waves) are significantly impacting results. Also apparent is the production of Rayleigh waves on the surface of the rods. (It should be noted that the vibratory phenomenon is more pronounced in rectangular bars than circular. [Ref. 3].) Radial displacements seem to approximately correspond to Love wave theory in Ref. 1.
This still left me with part of my original question unanswered: how much of each wave? Given the math of some of the sources was impenetrable, I fell back on another source: the solution to a circular disk siting on a homogenous half space. (I.e. something typically used to represent dynamically loaded foundations.) Results show (in such a case; see Ref. 4) that at low forcing frequencies (and for a Poisson's ratio of about 0.33), Rayleigh waves can take up as much as two-thirds of the waves produced by power transmitted (7% P-waves, S-waves transmit the rest). However, at high forcing frequencies (like impact), the power is almost entirely transmitted by P-Waves and S-Waves. (The vast majority being P-waves.)
While this may seem to be a inappropriate comparison at first......Ref. 4 states:
"Very high frequency vibrations can radiate only vertically downward without spreading; in effect they are confined within the prismatic "rod" of soil directly under the foundation......The physical reason why the importance of Rayleigh waves diminishes with frequency is quite simple . The depth of penetration of the Rayleigh wave....is about one wavelength beneath the surface (skin effect). The power propagates towards infinity through cylinders of this depth and ever-growing radius. Because the wavelength is inversely proportional to the frequency, the cylinder "surface infinity" becomes flatter and flatter as the frequency increases; and the window through which the power must pass closes to a circular slit."
That helps explain some of the wave production I see (away from impacted [rod] ends).
If I find more....will post.
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References:
[1] 'Wave Production in a Thick Cylindrical Bar Due to Longitudinal Impact', by; Vales, et al., JSME Journal, Series A, Vol. 39, No.1 1996.
[2] 'Wave motion in a thick cylindrical rod undergoing longitudinal impact', by: Cerv, et al., Wave Motion 66 (2016), p.88-105.
[3] 'Impact: The Theory and Physical Behavior of Colliding Solids', by: Werner Goldsmith, Dover books (2001), p. 30-31, 43-44.
[4] 'Foundation Vibration Analysis Using Simple Physical Models', by: Wolf, Prentice Hall (1994), p.115-118.