Conspiranon

description, blogger‑ready means: No LaTeX, no MathJax, no markdown math (so no $$, no , no backticks, no code blocks) All equations must be in plain Unicode or HTML, like: ∂²ₜΨ − v²∇²Ψ + μΨ + λ|Ψ|²Ψ = κSΨ Formatting must be valid Blogger HTML, using only tags Blogger accepts:

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No markdown, no unsupported embeds The output should look like an actual Blogger post, similar to the example you pasted, including: Title as an <h3> with a link Centered video embed Paragraphs in <p> tags Bolded section headers inside HTML, not markdown Inline math in Unicode or HTML entities On the Limiting Behavior of Curvature in Gravitational Collapse 1. Introduction In classical general relativity, sufficiently concentrated mass–energy leads, under broad and physically reasonable conditions, to spacetime singularities. The singularity theorems of Stephen Hawking and Roger Penrose demonstrate that gravitational collapse generically produces geodesic incompleteness, provided certain energy conditions and causal assumptions hold. It is essential, however, to state precisely what these theorems establish. They do not prove the existence of a physical object of infinite density. Rather, they show that the spacetime manifold cannot be extended in a smooth manner along incomplete geodesics. The conclusion is mathematical incompleteness, not the verified existence of physical infinities. In classical solutions describing collapse to a black hole, curvature invariants such as 𝑅 𝜇 𝜈 𝜌 𝜎 𝑅 𝜇 𝜈 𝜌 𝜎 R μνρσ  R μνρσ diverge along incomplete timelike or null geodesics. The divergence signals that the classical field equations are being extrapolated into a regime where their applicability is uncertain. The singularity is therefore best understood as the boundary of classical spacetime geometry. 2. Classical Prediction and Its Domain The Einstein field equations, 𝐺 𝜇 𝜈 = 8 𝜋 𝐺   𝑇 𝜇 𝜈 , G μν  =8πGT μν  , relate spacetime curvature to stress–energy. In weak gravitational fields, they have been confirmed to high precision. In strong but non-singular regimes—such as near the event horizon of a black hole—they remain internally consistent and observationally supported. The exterior solution for a static, uncharged black hole is given by the Schwarzschild metric. This solution remains well-behaved at the event horizon. The divergence appears only in the deep interior, where curvature invariants grow without bound as the classical solution is extended. Nothing in the structure of the classical equations themselves prevents such divergence. The field equations are local differential relations; they do not contain an intrinsic upper bound on invariant magnitudes. Consequently, continued compression of matter leads formally to arbitrarily large curvature. However, the extrapolation of any classical field theory beyond its experimentally tested regime requires caution. Classical general relativity is a macroscopic theory. It does not incorporate quantum fluctuations of geometry. 3. The Planck Scale and Dimensional Considerations Dimensional analysis already identifies a natural scale at which classical gravity must break down. The Planck length, ℓ 𝑃 = ℏ 𝐺 𝑐 3 , ℓ P  = c 3 ℏG   , defines the regime in which quantum gravitational effects become significant. Curvature invariants of order 𝑅 ∼ 1 ℓ 𝑃 2 R∼ ℓ P 2  1  correspond to energy densities approaching the Planck density. At such scales, one expects fluctuations of spacetime itself to become dynamically important. Thus, independently of detailed models of quantum gravity, there are strong theoretical grounds for expecting that arbitrarily large curvature is not physically realized. Rather, classical geometry becomes incomplete at Planckian scales. 