Overhang Mike Paterson Uri Zwick The overhang problem How far off the edge of the table can we reach by stacking n identical blocks of length 1? J.G. Coffin – Problem 3009, American Mathematical Monthly (1923). “Real-life” 3D version Idealized 2D version The classical solution Using n blocks we can get an overhang of Harmonic Stacks Is the classical solution optimal? Obviously not! Inverted pyramids? Inverted pyramids? Unstable! Diamonds? The 4-diamond is stable Diamonds? The 5-diamond is … Diamonds? The 5-diamond is unstable! What really happens? What really happens! Why is this unstable? … and this stable? Equilibrium F1 F2 F4 F3 F1 + F2 + F3 = F4 + F5 x1 F1+ x2 F2+ x3 F3 = x4 F4+ x5 F5 F5 Force equation Moment equation Forces between blocks Assumption: No friction. All forces are vertical. Equivalent sets of forces Stability Definition: A stack of blocks is stable iff there is an admissible set of forces under which each block is in equilibrium. 1 1 3 Checking stability Checking stability F2 F1 F3 F4 F5 F11 F7 F8 F9 F10 F13 F14 F15 F16 F6 F12 Equivalent to the feasibility of a set of linear inequalities: F17 F18 Stability and Collapse A feasible solution of the primal system gives a set of stabilizing forces. A feasible solution of the dual system describes an infinitesimal motion that decreases the potential energy. Small optimal stacks Blocks = 4 Overhang = 1.16789 Blocks = 5 Overhang = 1.30455 Blocks = 6 Overhang = 1.4367 Blocks = 7 Overhang = 1.53005 Small optimal stacks Blocks = 16 Overhang = 2.14384 Blocks = 17 Overhang = 2.1909 Blocks = 18 Overhang = 2.23457 Blocks = 19 Overhang = 2.27713 Support and balancing blocks Balancing set Principal block Support set Support and balancing blocks Balancing set Principal block Support set Loaded stacks Stacks with downward external forces acting on them Size = Principal block number of blocks + sum of external forces. Support set Spinal stacks Stacks in which the support set contains only one block at each level Principal block Support set Loaded vs. standard stacks 1 1 Loaded stacks are slightly more powerful. Conjecture: The difference is bounded by a constant. Optimal spinal stacks Optimality condition: Spinal overhang Let S (n) be the maximal overhang achievable using a spinal stack with n blocks. Let S*(n) be the maximal overhang achievable using a loaded spinal stack of total weight n. Theorem: Conjecture: A factor of 2 improvement over harmonic stacks! 100 blocks example Towers Shadow Spine Are spinal stacks optimal? No! Support set is not spinal! Blocks = 20 Overhang = 2.32014 Optimal weight 100 construction Weight = 100 Blocks = 47 Overhang = 4.20801 Brick-wall constructions Brick-wall constructions Brick-wall constructions “Parabolic” constructions 5-stack Number of blocks: Stable! Overhang: Using n blocks we can get an overhang of (n1/3) !!! An exponential improvement over the O(log n) overhang of spinal stacks !!! “Parabolic” constructions 5-slab 4-slab 3-slab r-slab 5-slab r-slab 5-slab r-slab 5-slab “Vases” Weight = 1151.76 Blocks = 1043 Overhang = 10 “Vases” Weight = 115467. Blocks = 112421 Overhang = 50 “Oil lamps” Weight = 1112.84 Blocks = 921 Overhang = 10 Open problems ● Is the (n1/3) construction tight? Yes! Shown recently by Paterson-Peres-Thorup-Winkler-Zwick ● What is the asymptotic shape of “vases”? ● What is the asymptotic shape of “oil lamps”? ● ● What is the gap between brick-wall constructions and general constructions? What is the gap between loaded stacks and standard stacks?
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