TAOCP 5.4.1 Exercise 13
Let $P$ be the number of keys held in the selection tree.
Section 5.4.1: Multiway Merging and Replacement Selection
Exercise 13. [13] [13] Why is the second run produced by replacement selection usually longer than the first run?
Verified: yes
Solve time: 1m13s
Solution
Let $P$ be the number of keys held in the selection tree.
Replacement selection produces a run by repeatedly outputting the smallest key among the active keys in the tree and replacing it by the next input record. If the new key is smaller than the last output key, it is marked for the next run and becomes inactive for the current run.
The length of a run is governed by how long the system maintains $P$ active keys. A run ends when all remaining keys in memory are frozen, so no active key remains available for selection.
During the first run, the system starts from an empty history. All $P$ memory locations are filled directly from the input, and none of the keys has been constrained by previous comparisons against a prior output threshold. The first time a replacement introduces a key smaller than the current output, that key is immediately frozen into the next run. Since the input is effectively unconstrained at this stage, many replacements generate such frozen keys early, reducing the number of active keys more rapidly than in a balanced situation. This causes the active set to deplete sooner, so the first run terminates before the system reaches a stable configuration.
After the first run completes, the memory is no longer in an unconstrained state. The surviving structure consists of keys that have already been filtered by the condition imposed during the first run, namely that they were not smaller than the output threshold at the time they were inserted. This introduces a bias: the distribution of keys in memory is no longer arbitrary with respect to the current output level, and many of the smallest early candidates have already been moved into earlier positions of the first run.
At the start of the second run, the system therefore begins closer to the steady regime described by Moore’s snowplow model, in which the number of active elements fluctuates around a stable level of $P$. Fewer replacements immediately violate the current run condition, so fewer keys are prematurely frozen. The active set is therefore maintained for a longer sequence of outputs before exhaustion occurs.
Since the first run starts far from this steady state and loses active capacity quickly, while the second run begins in a partially stabilized configuration in which the rate of freezing is lower, the second run is usually longer than the first run. This difference is a transient effect due to the initial imbalance in the selection tree, and it diminishes as successive runs approach the steady-state behavior in which typical run length is about $2P$. ∎