Simplifying assumptions:
Case 1: (quite non physical): the gravitational field is at S surface value to 1 S radius. What is the necessary launch velocity (V1) needed to reach just that altitude with 0 velocity upon reaching there.
Case 2: the gravitational field follows normal physics and declines on an inverse square basis measured in S radii. What is the necessary launch velocity (V2) needed so that the test particle's velocity is asymptotic to 0 (that is, never 0, but its limit is 0).
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∫ r 2 1 d r ⟹ − r 1 . ∫ 1 ∞ r 2 1 d r ⟹ 1 . The velocities are equal.