Maximu m Overha ng Mike Paterson Yuval Peres

  • Slides: 57
Download presentation
Maximu m Overha ng Mike Paterson Yuval Peres Mikkel Thorup Peter Winkler Uri Zwick

Maximu m Overha ng Mike Paterson Yuval Peres Mikkel Thorup Peter Winkler Uri Zwick

The overhang problem How far off the edge of the table can we reach

The overhang problem How far off the edge of the table can we reach by stacking n identical blocks of length 1? J. B. Phear – Elementary Mechanics (1850) J. G. Coffin – Problem 3009, American Mathematical Monthly (1923). No friction Length parallel to table “Real-life” 3 D version Idealized 2 D version

The classical solution Using n blocks we can get an overhang of Harmonic Stacks

The classical solution Using n blocks we can get an overhang of Harmonic Stacks

Is the classical solution optimal? Obviously not!

Is the classical solution optimal? Obviously not!

Inverted triangles? Balanced?

Inverted triangles? Balanced?

Inverted triangles? Balanced?

Inverted triangles? Balanced?

Inverted triangles? Unbalanced!

Inverted triangles? Unbalanced!

Diamonds? The 4 -diamond is balanced

Diamonds? The 4 -diamond is balanced

Diamonds? The 5 -diamond is …

Diamonds? The 5 -diamond is …

Diamonds? The 5 -diamond is Unbalanced!

Diamonds? The 5 -diamond is Unbalanced!

What really happens?

What really happens?

What really happens!

What really happens!

Why is this unbalanced?

Why is this unbalanced?

… and this balanced?

… and this balanced?

Equilibrium F 1 F 2 F 4 F 3 F 1 + F 2

Equilibrium F 1 F 2 F 4 F 3 F 1 + F 2 + F 3 = F 4 + F 5 x 1 F 1+ x 2 F 2+ x 3 F 3 = x 4 F 4+ x 5 F 5 Force equation Moment equation

Forces between blocks Assumption: No friction. All forces are vertical. Equivalent sets of forces

Forces between blocks Assumption: No friction. All forces are vertical. Equivalent sets of forces

Balance Definition: A stack of blocks is balanced iff there is an admissible set

Balance Definition: A stack of blocks is balanced iff there is an admissible set of forces under which each block is in equilibrium. 1 1 3

Checking balance

Checking balance

Checking balance F 2 F 1 F 3 F 4 F 5 F 11

Checking balance F 2 F 1 F 3 F 4 F 5 F 11 F 7 F 8 F 9 F 10 F 13 F 14 F 15 F 16 F 12 Equivalent to the feasibility of a set of linear inequalities: F 17 F 18 Static indeterminacy: balancing forces, if they exist, are usually not unique!

Balance, Stability and Collapse Most of the stacks considered are precariously balanced, i. e.

Balance, Stability and Collapse Most of the stacks considered are precariously balanced, i. e. , they are in an unstable equilibrium. In most cases the stacks can be made stable by small modifications. The way unbalanced stacks collapse can be determined in polynomial time

Small optimal stacks Blocks = 4 Overhang = 1. 16789 Blocks = 5 Overhang

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

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

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

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

Spinal stacks Stacks in which the support set contains only one block at each level Principal block Support set Assumed to be optimal in: J. F. Hall, Fun with stacking Blocks, American Journal of Physics 73(12), 1107 -1116, 2005.

Loaded vs. standard stacks Loaded stacks are slightly more powerful. Conjecture: The difference is

Loaded vs. standard stacks Loaded stacks are slightly more powerful. Conjecture: The difference is bounded by a constant.

… Optimal spinal stacks Optimality condition:

… Optimal spinal stacks Optimality condition:

Spinal overhang Let S (n) be the maximal overhang achievable using a spinal stack

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 on total weight n. Theorem: Conjecture: A factor of 2 improvement over harmonic stacks!

Optimal 100 -block spinal stack Towers Shield Spine

Optimal 100 -block spinal stack Towers Shield Spine

Optimal weight 100 loaded spinal stack

Optimal weight 100 loaded spinal stack

Loaded spinal stack + shield

Loaded spinal stack + shield

spinal stack + shield + towers

spinal stack + shield + towers

Are spinal stacks optimal? No! Support set is not spinal! Blocks = 20 Overhang

Are spinal stacks optimal? No! Support set is not spinal! Blocks = 20 Overhang = 2. 32014 Tiny gap

Optimal 30 -block stack Blocks = 30 Overhang = 2. 70909

Optimal 30 -block stack Blocks = 30 Overhang = 2. 70909

Optimal (? ) weight 100 construction Weight = 100 Blocks = 49 Overhang =

Optimal (? ) weight 100 construction Weight = 100 Blocks = 49 Overhang = 4. 2390

Brick-wall constructions

Brick-wall constructions

Brick-wall constructions

Brick-wall constructions

“Parabolic” constructions 6 -stack Number of blocks: Balanced! Overhang:

“Parabolic” constructions 6 -stack Number of blocks: Balanced! Overhang:

Using n blocks we can get an overhang of (n 1/3) !!! An exponential

Using n blocks we can get an overhang of (n 1/3) !!! An exponential improvement over the O(log n) overhang of spinal stacks !!!

“Parabolic” constructions 6 -slab 5 -slab 4 -slab

“Parabolic” constructions 6 -slab 5 -slab 4 -slab

r-slab

r-slab

r-slab within a (r+1)-slab

r-slab within a (r+1)-slab

“Vases” Weight = 1151. 76 Blocks = 1043 Overhang = 10

“Vases” Weight = 1151. 76 Blocks = 1043 Overhang = 10

“Vases” Weight = 115467. Blocks = 112421 Overhang = 50

“Vases” Weight = 115467. Blocks = 112421 Overhang = 50

Forces within “vases”

Forces within “vases”

Unloaded “vases”

Unloaded “vases”

“Oil lamps” Weight = 1112. 84 Blocks = 921 Overhang = 10

“Oil lamps” Weight = 1112. 84 Blocks = 921 Overhang = 10

Forces within “oil lamps”

Forces within “oil lamps”

Brick-by-brick constructions

Brick-by-brick constructions

Is the Yes! 1/3 (n ) the final answer? Maximu m Overha ng Mike

Is the Yes! 1/3 (n ) the final answer? Maximu m Overha ng Mike Paterson Yuval Peres Mikkel Thorup Peter Winkler Uri Zwick

Splitting game Start with 1 at the origin How many splits are needed to

Splitting game Start with 1 at the origin How many splits are needed to get, say, a quarter of the mass to distance n? At each step, split the mass in a given position between the two adjacent positions 1 -3 -2 -1 0 1 2 3

Skintling

Skintling

Slanting pyramids

Slanting pyramids

Concluding remarks and Open problems ● Is the 3 D problem solved? ● What

Concluding remarks and Open problems ● Is the 3 D problem solved? ● What is the effect of friction? ● What is the asymptotic shape of “vases”? ● What is the asymptotic shape of “oil lamps”? ● ● What is the gap between brick-wall stacks and general stacks? What is the gap between loaded stacks and standard stacks?