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Add gravity computational overhead card
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docs/walter-bishop.html

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font-weight: 700;
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}
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.big-card {
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margin-top: 28px;
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padding: 28px;
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border: 2px solid var(--gold);
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border-radius: 16px;
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background: linear-gradient(135deg, #fff8e7 0%, #ffffff 100%);
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box-shadow: 0 14px 30px rgba(20, 32, 27, 0.08);
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}
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.big-card .tag {
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margin-bottom: 14px;
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}
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.big-card h2 {
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margin-top: 0;
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border-bottom: none;
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font-size: 31px;
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}
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font-size: 18px;
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}
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.big-card .punchline {
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max-width: 920px;
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margin-top: 18px;
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font-size: 24px;
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font-weight: 800;
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line-height: 1.25;
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}
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.grid {
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display: grid;
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grid-template-columns: repeat(2, minmax(0, 1fr));
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.grid {
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grid-template-columns: 1fr;
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}
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.big-card {
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padding: 22px;
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}
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.big-card h2 {
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font-size: 26px;
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font-size: 21px;
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}
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}
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</style>
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</head>
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fact.
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</p>
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<section class="big-card" aria-label="Gravity as computational overhead">
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<span class="tag">For example</span>
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<h2>Gravity as computational overhead</h2>
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<p class="punchline">
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Gravity as an effect, or gravity as a force — either way you look at it,
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it is a computational overhead issue.
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</p>
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<p>
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In this interpretation, gravity is not first pictured as a marble being
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pulled through a spatial background. It is treated as the visible cost of
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maintaining global/local consistency: update delay, constraint propagation,
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bookkeeping pressure, and loop-rate skew inside the information process
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that renders distance, inertia, and apparent curvature.
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</p>
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<p>
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That does not prove a theory of gravity. It states the research posture:
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when a physical effect looks like force, curvature, delay, or resistance,
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ask what computational overhead the coupled system is paying to keep the
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event admissible.
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</p>
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</section>
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<h2>The Walter Bishop Version</h2>
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<div class="grid">
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<article class="card">
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</footer>
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</main>
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</body>
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</html>
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</html>

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