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</div>
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<main itemscope itemtype="https://schema.org/LearningResource https://schema.org/MathSolver" id="cgs">
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<meta itemprop="name" content="Core Geometric System ™">
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<meta itemprop="dateModified" content="2026-09-08T18:43:29+02:00">
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<meta itemprop="dateModified" content="2026-09-08T19:36:29+02:00">
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<meta itemprop="accessMode" content="mathOnVisual">
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<meta itemprop="accessMode" content="textual">
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<meta itemprop="accessMode" content="visual">
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<li>"a line is a set of points, therefore, it has no thickness"</li>
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</ul>
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<p itemprop="articleBody">Note that in these terms, even if the dimensions of the point are defined as 0, the thickness of the line is logically one point.
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<p itemprop="articleBody">Note that under these premises, even if an abstract point is assigned a dimension of zero, any realized or constructed line must possess an operational width of at least one constituent spatial unit.
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<br><br>
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The tangent point T and its two adjacent points T₋₁ and T₊₁ form a 3‑point long section on the tangent line.
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<br><br>
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In reality, as the side count increases in a regular polygon, the central angle subtended by a single side drops significantly — it approaches 0°.
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For any large circle, the central angle subtended by three adjacent spatial points is an infinitesimal fraction of a degree.
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<br>
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At very small angles, the sagitta collapses toward zero — billions of times smaller than the 1‑point threshold required to keep the arc and the tangent line apart.</p>
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For any macro-scale circle, the central angle subtended by three contiguous spatial units is an infinitesimal fraction of a degree. At these microscopic angles, the sagitta collapses quadratically toward zero — falling orders of magnitude below the single-unit threshold required to maintain physical separation between the arc and the tangent line.</p>
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<br>
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<figure itemprop="image" class="imgbox" itemscope itemtype="https://schema.org/ImageObject">
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<img class="center-fit" src="arcAndLine.png" alt="Once the sagitta drops below the fundamental grid threshold required to separate the arc from the straight line, single-point tangency ceases to exist. The arc and the tangent line physically and logically coincide across that entire interval.">
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<br>
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But it becomes a critical error at a higher side count and smaller angles. When the protruding area shrinks below the area where the side and the arc overlap, the triangle stops fully "containing" the slice, and the comparison becomes invalid.
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<br><br>
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The flaw in the classical method becomes even clearer when we try to implement it practically.
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<br>
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The breakdown is visible already at a small finite side count when attempting to draw a circumscribed 24-gon or 48-gon via exact angle bisection (central angle 15° → 7.5°).
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This breakdown becomes structurally evident at surprisingly modest side counts. When attempting to construct or model a circumscribed 24-gon with central angles of 15°, the required vertex clearance approaches spatial insignificance.
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The figure collapses:</p>
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<br>
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This is not a precision error, nor only a rendering limitation. It is the geometry refusing to produce a valid set of external tangents.
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<br><br>
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Classical limits assume infinite resolution to avoid this collapse.
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Classical limits assume infinite resolution to avoid this collapse. Classical geometry insists on maintaining a physical gap by declaring the tiny separation distance to be the "new minimum unit," but that comes with an inevitable consequence: the original tangent point itself morphs into a segment composed of several of these new minimum units. The result is the same:
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Classical geometry insists on maintaining a physical gap by declaring the tiny separation distance to be the "new minimum unit," but that comes with an inevitable consequence: the original tangent point itself morphs into a segment composed of several of these new minimum units. The result is the same:
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Either path leads to the same inescapable conclusion: <strong>Classical tangency is not physically or logically realizable under its own axioms.</strong> Single-point contact is a mathematical abstraction. In reality, as the angle shrinks, the curve flattens relative to the line, creating a multi-point span of coincidence/overlap.
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The boundary is no longer touching at an isolated 0‑dimensional point T; it shares an entire multi-point interval with the arc.
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This is the logical loophole at the foundation of Archimedes' method.
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The boundary is not touching at an isolated 0‑dimensional point T; it shares an entire multi-point interval with the arc. The polygon's side and the arc are forced into a multi‑point coincidence.
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Either path leads to the same inescapable conclusion: <strong>classical tangency is not physically or logically realizable under its own axioms.</strong> The polygon's side and the arc are forced into a multi‑point coincidence.
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<br>
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Archimedean pi bounds rely on taking the side count to infinity — which explicitly forces the central angle of each section approaching 0°.
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As the side count approaches infinity and the central angles approach 0°, the lack of the idealized single‑point tangency invalidates the circumscribed boundary that classical pi derivations rely upon.

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