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Huh — no solutions to POW-13 came in!  I guess I was surprised by that.

Ah well, that’s okay. The problem wasn’t exactly trivial; there are some fairly deep and interesting things going on in that problem that I’d like to share now. First off, let me say that the problem comes from The Unapologetic Mathematician, the blog written by John Armstrong, who posted the problem back in March this year. He in turn had gotten the problem from Noam Elkies, who kindly responded to some email I wrote and had some pretty insightful things to say.

In lieu of a reader solution, I’ll give John’s solution first, and then mine, and then touch on some of the things Noam related in his emails. But before we do so, let me paraphrase what John wrote at the end of his post:

Here’s a non-example. Pick m points (1, 0), (2, 0), (3, 0) and so on up to (m, 0). Pick n points (1, 1), (2, 1), (3, 1), and so on up to (n, 1). In this case we have m+n-1 blocking points at (1, \frac1{2}), (\frac{3}{2}, \frac1{2}), and so on by half-integers up to (\frac{m+n}{2}, \frac1{2}). Of course this solution doesn’t count because the first m points lie on a line as do the n points that follow, which violates the collinearity condition of the problem.

Here’s a picture of that scenario when m = n = 3:


Does this configuration remind you of anything? Did somebody say “Pappus’s theorem“? Good. Hold that thought please.

Okay, in the non-example the first m+n points were on two lines, which is disallowed. Now the two lines here, y = 0 and y = 1, form a degenerate conic y^2 - y = 0. Thinking in good algebraic geometry fashion, perhaps we can modify the non-solution by replacing the degenerate conic by an honest (smooth) nondegenerate conic, like an ellipse or something, so that at most two of the m+n points are on any given line. This should put one in the mood for our first solution.

John Armstrong writes:  Basically, I took the non-example and imagined bending back the two lines to satisfy the collinearity (pair-of-lines = degenerate conic, so non-example is degenerate example).  The obvious pair of curves to use is the two branches of a hyperbola.  But hyperbolas can be hard to work with, so I decided to do a projective transformation to turn it into a parabola.

So let’s consider points on a parabola.  The points (-i, i^2) and (j, j^2) are connected by a line of slope
\displaystyle \frac{j^2 - i^2}{j + i} = j - i

The line itself is y = (j-i)x + i j.  Which has the obvious y-intercept (0, i j).  Now we need to pick a lot of i and j values to get repeated products. Place m points at (-1, 1), (-2, 4), (-4, 16), (-8, 64), and so on above the negative powers of two.  Place n points at (1, 1), (2, 4), (4, 16), (8, 64), and so on above the positive powers of two.  The blocking points are then at (0, 1), (0, 2), (0, 4), (0, 8), and so on up the y-axis by powers of two.  Presto! \Box

Very nice. My own solution was less explicit in the sense that I didn’t actually write down coordinates of points, but gave instead a general recipe which relies instead on the geometry of conics, in fact on a generalization of Pappus’s theorem known to me as “Pascal’s mystic hexagon“. I first learned about this from a wonderful book:

  • C. Herbert Clemens, A Scrapbook of Complex Curve Theory (2nd Edition), Graduate Studies in Mathematics 55, AMS (2002).

Pascal’s Mystic Hexagon, version A: Consider any hexagon inscribed in a conic, with vertices marked x_1, x_2, x_3, y_1, y_2, y_3. For i \neq j, mark the intersection of the lines \overline{x_i y_j} \cap \overline{x_j y_i} by z_{i+j-1}. Then z_2, z_3, z_4 are collinear. (The reason for the strange indexing will be clear in a moment.)


Pascal’s Mystic Hexagon, version B: Consider any pentagon inscribed in a conic C, with vertices marked x_1, x_2, x_3, y_1, y_2. Choose any line L through z_2 = \overline{x_1 y_2} \cap \overline{y_1 x_2}, and define z_3 = L \cap \overline{y_1 x_3} and z_4 = L \cap \overline{y_2 x_3}.  Then the intersection y_3 := \overline{x_1 z_3} \cap \overline{x_2 z_4} is the sixth point of a hexagon inscribed in C.

The following solution uses version B.

