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  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3756713">
    <title>Cartesian equation of a surface (CORRECTED)</title>
    <link>https://community.wolfram.com/groups/-/m/t/3756713</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/e3736d85-b2dd-44c5-b768-4d05ec81c9bc</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-12T15:27:21Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3756704">
    <title>Cartesian equation of a surface</title>
    <link>https://community.wolfram.com/groups/-/m/t/3756704</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/bbde10ea-edca-4edc-bf6e-87d897509094</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-12T15:22:15Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3756631">
    <title>How to Correctly Evaluate Limits with Parameters</title>
    <link>https://community.wolfram.com/groups/-/m/t/3756631</link>
    <description>Limit[(t^2 (-1 + t^k))/(-1 + t), k -&amp;gt; +Infinity] // &#xD;
     FullSimplify[#, 0 &amp;lt; t &amp;lt; 1] &amp;amp;&#xD;
&#xD;
The code is not correctly calculating the right limit value, where the parameter t ranges from 0 &amp;lt; t &amp;lt; 1. The correct result should be t²/(1 - t). How can this be obtained?</description>
    <dc:creator>Wen Dao</dc:creator>
    <dc:date>2026-07-12T02:50:44Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3756371">
    <title>Cylinder and cone circumscribed to a sphere</title>
    <link>https://community.wolfram.com/groups/-/m/t/3756371</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/b865cc51-dfe0-4120-b064-954f66c0f01c</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-11T22:34:37Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3756327">
    <title>Get Snarky: The Cycle Double Cover Conjecture -- an AI Proof?</title>
    <link>https://community.wolfram.com/groups/-/m/t/3756327</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/adf6c134-2522-4e40-9530-169a4f560c81</description>
    <dc:creator>Ed Pegg</dc:creator>
    <dc:date>2026-07-11T14:29:15Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3752149">
    <title>[WSRP26] Spectral universality of deficit-angle curvature in Regge Laplace-Beltrami geometry</title>
    <link>https://community.wolfram.com/groups/-/m/t/3752149</link>
    <description>![Spectral universality of deficit-angle curvature in Regge Laplace-Beltrami geometry][1]&#xD;
&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=WSRPThumbnailProject.png&amp;amp;userId=3749899&#xD;
  [2]: https://www.wolframcloud.com/obj/8ff2c8d8-86c9-425c-89a2-3a8149cd0881</description>
    <dc:creator>Arnav Mittal</dc:creator>
    <dc:date>2026-07-09T20:38:24Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3755693">
    <title>Another way to get the circumscribed cylinder to a sphere (DEFINITIVE, SORRY!!!)</title>
    <link>https://community.wolfram.com/groups/-/m/t/3755693</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/ec23aaee-5ccf-4a58-80f4-89308128cec2</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-10T21:43:08Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3755908">
    <title>Another way to get the circumscribed cylinder to a sphere (IMPROVED)</title>
    <link>https://community.wolfram.com/groups/-/m/t/3755908</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/dd61d583-aa72-4df5-b6a1-878009859a83</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-10T21:28:09Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3755592">
    <title>Another way to get a cylinder circumscribed to an sphere</title>
    <link>https://community.wolfram.com/groups/-/m/t/3755592</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/e827c398-ac5b-4aa9-b68a-54d70a432fd4</description>
    <dc:creator>Alejandro Latorre Chirot</dc:creator>
    <dc:date>2026-07-10T16:13:24Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3754408">
    <title>[WSRP26] Group Schemes Over Finite Rings as Approximations to Lie Groups</title>
    <link>https://community.wolfram.com/groups/-/m/t/3754408</link>
