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Next,, are intervals to second zero crossing and to the maximum in the contact phase, respectively.
Therefore has just one positive local maximum between its first zero and second zero.
Therefore has just one negative minimum between its second zero and third zero.
Therefore there are and satisfying (2.26) and, by Lemma 2.6, either fulfils (2.21) or has the second zero with.
Then, by Lemma 2.6, either fulfils (2.21) or has its second zero and, arguing as in Steps 2 5 of the proof of Theorem 3.3, we deduce that is a damped solution.
According to the proof of Theorem 3.3, we see that if is oscillatory, it has just one positive local maximum between the first and the second zero, then just one negative local minimum between the second and the third zero, and so on.
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