Block-stacking problem
In statics, the block-stacking problem (sometimes known as The Leaning Tower of Lire (Johnson 1955), also the book-stacking problem, or a number of other similar terms) is a puzzle concerning the stacking of blocks at the edge of a table.
The block-stacking problem is the following puzzle: Place
identical rigid rectangular blocks in a stable stack on a table edge in such a way as to maximize the overhang.
Paterson et al. (2007) provide a long list of references on this problem going back to mechanics texts from the middle of the 19th century.
The single-wide problem involves having only one block at any given level.
In the ideal case of perfectly rectangular blocks, the solution to the single-wide problem is that the maximum overhang is given by
times the width of a block.
This sum is one half of the corresponding partial sum of the harmonic series.
Because the harmonic series diverges, the maximal overhang tends to infinity as
increases, meaning that it is possible to achieve any arbitrarily large overhang, with sufficient blocks.
The number of blocks required to reach at least
block-lengths past the edge of the table is 4, 31, 227, 1674, 12367, 91380, ... (sequence A014537 in the OEIS).
[1] Multi-wide stacks using counterbalancing can give larger overhangs than a single width stack.
Even for three blocks, stacking two counterbalanced blocks on top of another block can give an overhang of 1, while the overhang in the simple ideal case is at most 11/12.
As Paterson et al. (2007) showed, asymptotically, the maximum overhang that can be achieved by multi-wide stacks is proportional to the cube root of the number of blocks, in contrast to the single-wide case in which the overhang is proportional to the logarithm of the number of blocks.
However, it has been shown that in reality this is impossible and the number of blocks that we can move to the right, due to block stress, is not more than a specified number.
For example, for a special brick with h = 0.20 m, Young's modulus E = 3000 MPa and density ρ = 1.8×103 kg/m3 and limiting compressive stress 3 MPa, the approximate value of N will be 853 and the maximum tower height becomes 170 m.[2] The above formula for the maximum overhang of
blocks, each with length
, stacked one at a level, can be proven by induction by considering the torques on the blocks about the edge of the table they overhang.
The blocks can be modelled as point-masses located at the center of each block, assuming uniform mass-density.
), the center of mass of the block lies above the table's edge, meaning an overhang of
blocks, the center of mass of the
-block system must lie above the table's edge, and the center of mass of the
top blocks must lie above the edge of the first for static equilibrium.
th block overhangs the
denotes the gravitational field.
top blocks overhang their center of mass by
, then, by assuming the inductive hypothesis, the maximum overhang off the table is
top blocks overhang their center of mass
Hall (2005) discusses this problem, shows that it is robust to nonidealizations such as rounded block corners and finite precision of block placing, and introduces several variants including nonzero friction forces between adjacent blocks.