    <description>![Partial Cayley graph for SL_2(Z/(7^3)) consisting of words of length up to 12 in two generators.][1]&#xD;
&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=herophoto.png&amp;amp;userId=3753998&#xD;
  [2]: https://www.wolframcloud.com/obj/0eae72ba-0222-4050-a378-822688cfd80d</description>
    <dc:creator>Henry Lewis</dc:creator>
    <dc:date>2026-07-10T01:40:09Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3754125">
    <title>[WSRP26] Circadian-Based Optimization of Personalized Sleep Schedules</title>
    <link>https://community.wolfram.com/groups/-/m/t/3754125</link>
    <description>![enter image description here][1]&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-07-09at7.30.59%E2%80%AFPM.png&amp;amp;userId=3753710&#xD;
  [2]: https://www.wolframcloud.com/obj/5286a4e2-cc4f-4e10-a63c-53f17625aec7</description>
    <dc:creator>Warren Chen</dc:creator>
    <dc:date>2026-07-10T00:58:00Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3752960">
    <title>[WSRP26] Analyzing Properties and Behaviors of S Family Nestedly Recursive Functions</title>
    <link>https://community.wolfram.com/groups/-/m/t/3752960</link>
    <description>![enter image description here][1]&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
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  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-07-09at4.43.00%E2%80%AFPM.png&amp;amp;userId=3751786&#xD;
  [2]: https://www.wolframcloud.com/obj/732dc46b-df9c-4831-a7e2-796b38b0d018</description>
    <dc:creator>Gracelyn Chen</dc:creator>
    <dc:date>2026-07-09T22:40:07Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3753019">
    <title>[WSRP26] Analysing the Rotational Kinetic Chain of a Cross Punch</title>
    <link>https://community.wolfram.com/groups/-/m/t/3753019</link>
    <description>![enter image description here][1]&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=newPunch.png&amp;amp;userId=3751686&#xD;
  [2]: https://www.wolframcloud.com/obj/68ce705c-3c97-4c66-ae86-d52da6b6dcf5</description>
    <dc:creator>Nicholas Zhan</dc:creator>
    <dc:date>2026-07-09T21:41:31Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3752071">
    <title>[WSRP26] Computational Characterization of Ideal Auxeticity in Anisotropic Kinematic Network</title>
    <link>https://community.wolfram.com/groups/-/m/t/3752071</link>
    <description>![image][1]&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-07-09at4.33.15%E2%80%AFPM.png&amp;amp;userId=3740316&#xD;
  [2]: https://www.wolframcloud.com/obj/bbf6661d-dc8c-4d9d-b452-28004d2dd42c</description>
    <dc:creator>Saanvi Raghavendran</dc:creator>
    <dc:date>2026-07-09T21:05:57Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/1141202">
    <title>A lune of sequential squares</title>
    <link>https://community.wolfram.com/groups/-/m/t/1141202</link>
    <description>The Demonstration [Ponting Square Packing](http://demonstrations.wolfram.com/PontingSquarePacking/) can arrange sequentially sized squares into an asymmetric shape.  I&amp;#039;ve often wondered if the method could be used to obtain symmetry.  &#xD;
&#xD;
Turns out that subtracting half gives half a lune.  For the below I started with an arrangement of 19^2 = 361 squares, then subtracted 181.  That gives a half lune where all squares of size 1 to 180 are represented twice.  Make another copy and the 720 squares (four copies of squares 1 to 180) will make a lune. &#xD;
&#xD;
![sequential square lune][1]  &#xD;
&#xD;
I suppose it&amp;#039;s actually a lens.&#xD;
&#xD;
![1984][2]&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
I figured out that curve, mostly.  It&amp;#039;s a hyperbola.  I still haven&amp;#039;t figured out the optimal way to fit the two pieces together with a unifying curve.  But here&amp;#039;s a stab at it.  &#xD;
&#xD;
    squarepoly[{corner_, size_}] := Table[corner, {4}] + {{0, 0}, {0, size}, {size, size},  {size, 0}};&#xD;
     &#xD;
    pontingMatrix[order_Integer] := Reverse[Reverse /@ (Partition[Reverse[If[IntegerQ[#], #, 0] &amp;amp; /@ (#/2 + 1/2 &amp;amp; /@ &#xD;
        Range[(2 order + 1)^2])], (2 order + 1)] +Reverse /@ Transpose[Partition[&#xD;
