Understanding Classical Mechanics: Acceleration

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I'm reading once again through Landau-Lifchitz and I am stuck on the first page! I can't wrap my head around why we only need to define the coordinates and velocities to determine the acceleration? Surely if we only know those two in a single point in time, that's not enough to determine an acceleration? What am I missing here? Thanks!
 
From the equations of motion with given ##q## and ##\dot{q}## you get ##\ddot{q}##. Of course you need the assumption that the (generalized) force depends only on ##q## and ##\dot{q}## as usual in classical mechanics.
 
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