4. Nonlinear Field Dynamics as Illustration It is instructive to consider how nonlinear self-interaction can regulate growth in relativistic field theory without modifying verified weak-field behavior. Consider schematically a scalar degree of freedom 𝑆 S coupled to a matter field Ψ Ψ: □ 𝑆 + 𝛽 𝑆 3 = 𝜎 ( 𝑥 ) 𝐹 [ Ψ ] , □S+βS 3 =σ(x)F[Ψ], □ Ψ + 𝜇 Ψ + 𝜆 ∣ Ψ ∣ 2 Ψ = 𝜅 𝑆 Ψ . □Ψ+μΨ+λ∣Ψ∣ 2 Ψ=κSΨ. Here: □ ≡ ∂ 𝑡 2 − 𝑐 2 ∇ 2 □≡∂ t 2  −c 2 ∇ 2 is the d’Alembertian, 𝛽 , 𝜇 , 𝜆 , 𝜅 β,μ,λ,κ are coupling constants, 𝐹 [ Ψ ] F[Ψ] is a functional source term. This system is not proposed as a replacement for the Einstein equations. It serves as a schematic illustration of a general principle familiar from nonlinear field theory. For small amplitudes, the cubic terms are negligible. The system reduces to linear relativistic propagation, preserving established weak-field behavior. For large amplitudes, the nonlinear terms dominate. The effective restoring force grows faster than linearly, and the associated energy functional contains quartic contributions of the form ∼ 𝛽 𝑆 4 ∼βS 4 . For 𝛽 > 0 β>0, the energy is bounded below. Finite initial data do not evolve to infinite amplitude. Growth is resisted by nonlinear stiffness. The qualitative lesson is simple: nonlinear dynamics generically replace runaway divergence with saturation or asymptotic limiting behavior. 5. Application to Gravitational Collapse In gravitational collapse, the classical solution predicts monotonic growth of curvature invariants in the interior region. However, once curvature approaches Planckian magnitude, the assumptions underlying classical relativity cease to be valid. Semiclassical gravity already demonstrates that quantum effects modify the classical picture. Particle creation in curved spacetime, vacuum polarization, and stress–energy renormalization introduce corrections near strong gravitational fields. These effects are central to Hawking radiation and the thermodynamic interpretation of black holes. It is therefore reasonable to expect that a full quantum theory of gravity introduces additional nonlinear dynamics at extreme curvature. Under this perspective: The exterior Schwarzschild geometry remains valid where curvature is small compared with Planckian values. The event horizon remains a global causal boundary. The interior evolution approaches a regime in which classical spacetime ceases to be an adequate description. The divergence predicted by classical theory marks the limit of applicability of that theory. 6. On the Nature of Singularities A singularity in classical general relativity is defined by geodesic incompleteness. It is not a point within spacetime possessing infinite density in an operational sense. Infinite quantities are not physical observables. In theoretical physics, divergences typically indicate that a model has been extended beyond its regime of validity. Ultraviolet divergences in quantum field theory led to renormalization and, ultimately, to the recognition of new structure at short distances. Similarly, curvature divergences in classical general relativity signal that the continuum description of spacetime cannot be extrapolated arbitrarily far. The singularity is not a physical object. It is the boundary of classical geometry. 7. Conclusion Classical general relativity predicts unbounded curvature under continued gravitational collapse. The singularity theorems establish geodesic incompleteness, not the physical realization of infinite density. Dimensional analysis identifies the Planck scale as the regime where classical spacetime must fail. Semiclassical considerations already demonstrate that quantum effects modify gravitational dynamics in strong fields. Nonlinear field theory provides a generic mechanism by which growth may be regulated without altering well-tested weak-field predictions. It is therefore plausible that a complete theory of quantum gravity replaces classical divergence with finite, though extreme, curvature. In this interpretation, black holes do not contain infinite physical objects. They contain regions where classical spacetime ceases to provide a complete