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Mike Paterson Overhang Academic Sponsors’ Day, MSRI, March 2, 2012 Peter Winkler Uri Zwick Yuval Peres Mikkel Thorup

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Academic Sponsors’ Day, MSRI, March 2, 2012. Overhang. Uri Zwick. Peter Winkler. Mikkel Thorup. Yuval Peres. Mike Paterson. A Crow Problem:. How long does it take to drive off the crow?. n. -n. -2. -1. 0. 1. 2. Simple random walk: about n 2 throws. - PowerPoint PPT Presentation

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Page 1: Mike Paterson

Mike Paterson

Overhang

Academic Sponsors’ Day, MSRI, March 2, 2012

Peter WinklerUri Zwick

Yuval PeresMikkel Thorup

Page 2: Mike Paterson

A Crow Problem:

Page 3: Mike Paterson

How long does it take to drive off the crow?

-n 0 1-1-2 2 n

Simple random walk: about n2 throws.

One way to see that: consider the probability distribution of crow’s location; its variance

goes up by 1 after each throw.

Page 4: Mike Paterson

A new problem, brought to MSRI in spring ’05

by Zwick: the crow comes back…

Page 5: Mike Paterson

…at night!Now what---your first stone will hit the crow and dislodge him, but after that

you’re increasingly unsure where he is.

You can certainly get him off the wallin order n3 throws, and you certainly

still need at least n2 . Which is the truth?

Page 6: Mike Paterson

Theorem: Order n3 throws are necessary.

Proof: Uses two different potential functions, each for the wrong problem.

An unusual case of two wrongs making a right.

-n 0 n

Page 7: Mike Paterson

The overhang problemHow far off the edge of the table

can we reach by stacking n identical blocks of length 1?

“Real-life” 3D version

Idealized 2D version

Page 8: Mike Paterson

Back in time with the overhang problem…

John F. Hall, Fun with Stacking Blocks, Am. J. Physics December 2005.Martin Gardner - Scientific American’s “Mathematical Games” column, 1969.

J.G. Coffin – Problem 3009, American Mathematical Monthly, 1923. George M. Minchin, A Treatise on Statics with Applications to Physics, 6th ed. (Clarendon, Oxford, 1907), Vol. 1, p. 341.

William Walton, A Collection of Problems in Illustration of the Principles of Theoretical Mechanics 2nd ed. (Deighton, Bell, Cambridge, 1855), p. 183.

J.B. Phear, Elementary Mechanics (MacMillan, Cambridge, 1850), pp. 140–141.

Page 9: Mike Paterson

The classical solution

“Harmonic Stack”

Using n bricks we can get an overhang

of

Page 10: Mike Paterson

Is the classical solution optimal?

Apparently not. How can we improve the construction?

Page 11: Mike Paterson

Inverted pyramids?

Claimed to be stable in Mad About Physics, by Chris Jargodzki and Franklin Potter,

but…

Page 12: Mike Paterson

They are unbalanced, when the number of layers exceeds 2.

Page 13: Mike Paterson

Diamonds?

The 4-diamond is balanced…

Page 14: Mike Paterson

But the 5-diamond is …

Page 15: Mike Paterson

not.

Page 16: Mike Paterson

What really happens?

Page 17: Mike Paterson

What really happens!

Page 18: Mike Paterson

Why is this unbalanced?

Page 19: Mike Paterson

… and this balanced?

Page 20: Mike Paterson

Equilibrium

F1 + F2 + F3 = F4 + F5

x1 F1+ x2 F2+ x3 F3 = x4 F4+ x5 F5

Force equationMoment equation

F1

F5F4

F3

F2

Page 21: Mike Paterson

Forces between bricksAssumption: No

friction.All forces are vertical.

Equivalent sets of forces

Page 22: Mike Paterson

Balanced StacksDefinition: A stack of bricks is balanced iff there is an admissible set of forces under which each brick is in equilibrium.

1 1

3

Page 23: Mike Paterson

How can we tell if a stack is balanced?

