| V.6 No 4, pp 13 - 19 | 17 |
| The features of inclined force acting | |
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Actually, for each picked out region at the moment t0 |
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(22) |
where  xi
= xi - x0 . With it the denominator of (7) takes the
form |
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(23) |
Consequently, |
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(24) |
As we can see from (24), Gi
variation depends as on the parameters t0 and x0
determining the momentary time of Gi
investigation and location of the picked out region as on the wave delay phase when
transiting from the surface a0 to the surface ai. But
the wave delay has the time-dependent pattern, since, though the wave propagates in space,
its delay is caused by the finiteness of its propagation velocity, which makes it just
time-dependent. So we can transform |
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| where ti is the wave delay time when transiting along the
picked out region V0i . Then (10) takes the
form |
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(25) |