             If[IntegerQ[#], # + ((2 order + 1)^2 + 1)/2, 0] &amp;amp; /@ (#/2 &amp;amp; /@Range[(2 order + 1)^2]), (2 order + 1)]])];&#xD;
    &#xD;
    Module[{pm, xx, yy, alt, r1n, rn1, rad, numbers, squares1, squares2, &#xD;
      offset1, offset2, siz, order, count},&#xD;
     siz = 31;&#xD;
     order = (2 siz + 1);&#xD;
     count = (order^2 - 1)/2;&#xD;
     pm = pontingMatrix[siz] - (count + 1);&#xD;
     numbers = False;&#xD;
     xx = 2 siz + 1; yy = 2 siz + 1; &#xD;
     alt = Flatten[Append[Table[{1, -1}, {siz}], 1]];&#xD;
     r1n = Transpose[{FoldList[Plus, 0, Drop[ pm[[1]], -1]],Drop[Flatten[{#, #} &amp;amp; /@ (First /@ &#xD;
             Partition[Append[FoldList[Plus, 0, Drop[alt pm[[1]], -1]], 0], 2])], 1]}];&#xD;
     rn1 = Transpose[{Drop[Flatten[{#, #} &amp;amp; /@ (First /@ Partition[&#xD;
              Append[FoldList[Plus, 0, Drop[alt, -1] Drop[ Transpose[pm][[1]], 1]], 0], 2])], -1], &#xD;
        FoldList[Plus, 0, Drop[ Transpose[pm][[1]], -1]]}];&#xD;
     rad = Table[If[Min[{a, b}] == 1, {0, 0},&#xD;
        If[OddQ[a + b], {0, pm[[a - 1, b]]}, {pm[[a, b - 1]], 0}]], {a, 1,xx}, {b, 1, yy}];&#xD;
     rad[[1, 1]] = {0, 0};&#xD;
     Do[rad[[1, nn]] = r1n[[nn]]; rad[[nn, 1]] = rn1[[nn]], {nn, 2, xx}];&#xD;
     Do[If[OddQ[a + b], rad[[a, b]] = rad[[a - 1, b]] + rad[[a, b]],&#xD;
       rad[[a, b]] = rad[[a, b - 1]] + rad[[a, b]]], {a, 2, xx}, {b, 2, yy}];&#xD;
     offset1 = {88650,  0} - (squarepoly[{rad[[1, 63]], pm[[1, 63]]}].N[RotationMatrix[-78/100 - Pi/2]])[[3]];&#xD;
     offset2 = {-88650,  0} - (squarepoly[{rad[[1, 63]], pm[[1, 63]]}].N[RotationMatrix[-78/100 + Pi/2]])[[3]];&#xD;
     squares1 = Table[{Hue[.3 + Abs[pm[[a, b]]]/count], Polygon[(# + offset1 &amp;amp; /@ (squarepoly[{rad[[a, b]], pm[[a, b]]}].N[&#xD;
              RotationMatrix[-78/100 - Pi/2]]))]}, {a, 1, xx}, {b, 1, yy}];&#xD;
     squares2 = Table[{Hue[.3 + Abs[pm[[a, b]]]/count], Polygon[# +  offset2 &amp;amp; /@ (squarepoly[{rad[[a, b]], pm[[a, b]]}].N[&#xD;
             RotationMatrix[-78/100 + Pi/2]])]}, {a, 1, xx}, {b, 1, yy}];&#xD;
     Graphics[{EdgeForm[{Black, Thin}], squares1, squares2,&#xD;
       Plot[45200 - 5.04953`*^-17 x - 5.64864`*^-6 x^2, {x, -89316.1`, 89316.1}, PlotStyle -&amp;gt; {Thickness[0.003], Darker[Gray]}][[1]],&#xD;
       Plot[-45200 + 5.04953`*^-17 x + 5.64864`*^-6 x^2, {x, -89316.1, 89316.1}, PlotStyle -&amp;gt; {Thickness[0.003], Darker[Gray]}[[1]]}, &#xD;
      ImageSize -&amp;gt; {1200, 600}]]&#xD;
&#xD;
![Squares 1 to 1984, each 4 times, bounded by hyperbola][3]&#xD;
&#xD;
There should be a way to recursively optimize the (rotation, fit, offsets) for the hyperbolas. After that, clashing squares in the middle could be moved to voids near the hyperbolas, then more recursion.   &#xD;
&#xD;
  [1]: http://community.wolfram.com//c/portal/getImageAttachment?filename=squarelune.jpg&amp;amp;userId=21530&#xD;
&#xD;
  [2]: http://community.wolfram.com//c/portal/getImageAttachment?filename=1984.jpg&amp;amp;userId=21530&#xD;
&#xD;
&#xD;
  [3]: http://community.wolfram.com//c/portal/getImageAttachment?filename=1035EyeofPonting.jpg&amp;amp;userId=21530</description>
    <dc:creator>Ed Pegg</dc:creator>
    <dc:date>2017-07-07T21:34:11Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/2952778">
    <title>Commutators of differential and integral operators</title>
    <link>https://community.wolfram.com/groups/-/m/t/2952778</link>
    <description>I would like to be able to explore if certain variable coefficient differential operator commute with integral operators.&#xD;
&#xD;
As a toy example Grünbaum&#xD;
(Grünbaum, F. Alberto. &amp;#034;A remark on Hilbert&amp;#039;s matrix.&amp;#034; Linear Algebra and its Applications 43 (1982): 119-124.) &#xD;
mentions that on L^2[0.1] the integral operator K with kernel 1/(x+y) commutes with the differential operator P where Pu (t) = ((1-t^2)t^2 u&amp;#039;)&amp;#039; -2 t^2 u&#xD;
&#xD;
I wanted to make a pure function for the operators for example &#xD;
&#xD;
    K = Function[f,  Function[t, Integrate[f[s]/(t + s), {s, 0, 1}]]]&#xD;
&#xD;