Page 24: Mike Paterson

Checking for balance

F1 F2 F3 F4 F5 F6

F7 F8 F9 F10 F11 F12

F13 F14 F15 F16

F17 F18

Equivalent to the feasibilityof a set of linear

inequalities:

Page 25: Mike Paterson

Stability and Collapse

A feasible solution of the primal system gives a set of balancing

forces.A feasible solution of the dual

system describes an infinitesimal motion that decreases the potential

energy.

Page 26: Mike Paterson

Small optimal stacks

Overhang = 1.16789Bricks = 4

Overhang = 1.30455Bricks = 5

Overhang = 1.4367Bricks = 6

Overhang = 1.53005Bricks = 7

Page 27: Mike Paterson

Small optimal stacks

Page 28: Mike Paterson

Small optimal stacks

Page 29: Mike Paterson

Small optimal stacks

Overhang = 2.14384Bricks = 16

Overhang = 2.1909Bricks = 17

Overhang = 2.23457Bricks = 18

Overhang = 2.27713Bricks = 19

Page 30: Mike Paterson

Support and counterweight bricks

Support

set

Counter-weights

These examples are “spinal”: support stack has only one brick per level, so overhang increases

with height.Spinal stacks can achieve overhang S(n) ~ log n.

Page 31: Mike Paterson

100 bricks example

Page 32: Mike Paterson

But are spinal stacks optimal?No! When # bricks reaches 20 . . .

Support set is not spinal.

Overhang = 2.32014, slightly exceeding S(20).

Page 33: Mike Paterson

Optimal weight 100 construction

Overhang = 4.20801

Bricks = 47Weight = 100

Page 34: Mike Paterson

Brick-wall constructions

Page 35: Mike Paterson

Brick-wall constructions

Page 36: Mike Paterson

“Parabolic” construction

5-stack

Number of bricks: Overhang:Stable!

Page 37: Mike Paterson

Thus: n bricks can achieve an overhang of order n1/3 ...

an exponential improvement over the order log n overhang

of spinal stacks.

Page 38: Mike Paterson

Mayan from 900 BC---no keystone

Page 39: Mike Paterson

Yes! Argument is based on the idea that laying bricks is like stoning crows.

Each additional brick…

spreads forces the same way that throwing a stone (at night) spreads the crow’s probability

bar.

The Upper BoundIs order n1/3 best possible??

Page 40: Mike Paterson

In particular, a stack of only n bricks cannot overhang by more than 6n1/3 brick

lengths. The parabolic construction gives overhang (3/16)1/3 n1/3 ~ .572357121 n1/3, so we have the order right but the constant is off by an

order of magnitude. Simulations suggest that the constant

can be improved by adjusting the shape of the brick wall construction…

A generalized version of the “stoning crows” analysis shows that it takes order n3 bricks to

get the stack to lean out by n .

Page 41: Mike Paterson

“Vases”

Weight = 1151.76

Bricks = 1043

Overhang = 10

Page 42: Mike Paterson

“Vases”

Weight = 115467.

Bricks = 112421

Overhang = 50

Page 43: Mike Paterson

“Oil lamps”

Weight = 1112.84

Bricks = 921

Overhang = 10

giving overhang of about 1.02 n1/3 .

Page 44: Mike Paterson

How about using the third dimension?Our upper bound proof makes no use of the fact

that bricks cannot overlap in space! Hence, the 6n1/3 bound applies even in 3D, as long as there are no non-vertical forces.

However, the constant can be improved in space by skintling,

Effectively increasing the brick length to (1+w)1/2 .

Page 45: Mike Paterson

Open problems● What is the correct constant in the maximum

overhang, in the rectilinear case? In the general 3-dimensional case?

● What is the asymptotic shape of “vases”?● What is the asymptotic shape of “oil lamps”?● What is the gap between brick-wall

constructionsand general constructions?

● Can the proof be extended to cover non-vertical forces (if, indeed, they are possible for 3D bricks)?

● How much friction is needed to change the 1/3 exponent for overhang?

Page 46: Mike Paterson

Thank you for your attention. Happy stacking…