description. The singularity is not a thing within the universe. It is the limit of the classical scale. Nonlinear Saturation and the Limiting Behavior of Curvature 1. A Schematic Nonlinear Model To illustrate how divergence may be avoided without altering verified weak-field predictions, consider a coupled relativistic field system of the schematic form: ∂ 2 𝑆 ∂ 𝑡 2 − 𝑐 2 ∇ 2 𝑆 + 𝛽 𝑆 3 = 𝜎 ( 𝑥 , 𝑡 )   𝐹 [ Ψ ] , ∂t 2 ∂ 2 S  −c 2 ∇ 2 S+βS 3 =σ(x,t)F[Ψ], ∂ 2 Ψ ∂ 𝑡 2 − 𝑣 2 ∇ 2 Ψ + 𝜇 Ψ + 𝜆 ∣ Ψ ∣ 2 Ψ = 𝜅 𝑆 Ψ . ∂t 2 ∂ 2 Ψ  −v 2 ∇ 2 Ψ+μΨ+λ∣Ψ∣ 2 Ψ=κSΨ. Here: 𝑆 S denotes a scalar degree of freedom representing geometric response, Ψ Ψ denotes a matter or excitation field, 𝛽 , 𝜇 , 𝜆 , 𝜅 β,μ,λ,κ are coupling constants, 𝜎 ( 𝑥 , 𝑡 ) σ(x,t) modulates the source strength, 𝐹 [ Ψ ] F[Ψ] is a functional of the matter field. This system is not introduced as a modification of the Einstein field equations. It serves as an illustrative model demonstrating how nonlinear self-interaction can regulate amplitude growth while preserving linear behavior in the weak-field regime. 2. Nonlinear Stiffening The cubic term 𝛽 𝑆 3 βS 3 introduces nonlinear stiffness. For small amplitudes of 𝑆 S, the cubic term is negligible. The equation reduces to linear relativistic wave propagation, consistent with well-tested weak-field dynamics. However, as the amplitude increases, the cubic term becomes dominant. The effective restoring force grows faster than linearly. The associated energy functional contains a quartic contribution proportional to 𝛽 𝑆 4 βS 4 . For 𝛽 > 0 β>0, this contribution ensures that the energy is bounded below. Finite initial data do not evolve toward infinite amplitude. Instead, the nonlinear term increasingly resists growth. The field asymptotically approaches a limiting configuration. The essential point is that nonlinear self-interaction replaces runaway divergence with saturation, without disturbing the small-amplitude regime. 3. The Slide-Rule Analogy The classical field equations of general relativity may be compared to a slide rule. Within the engraved scale of the instrument, it produces accurate results. If one attempts to compute beyond its physical length, the scale simply ends. The mathematics of multiplication has not failed; the instrument has reached its limit. Similarly, the Einstein equations describe the growth of curvature under increasing stress–energy. Nothing within their classical structure imposes an intrinsic upper bound on curvature invariants. Continued extrapolation therefore yields divergence. However, divergence does not necessarily imply the physical realization of infinite quantities. It indicates that the classical description has been extended beyond its admissible domain. The appearance of infinite curvature may thus signal the limit of applicability of classical spacetime geometry. 4. Origin of the Limiting Scale Dimensional analysis identifies a natural scale at which classical gravity must fail: the Planck length, ℓ 𝑃 = ℏ 𝐺 𝑐 3 . ℓ P  = c 3 ℏG   . Curvature invariants approaching 𝑅 ∼ 1 ℓ 𝑃 2 R∼ ℓ P 2  1  correspond to Planckian energy densities. At such scales, quantum fluctuations of spacetime cannot be neglected. Independent theoretical considerations — including semiclassical gravity and quantum field theory in curved spacetime — strongly suggest that arbitrarily large curvature is unlikely to be physically realized. Instead, new dynamics are expected to intervene near the Planck scale. Nonlinear self-interaction provides a generic mathematical mechanism by which invariant growth may be regulated in that regime. The precise form of such regulation belongs to a complete theory of quantum gravity, but the expectation of limiting behavior follows from dimensional reasoning alone. 