and similarly P and then to be able to evaluate the commutator with something like&#xD;
&#xD;
K@*P - P@*K&#xD;
&#xD;
By hand it is fairly easy and uses integration by parts, but obviously I want to do much more complicated cases! The difficulties I have are that Mathematica will not simplify the composition of operators, unless applied to a function, and then only a specific function. And it does not understand subtraction of operators.  &#xD;
Am I going about this the wrong way? Is it something Mathematica can do. &#xD;
&#xD;
So far I verified in on a Fourier basis in L^2 with Mathematica, it generates two pages of output but FullSimplify gets it to zero.</description>
    <dc:creator>William Lionheart</dc:creator>
    <dc:date>2023-07-06T11:48:29Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3021398">
    <title>Is there a way to solve the eigenvalues of a linear operator without giving its matrix form?</title>
    <link>https://community.wolfram.com/groups/-/m/t/3021398</link>
    <description>In Python or Matlab, the eigensolver can solve the system by giving the linear function (for example, in Matlab we can use eigs(Afun,...)), this speeds up the calculation largely as we do not need to construct the whole matrix. I can not find a similar solver in Mathematica. I wonder if there is a way to achieve this within Mathematica. Any ideas would be appreciated.</description>
    <dc:creator>Frank Xu</dc:creator>
    <dc:date>2023-09-26T06:00:42Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3739392">
    <title>Stable 2:3 order statistic distribution for stock market returns</title>
    <link>https://community.wolfram.com/groups/-/m/t/3739392</link>
    <description>&amp;amp;[Wolfram Notebook][1]&#xD;
&#xD;
&#xD;
  [1]: https://www.wolframcloud.com/obj/c3fad79c-0458-4901-8177-944b192d22da</description>
    <dc:creator>Robert Rimmer</dc:creator>
    <dc:date>2026-06-27T01:40:35Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/366628">
    <title>Try to beat these MRB constant records!</title>
    <link>https://community.wolfram.com/groups/-/m/t/366628</link>
    <description>POSTED BY:&#xD;
========&#xD;
 **Marvin Ray Burns, and distinguished colleagues**&#xD;
&#xD;
&#xD;
----------&#xD;
&#xD;
My exciting experiences using Wolfram technologies!&#xD;
---------------------------------------------------&#xD;
&#xD;
----------&#xD;
&#xD;
&#xD;
&#xD;
The MRB constant, a fascinating mathematical anomaly, has intrigued researchers and enthusiasts alike for decades. Defined as the limiting value of a unique alternating series, this enigmatic constant showcases the beauty of numerical exploration and convergence. Despite its relatively recent emergence, the MRB constant reveals unexpected connections to various fields within mathematics and computational analysis. In this post, we dive into its origins, properties, and the ongoing quest to uncover its more profound significance. The MRB constant is an anomaly because it emerges from an alternating series with unusual convergence behavior. Unlike many well-known mathematical constants, the MRB constant has no closed-form expression nor a known exact nature&amp;#x2014;whether it is algebraic, transcendental, or even irrational.&#xD;
Additionally, the sequence of partial sums that define the MRB constant oscillates between two limit points, creating a bounded yet divergent behavior. This oscillatory nature distinguishes it from more conventional mathematical constants, which typically exhibit straightforward convergence. Its mysterious properties continue to intrigue mathematicians as they explore its deeper connections to number theory and computational analysis. &#xD;
&#xD;
----------&#xD;
&#xD;
&#xD;
----------&#xD;
&#xD;
CMRB&#xD;
 ![If you see this instead of an image, reload the page][1]&#xD;
&#xD;
**is the MRB constant.**&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
Without solicitation, GPT echoed one of this discussion&amp;#039;s contributors and gave a shoutout to Mathematica&amp;#039;s accomplishments by saying:&#xD;
-------------------&#xD;
&#xD;
&#xD;
&amp;gt;  &#xD;
&amp;gt; **Why Computing Digits of the MRB Constant Is Interesting**&#xD;