Solution by Todd and Vishal: For the sake of explicitness, let the conic C be a circle x^2 + y^2 = 1 and let the line (segment) L be the diameter along y = 0. Choose two points x_1, x_2 on C above L and a point y_1 on C below L. The remaining points are determined recursively by a zig-zag procedure, where at each stage x_{n+1} is the intersection C \cap \overline{y_1 z_{n+1}}, where z_{2n} = L \cap \overline{x_{n+1} y_n}, where y_{n+1} = C \cap \overline{x_1 z_{n+1}}, and z_{2n+1} = L \cap \overline{x_{n+1} y_{n+1}}. We will show the blocking condition is satisfied: for all i, j, the point z_{i+j-1} is on the line \overline{x_i y_j}.

To get started, notice that the blocking condition is trivially satisfied up to the point where we construct z_1, z_2, y_2, z_3, x_3, z_4. Mystic Hexagon B ensures that y_3, as defined above, is blocked from x_1 by z_3 and from x_2 by z_4. Then define z_5 as above. So far the blocking condition is satisfied.


Suppose the blocking condition is satisfied for the points x_1, \ldots, x_n, y_1, \ldots, y_n, z_1, \ldots, z_{2n-1}. Define x_{n+1} = C \cap \overline{y_1 z_{n+1}}, as above. Then Mystic Hexagon B, applied to the pentagon consisting of points y_1, y_2, y_3, x_{n-1}, x_n, shows that x_{n+1} is blocked from y_1 by z_{n+1} and from y_2 by z_{n+2}.

This shows that x_{n+1} could have been defined to be C \cap \overline{y_2 z_{n+2}}. Then Mystic Hexagon B, applied to the pentagon y_2, y_3, y_4, x_{n-1}, x_n, shows that x_{n+1} is blocked from y_2 by z_{n+2} and from y_3 by z_{n+3}. This shows x_{n+1} could have been defined to be C \cap \overline{y_3 z_{n+3}}.

And so on up the inductive ladder: for 2 \leq i \leq n-1, defining x_{n+1} = C \cap \overline{y_{i-1} z_{n+i-1}}, Hexagon B applied to the pentagon y_{i-1}, y_i, y_{i+1}, x_{n-1}, x_n shows that x_{n+1} could have been defined to be C \cap \overline{y_i z_{n+i}}. This shows the blocking condition is satisfied for 1 \leq i \leq n+1, 1 \leq j \leq n-1. We block x_{n+1} from y_n by defining z_{2n} as above, to extend up to j = n.

Then, as prescribed above, we define y_{n+1} = C \cap \overline{x_1 z_{n+1}}, and repeat the preceding argument mutatis mutandis (interchanging x‘s and y‘s), to obtain the blocking conditions up to 1 \leq i \leq n+1, 1 \leq j \leq n+1. This completes the proof. \Box

What this argument shows (with Hexagon B doing all the heavy lifting) is that no cleverness whatsoever is required to construct the desired points: starting with any nondegenerate conic C, any secant line L, and any three initial points x_1, x_2, y_1 on C to get started (with x_1, x_2‘s on one side of L and y_1 on the other), the whole construction is completely forced and works no matter what!

Which may lead one to ask: what is behind this “miracle” called Pascal’s Mystic Hexagon?  Actually, not that much! Let me give a seat-of-the-pants argument for why one might expect it to hold, and then give a somewhat more respectable argument.

Define a planar cubic to be the locus P(x, y) = 0 of any degree 3 polynomial P in two variables. (We should actually be doing this as projective geometry, so I ought to write P(x, y, z) = 0 where P is homogeneous of degree 3, but I think I’ll skip that.) For example, the union of three distinct lines is a cubic where P is a product of three degree 1 polynomials. What is the dimension of the space of planar cubics? A cubic polynomial P(x, y),

a_0 + a_1 x + a_2 y + a_3 x^2 + a_4 x y + a_5 y^2 + a_6 x^3 + a_7 x^2 y + a_8 x y^2 + a_9 y^3,

has 10 coefficients. But the equation P(x, y) = 0 is equivalent to the equation \lambda P(x, y) = 0 for any nonzero scalar \lambda; modding out by scalars, there are 9 degrees of freedom in the space of cubics. What is the dimension of the space of cubics passing through a given point (x, y) = (a, b)? The condition P(a, b) = 0 gives one linear equation on the coefficients a_0, \ldots, a_9, so we cut down a degree of freedom, and the dimension would be 8. Similarly, if we ask for the dimension of cubics passing through 8 given points, we get a system of eight linear equations, and we cut down by eight degrees of freedom: in general, the space of cubics through 8 points is “expected” to be (is “almost always”) 1-dimensional, in fact, a (projective) line.