5. Reinterpretation of Singularities Under this perspective, the structure of black hole solutions may be reconsidered as follows: The Exterior. The Schwarzschild geometry remains valid where curvature is small compared with Planckian values. All observationally tested predictions remain intact. The Horizon. The event horizon remains a global causal boundary defined by classical geometry. Its existence does not depend on interior divergence. The Interior. As collapse proceeds and curvature approaches Planckian magnitude, classical general relativity ceases to be reliable. Rather than infinite curvature, one expects approach to a high-curvature regime governed by quantum gravitational dynamics. The classical singularity corresponds to geodesic incompleteness — not to a physical object of infinite density. It marks the boundary at which the classical manifold cannot be extended. Just as ultraviolet divergences in quantum field theory indicate the necessity of renormalization or new short-distance structure, curvature divergences indicate that classical spacetime is incomplete at extreme scales. 6. Conclusion Classical gravitational collapse predicts unbounded curvature only under the assumption that the Einstein equations remain valid arbitrarily far beyond their tested regime. There are strong theoretical reasons to expect otherwise. Dimensional analysis, semiclassical effects, and general properties of nonlinear field dynamics all suggest that invariant growth is regulated near the Planck scale. Black holes therefore need not contain infinite physical objects. They contain regions where classical spacetime ceases to provide a complete description. The equations do not fail in their proper domain. The divergence marks the end of the classical scale. <p><b>BLOGGER‑READY MODE</b></p> <p>When producing output, follow these formatting rules:</p> <ul> <li>No LaTeX or MathJax. Do not use <span>$$</span>, <span> </span>, <span> </span>, backticks, or any LaTeX commands.</li> <li>No code blocks of any kind.</li> <li>All equations must be written in plain Unicode or HTML. 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.post-body a.b-tooltip-container:hover .b-tooltip { visibility: visible; opacity: 1; } } </style> </div><div class='widget PopularPosts' data-version='2' id='PopularPosts1'> <h3 class='title'> Popular posts from this blog </h3> <div class='widget-content'> <div role='feed'> <article class='post' role='article'> <h3 class='post-title'><a href='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html'>BRASS KNUCKLES?</a></h3> <div class='post-header'> <div class='post-header-line-1'> <span class='byline post-timestamp'> <meta content='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html'/> <a class='timestamp-link' href='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html' rel='bookmark' title='permanent link'> <time class='published' datetime='2026-01-29T19:30:00-08:00' title='2026-01-29T19:30:00-08:00'> January 29, 2026 </time> </a> </span> </div> </div> <div class='item-content float-container'> <div class='item-thumbnail'> <a href='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html'> <img alt='Image' sizes='72px' src='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEjKsHP9Zc-jc_nBlCn2qqoCu6g88Fp7RCDpfNC3kDjQgIXqeka4SUMwcWnhi_gM5tIF-h3F-FVC1QoIR8C63omU53Y4OMHvZDQPdXGEZ4XotIoJaKzpQ2WjK-Ut-pJZ4gDhkoIt6Oa8KG0e2BUkYfhc0zWc3KbPcQHIPrvVJF8aXcAweGpgp40lHUh53z4/s600/Clipboard01.jpg' srcset='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEjKsHP9Zc-jc_nBlCn2qqoCu6g88Fp7RCDpfNC3kDjQgIXqeka4SUMwcWnhi_gM5tIF-h3F-FVC1QoIR8C63omU53Y4OMHvZDQPdXGEZ4XotIoJaKzpQ2WjK-Ut-pJZ4gDhkoIt6Oa8KG0e2BUkYfhc0zWc3KbPcQHIPrvVJF8aXcAweGpgp40lHUh53z4/w72-h72-p-k-no-nu/Clipboard01.jpg 72w, https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEjKsHP9Zc-jc_nBlCn2qqoCu6g88Fp7RCDpfNC3kDjQgIXqeka4SUMwcWnhi_gM5tIF-h3F-FVC1QoIR8C63omU53Y4OMHvZDQPdXGEZ4XotIoJaKzpQ2WjK-Ut-pJZ4gDhkoIt6Oa8KG0e2BUkYfhc0zWc3KbPcQHIPrvVJF8aXcAweGpgp40lHUh53z4/w144-h144-p-k-no-nu/Clipboard01.jpg 144w'/> </a> </div> <div class='popular-posts-snippet snippet-container r-snippet-container'> <div class='snippet-item