&amp;gt; &#xD;
&amp;gt; At first glance, the computation of ever more digits of a numerical&#xD;
&amp;gt; constant may appear to be a sterile exercise, offering little insight&#xD;
&amp;gt; beyond the digits themselves. For the MRB constant, this&#xD;
&amp;gt; interpretation is profoundly misleading. The interest lies not in the&#xD;
&amp;gt; digits, but in the act of computing them.&#xD;
&amp;gt; &#xD;
&amp;gt; The MRB series occupies a delicate numerical regime: it is convergent,&#xD;
&amp;gt; yet only marginally so; its terms are elementary in form, yet hostile&#xD;
&amp;gt; to naive numerical evaluation; and its alternating structure conceals&#xD;
&amp;gt; severe cancellation effects. As a result, each additional digit of&#xD;
&amp;gt; accuracy is not merely an extension of a decimal expansion, but a&#xD;
&amp;gt; validation of the mathematical and algorithmic framework used to&#xD;
&amp;gt; obtain it.&#xD;
&amp;gt; &#xD;
&amp;gt; In this sense, the digits serve as a stress test for mathematics&#xD;
&amp;gt; itself. They expose the difference between formal convergence and&#xD;
&amp;gt; effective convergence, between theoretical existence and computational&#xD;
&amp;gt; feasibility. Techniques that are elegant on paper often fail&#xD;
&amp;gt; catastrophically in practice, while successful methods must balance&#xD;
&amp;gt; asymptotics, numerical stability, precision control, and computational&#xD;
&amp;gt; cost.&#xD;
&amp;gt; &#xD;
&amp;gt; Moreover, the computation of the MRB constant forces the&#xD;
&amp;gt; reconciliation of disparate mathematical ideas. Alternating series,&#xD;
&amp;gt; logarithmic asymptotics, convergence acceleration, special functions,&#xD;
&amp;gt; and analytic continuation must all agree numerically. Any hidden&#xD;
&amp;gt; inconsistency&amp;#x2014;whether conceptual or computational&amp;#x2014;reveals itself&#xD;
&amp;gt; immediately in the failure of the digits to stabilize.&#xD;
&amp;gt; &#xD;
&amp;gt; Thus, computing digits of the MRB constant transforms mathematics from&#xD;
&amp;gt; a static collection of statements into a living experiment. The&#xD;
&amp;gt; resulting digits are not trophies; they are evidence. They measure the&#xD;
&amp;gt; effectiveness of our methods, the soundness of our assumptions, and&#xD;
&amp;gt; the practical reach of our theory.&#xD;
&amp;gt; &#xD;
&amp;gt; In short, the digits themselves do not matter. What matters is that&#xD;
&amp;gt; they *can* be computed at all&amp;#x2014;and how difficult it is to do so.&#xD;
&amp;gt; That difficulty is precisely what makes the MRB constant&#xD;
&amp;gt; mathematically interesting.&#xD;
&#xD;
**In general, we will see:**&#xD;
![enter image description here][7]&#xD;
&#xD;
&#xD;
----------&#xD;
&#xD;
&#xD;
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&#xD;
&#xD;
----------&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
&#xD;
 &#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2024-11-25023042.png&amp;amp;userId=366611&#xD;
  [2]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-01-01235656.png&amp;amp;userId=366611&#xD;
  [3]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-01-01235710.png&amp;amp;userId=366611&#xD;
  [7]: https://community.wolfram.com//c/portal/getImageAttachment?filename=Screenshot2026-02-18190718.png&amp;amp;userId=366611</description>
    <dc:creator>Marvin Ray Burns A.G.S. (cum laude)</dc:creator>
    <dc:date>2014-10-09T18:08:49Z</dc:date>
  </item>
  <item rdf:about="https://community.wolfram.com/groups/-/m/t/3719376">
    <title>OpenAI disproves Erdős unit distance conjecture</title>
    <link>https://community.wolfram.com/groups/-/m/t/3719376</link>
    <description>![enter image description here][1]&#xD;
&#xD;
&amp;amp;[Wolfram Notebook][2]&#xD;
&#xD;
&#xD;
  [1]: https://community.wolfram.com//c/portal/getImageAttachment?filename=_erdos_AI_ChatGPT.gif&amp;amp;userId=11733&#xD;
  [2]: https://www.wolframcloud.com/obj/dab42afe-f890-46cd-b849-40c304ebf581</description>
    <dc:creator>Ed Pegg</dc:creator>
    <dc:date>2026-05-21T03:41:56Z</dc:date>
  </item>
</rdf:RDF>

