Gregory Galperin (EIU) Billiard bouncing in gravitational field Abstract: There is a collection of semi-circles of diameter 1 in the upper half plane centered at the integer points (n, 0) on the x-axis. A released billiard ball falls down under the vertical constant gravitational force g. The ball bounces off the semi-circles according to the billiard law and describes a tra jectory γ . Record the indices of the semi-circles the ball hits as a sequence ω = (ω1 , ω2 , ...), which we call the one-sided itinerary of the tra jectory γ . What one-sided itineraries are realizable, if one can change (a) the initial height of the bal l; (b) both the initial height and the initial velocity of the bal l? For example, can the following itinerary ω = (ω1 , ω2 , ...) be realized by some billiard tra jectory γ ? Draw the digits of π = 3.14159265... on an one-sided infinite strip and cut this strip into pieces of positive integers, each of which has an arbitrary length not exceeding one billion. Reversing time, we can also consider billiard tra jectories in the gravitational field g with two-sided itineraries. What two-sided itineraries are realizable? For example, can the following two-sided itinerary ω = (..., ω −2 , ω−1 , ω0 , ω1 , ω2 , ...) be realized by some billiard tra jectory γ ? Draw the digits of π = 3.14159265... in the forward direction and the digits of e = 2.718281828... in the backward direction on an infinite two-sided strip and cut this strip into pieces of positive integers, each of which has an arbitrary length not exceeding one billion. The speaker will describe the sets of all realizable one- and two-sided itineraries of billiard tra jectories. |
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