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Open image in new window Fig. 5 Change rule of per revolution-specific rock-breaking work with the increase of radius of gyration.

Keeping the outer cone radius 30 mm unchanged, changes inner cone angle, and counts the change regulation of per revolution-specific rock-breaking work along with the increase of radius of gyration, as shown in Fig. 7.

Because it has the same change rule of per revolution-specific rock-breaking work with the increase of radius of gyration for different types of rocks, this paper takes the sandstone as an example.

The relatively small biexciton binding energy for the present QDs would be attributed to a large size of QDs, since an increase of radius of QDs reduces biexciton binding energy [19].

The greater the rock strength, the larger the work required to break per unit volume of rock at the same radius of gyration, also the steeper the changing trend of per revolution-specific rock-breaking work with the increase of radius of gyration.

Also take sandstone for example, keeps the inner cone angle 20° unchanged, changing outer cone arc radius, and counts the change regulation of per revolution-specific rock-breaking work along with the increase of radius of gyration, as shown in Fig. 8.

Also, the radiation losses decrease with increasing of radius of cylinder.

The threshold excitation energy (ωth) decreases in the increasing of radius.

On the other hand, output energy coefficient, which decreases with the increasing of radius ratio, achieves peak when force ratio (external load to blocked force of piezostack) is 0.5.

Results revealed that ratchet limit increases obviously with the increment of radius ratio.

For thin barrier, the critical dimensions decrease as the core radius increases, while when the barrier is thick enough, the critical dimensions show an increase with the increase of core radius conversely.