In the configuration for Pascal’s Mystic Hexagon, version A


we see three cubics passing through the 8 points x_1, x_2, x_3, y_1, y_2, y_3, z_2, z_3, namely:

  • A = \overline{x_1 y_2} \cup \overline{x_2 y_3} \cup \overline{x_3 y_1}
  • B = \overline{x_2 y_1} \cup \overline{x_3 y_2} \cup \overline{x_1 y_3}
  • C \cup L where the conic C is defined by a degree 2 polynomial

Since we expect that the space of cubics through these eight points is a line, we should have a linear relationship between the cubic polynomials P, Q, R used respectively to define A, B, and C \cup L above, hence we would get

\lambda P(x, y) + \mu Q(x, y) = R(x, y)

for some scalars \lambda, \mu. Thus, if a ninth point z_4 = (a, b) is in A and B, so that P(a, b) = Q(a, b) = 0, then R(a, b) = 0. Thus z_4 lies in C \cup L as well, and if z_4 isn’t on C, it must be on the line L. Thus, “generically” we expect z_2, z_3, z_4 to be collinear, whence Hexagon A.

This rough argument isn’t too far removed from a slightly more rigorous one. There’s a general result in projective algebraic geometry called Bézout’s theorem, which says that a degree m planar curve and a degree n planar curve either intersect in m n points (if you count them right, “with multiplicity”) or they have a whole curve component in common. (Fine print: to make this generally true, you have to work in the projective plane, and you have to work over an algebraically closed field.) A much weaker result which removes all the fine print is that a degree m curve and a degree n curve either have a curve component in common, or they intersect in at most m n points. In particular, in the notation above, the cubics A and B intersect in 9 points, 6 of which are on the conic C. Pick a seventh point (a, b) on C, away from those six, and let \lambda = Q(a, b) and \mu = -P(a, b). Then we see that the locus of the degree 3 polynomial

T(x, y) = \lambda P(x, y) + \mu Q(a, b) = 0

intersects the degree 2 conic C in at least 7 points (namely, x_1, x_2, x_3, y_1, y_2, y_3 and (a, b)), greater than the expected number 3 \cdot 2, which is impossible  unless the loci of T and C have a component in common. But the conic C has just one component — itself — so one can conclude that its defining degree 2 polynomial (I’ll call it C(x, y)) must divide T. Then we have

T(x, y) = \lambda P(x, y) + \mu Q(x, y) = C(x, y)L(x, y)

for some degree 1 polynomial L, so the last three of the nine points of intersection A \cap B, which are zeroes of P and Q, must be zeroes of the linear polynomial L, and hence are collinear. Thus we obtain Pascal’s Mystic Hexagon, version A. \Box

It’s clear then that what makes the Mystic Hexagon tick has something to do with the geometry of cubic curves. With that in mind, I’m now going to kick the discussion up a notch, and relate a third rather more sophisticated construction on cubics which basically subsumes the first two constructions. It has to do with so-called “elliptic curves“.

Officially, an elliptic curve is a smooth projective (irreducible) cubic “curve” over the complex numbers. I put “curve” in quotes because while it is defined by an equation P(x, y) = 0 where P is a polynomial of degree 3, the coefficients of P are complex numbers as are the solutions to this equation. We say “curve” in the sense that locally it is like a “line”, but this is the complex line \mathbb{C} we’re talking about, so from our real number perspective it is two-dimensional — it actually looks more like a surface. Indeed, an elliptic curve is an example of a Riemann surface. It would take me way too far afield to give explanations, but when you study these things, you find that elliptic curves are Riemann surfaces of genus 1. In more down-to-earth terms, this means they are tori (toruses), or doughnut-shaped as surfaces. Topologically, such tori or doughnuts are cartesian products of two circles.

