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Worked solution: The planar case: every Kakeya set in $\mathbb{R}^2$ has dimension 2 (Davies, 1971)

Step 2 of 4: Reducing to a finite question about tubes
In plain words

Hausdorff dimension is defined by an infinite covering process, which is awkward to attack directly. The standard move is to discretize: thicken each unit segment of KK into a thin tube of width δ\delta, keep one tube per δ\delta-separated direction (about N∼1/δN \sim 1/\delta of them), and ask how small their union can be. If one can show this union always has area at least N2−o(1)δ2N^{2-o(1)}\delta^2 — nearly as large as if the NN tubes of area δ\delta each were completely disjoint — then letting δ→0\delta \to 0 forces KK itself to have Minkowski dimension 22, and with extra care, Hausdorff dimension 22 as well.

T={T1,…,TN},N∼δ−1,Ti: δ×1 tube,∣θi−θj∣≳∣i−j∣ δ\mathbb{T} = \{T_1,\dots,T_N\},\quad N \sim \delta^{-1},\quad T_i:\ \delta \times 1 \text{ tube},\quad |\theta_i - \theta_j| \gtrsim |i-j|\,\delta
Detailed analysis

Concretely, the equivalence used is: dim⁡M(K)=2  ⟺  \dim_M(K) = 2 \iff for every ε>0\varepsilon>0 there is δ0\delta_0 such that for all δ<δ0\delta<\delta_0, the δ\delta-neighborhood of KK has area ≥δε\ge \delta^{\varepsilon}; since KK contains a unit segment in each of the N∼δ−1N\sim\delta^{-1} directions, its δ\delta-neighborhood contains the union of the corresponding NN tubes T1,…,TNT_1,\dots,T_N (this is where the segment-version of the conjecture implies the tube-version). So it suffices to lower-bound ∣⋃iTi∣|\bigcup_i T_i| by any power δo(1)\delta^{o(1)}, and the next two steps produce exactly δ−2/log⁡(1/δ)⋅δ2=1/log⁡(1/δ)\delta^{-2}/\log(1/\delta) \cdot \delta^2 = 1/\log(1/\delta), which indeed tends to 00 slower than any positive power of δ\delta.

Common mistake. Discreteness matters: the δ\delta-tube bound only controls Minkowski dimension directly. Getting the (a priori weaker, but here equal) Hausdorff dimension requires an extra argument across scales, which is part of what makes Davies' original 1971 paper — using projective duality and Marstrand-type projection theorems rather than the tube counting below — a genuinely different route to the same conclusion.