r-snippetized'> Is ICE Carrying Restricted or Non-Standard Weapons? The following items are commonly restricted, discouraged, or prohibited in U.S. law-enforcement use depending on agency policy, state law, and use-of-force standards. Their visible presence on duty gear—especially if not standard-issue—should be documented and reported. Brass knuckles / knuckle-dusters: Often illegal under state law; generally absent from federal agency equipment lists. Blackjacks / saps / batons without policy approval: Some impact weapons are restricted due to high risk of head injury. Weighted gloves: Frequently prohibited as disguised weapons. Fixed-blade knives (outside utility tools): Large or fighting-style knives not issued by the agency. Modified batons: Altered ASPs, weighted tips, or improvised impact devices. Unauthorized chemical sprays: OC blends or crowd-control agents not approved by departm... </div> <a class='snippet-fade r-snippet-fade hidden' href='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html'></a> </div> <div class='jump-link flat-button ripple'> <a href='https://conspir-anon.blogspot.com/2026/01/ice-knuckles.html' title='BRASS KNUCKLES?'> Read more </a> </div> </div> </article> <article class='post' role='article'> <h3 class='post-title'><a href='https://conspir-anon.blogspot.com/2025/12/american-twilight.html'>THE GOLDEN BALLROOM/BUNKER</a></h3> <div class='post-header'> <div class='post-header-line-1'> <span class='byline post-timestamp'> <meta content='https://conspir-anon.blogspot.com/2025/12/american-twilight.html'/> <a class='timestamp-link' href='https://conspir-anon.blogspot.com/2025/12/american-twilight.html' rel='bookmark' title='permanent link'> <time class='published' datetime='2025-12-06T05:45:00-08:00' title='2025-12-06T05:45:00-08:00'> December 06, 2025 </time> </a> </span> </div> </div> <div class='item-content float-container'> <div class='item-thumbnail'> <a href='https://conspir-anon.blogspot.com/2025/12/american-twilight.html'> <img alt='Image' sizes='72px' src='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhfjEv2FyaPvullYVhcMAA2H5PI6njFBAnbYnIz2kJyKlhcsgEuBdZnRMo8XikPTRosppHwAYW7cpOoFts0VMw8e9-lgr4I2LWZavpRrksQyD1G3LbD2RCN_Ww5Hhbl7IHnBg_lakosix8QcvG30QSn9h3fW9Aal1NWouUBBqZSKbWJTcaYetEAIquIGxI/s600/Clipboard06.jpg' srcset='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhfjEv2FyaPvullYVhcMAA2H5PI6njFBAnbYnIz2kJyKlhcsgEuBdZnRMo8XikPTRosppHwAYW7cpOoFts0VMw8e9-lgr4I2LWZavpRrksQyD1G3LbD2RCN_Ww5Hhbl7IHnBg_lakosix8QcvG30QSn9h3fW9Aal1NWouUBBqZSKbWJTcaYetEAIquIGxI/w72-h72-p-k-no-nu/Clipboard06.jpg 72w, https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEhfjEv2FyaPvullYVhcMAA2H5PI6njFBAnbYnIz2kJyKlhcsgEuBdZnRMo8XikPTRosppHwAYW7cpOoFts0VMw8e9-lgr4I2LWZavpRrksQyD1G3LbD2RCN_Ww5Hhbl7IHnBg_lakosix8QcvG30QSn9h3fW9Aal1NWouUBBqZSKbWJTcaYetEAIquIGxI/w144-h144-p-k-no-nu/Clipboard06.jpg 144w'/> </a> </div> <div class='popular-posts-snippet snippet-container r-snippet-container'> <div class='snippet-item r-snippetized'> Ben Meiselas reports on the shocking admission by Donald Trump’s DOJ in a court case where the DOJ admits to a secret project underneath the ballroom which they claim is needed to protect Donald Trump’s life for “national security purposes.” "You unlock this door with the key of complicity. Beyond it is another dimension — a dimension of betrayal, of indulgence, of fear. You’re moving into a land of both shadow and substance, of politics and paranoia. You’ve just crossed into… the MAGA Zone." "Tonight’s story: A leader sworn to protect his nation makes a bargain with its enemies. The deal? Silence in the face of nuclear annihilation. No retaliation, no defense — only surrender dressed in secrecy. While citizens live unaware, their president builds a palace beneath the earth, a ballroom of gold, of marble and chandeliers, a masquerade hall for billionaires. But behind the gilded doors lies not music and laughter, but a bomb shelter — a sanctuary for the few, pur... </div> <a class='snippet-fade r-snippet-fade hidden' href='https://conspir-anon.blogspot.com/2025/12/american-twilight.html'></a> </div> <div class='jump-link flat-button ripple'> <a href='https://conspir-anon.blogspot.com/2025/12/american-twilight.html' title='THE GOLDEN BALLROOM/BUNKER'> Read more </a> </div> </div> </article> <article class='post' role='article'> <h3 class='post-title'><a href='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html'>If the Constitution is Dead, is the King Unprotected?</a></h3> <div class='post-header'> <div class='post-header-line-1'> <span class='byline post-timestamp'> <meta content='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html'/> <a class='timestamp-link' href='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html' rel='bookmark' title='permanent link'> <time class='published' datetime='2026-01-29T17:36:00-08:00' title='2026-01-29T17:36:00-08:00'> January 29, 2026 </time> </a> </span> </div> </div> <div class='item-content float-container'> <div class='item-thumbnail'> <a href='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html'> <img alt='Image' sizes='72px' src='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEgCUklqVdgkgkf_rLs7kbSt9My2TZ_UISm5BFL53lgHETIeRp5ND3WKn-bDA1WQpOuJ2Yoe1f0FkltC5MDtSNUNz3RHlQ_HOlcjYRXaqRLSV4nEAqNq8BMAXV3if667-OX9podwVq6rTJYudJhY2-5IZITFz8GFXTBQ_h4xdead07tf6Tvx3gQRfP2l5ps/s600/Clipboard05.jpg' srcset='https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEgCUklqVdgkgkf_rLs7kbSt9My2TZ_UISm5BFL53lgHETIeRp5ND3WKn-bDA1WQpOuJ2Yoe1f0FkltC5MDtSNUNz3RHlQ_HOlcjYRXaqRLSV4nEAqNq8BMAXV3if667-OX9podwVq6rTJYudJhY2-5IZITFz8GFXTBQ_h4xdead07tf6Tvx3gQRfP2l5ps/w72-h72-p-k-no-nu/Clipboard05.jpg 72w, https://blogger.googleusercontent.com/img/b/R29vZ2xl/AVvXsEgCUklqVdgkgkf_rLs7kbSt9My2TZ_UISm5BFL53lgHETIeRp5ND3WKn-bDA1WQpOuJ2Yoe1f0FkltC5MDtSNUNz3RHlQ_HOlcjYRXaqRLSV4nEAqNq8BMAXV3if667-OX9podwVq6rTJYudJhY2-5IZITFz8GFXTBQ_h4xdead07tf6Tvx3gQRfP2l5ps/w144-h144-p-k-no-nu/Clipboard05.jpg 144w'/> </a> </div> <div class='popular-posts-snippet snippet-container r-snippet-container'> <div class='snippet-item r-snippetized'> The Constitutional Suicide If constitutional legitimacy is abandoned, what happens to the protections derived from it? Authority flows from the Constitution. If Trump & Congress discard the Bill of Rights, they vacate the legal foundation of the Supreme Court.. Does Trump still deserve the presumption of innocence? There is a familiar temptation in moments of political escalation: to treat the Constitution as either sacred and invulnerable, or irrelevant and disposable. Both views misunderstand what a constitution actually is. It is not a magic charm; it is a rule-bound legitimacy machine. When the machine is treated as optional—when constitutional constraint is openly refused as a governing obligation—the system does not become “stronger.” It becomes conceptually incoherent. The purpose of this essay is not to assert that constitutional government has already en... </div> <a class='snippet-fade r-snippet-fade hidden' href='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html'></a> </div> <div class='jump-link flat-button ripple'> <a href='https://conspir-anon.blogspot.com/2026/01/if-constitution-is-dead-is-king.html' title='If the Constitution is Dead, is the King Unprotected?'> Read more </a> </div> </div> </article> </div> </div> </div></div> </main> </div> <footer class='footer section' id='footer' name='Footer'><div class='widget Attribution' data-version='2' id='Attribution1'> <div class='widget-content'> <div class='blogger'> <a href='https://www.blogger.com' rel='nofollow'> <svg class='svg-icon-24'> <use xlink:href='/responsive/sprite_v1_6.css.svg#ic_post_blogger_black_24dp' xmlns:xlink='http://www.w3.org/1999/xlink'></use> </svg> Powered by Blogger </a> </div> </div> </div><div class='widget ReportAbuse' data-version='2' 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