Now a circle or 1-dimensional sphere S^1 carries a continuous (abelian) group structure, if we think of it as the set of complex numbers \{z: |z| = 1\} of norm 1, where the group operation is complex multiplication. A torus S^1 \times S^1 also carries a group structure, obtained by multiplying in each of the two components. Thus, given what we have said, an elliptic curve also carries a continuous group structure. But it’s actually much better than that: one can define a group structure on a smooth complex cubic C (in the complex plane \mathbb{C}^2, or rather the projective complex plane P^2(\mathbb{C})) not just by continuous operations, but by polynomially defined operations, and the definition of the group law is just incredibly elegant as a piece of geometry. Writing the group multiplication as addition, it says that if a, b, c are points on C, then

a + b = -c \qquad (a + b + c = 0)

if a, b, c are collinear. [To be precise, one must select a point 0 on C to serve as identity, and this point must be one of the nine inflection points of C. When a and b coincide (are “infinitesimally close”), the line through a and b is taken to be tangent to C; when a, b, c coincide, this is a line of inflection.]

This is rather an interesting thing to prove, that this prescription actually satisfies the axioms for an abelian group. The hardest part is proving associativity, but this turns out to be not unlike what we did for Pascal’s Mystic Hexagon: basically it’s an application of Bézout’s theorem again. (In algebraic geometry texts, such as Hartshorne’s famous book, the discussion of this point can be far more sophisticated, largely because one can and does define elliptic curves as certain abstract 1-dimensional varieties or schemes which have no presupposed extrinsic embeddings as cubic curves in the plane, and there the goal is to understand the operations intrinsically.)

In the special case where C is defined by a cubic polynomial with real coefficients, we can look at the locus of real solutions (or “real points”), and it turns out that this prescription for the group law still works on the real locus, in particular is still well-defined. (Basically for the same reason that if you have two real numbers a, b which are solutions to a real cubic equation p(x) = 0, then there is also a third real solution c.) There is still an identity element, which will be an inflection point of the cubic.

Okay, here is a third solution to the problem, lifted from one of Noam Elkies’ emails. (The original formulation of the problem spoke in terms of r “red” points (instead of my x_1, \ldots, x_m), b “blue” points (instead of my y_1, \ldots, y_n), and “blocking” points which play the role of my z_1, \ldots, z_{m+n-1}.) The addition referred to is the addition law on an elliptic curve. I’ve taken the liberty of paraphrasing a bit.

“Choose points B, R on the real points of an elliptic curve such that -(B+R) is in-between B and R.  Then set

  • red points:     R + i P, 0 \leq i \leq r-1
  • blue points:    B + j P, 1 \leq j \leq b-1
  • blocking points:  -(R+B+kP), 0 \leq k \leq r+b-2

where P is a real point on the elliptic curve very close to the identity.  The  pair R + i P, B + j P is blocked by -(R + B + (i + j)P, because these three points are collinear, and the smallness of P guarantees that the blocking point is actually between the red point and blue point, by continuity.”

Well, well. That’s awfully elegant. (According to Noam’s email, it came out of a three-way conversation between Roger Alperin, Joe Buhler, and Adam Chalcraft. Edit: Joe Buhler informs me in email that Joel Rosenberg’s name should be added. More at the end of this post.) Noam had given his own slick solution where again the red and blue points sit on a conic and the blocking points lie on a line not tangent to the conic, and he observed that his configuration was a degenerate cubic, leading him to surmise that his example could in a sense be seen as a special case of theirs.

How’s that? The last solution took place on a smooth (nondegenerate) cubic, so the degenerate cubic = conic+line examples could not, literally speaking, be special cases. Can the degenerate examples be seen in terms of algebraic group structures based on collinearity?

The answer is: yes!  As you slide around in the space of planar cubics, nondegenerate cubics (the generic or typical case) can converge to cubics which are degenerate in varying degrees (including the case of three lines, or even a triple line), but the group laws on nondegenerate cubics based on collinearity converge to group laws, even in degenerate cases! (I hadn’t realized that.)  You just have to be careful and throw away the singular points of the degenerate cubic, but otherwise you can basically still use the definition of the group law based on collineation, although it gets a little tricky saying exactly how you’re supposed to add points on a line component, such as the line of conic+line.

So let me give an example of how it works. It seems convenient for this purpose to use John Armstrong’s model which is based on the parabola+line, specifically the locus of (y - x^2)x = 0. The singular points of its projective completion are at (0, 0) and the point where the y-axis meets the line at infinity. After throwing those away, what remains is a disjoint union of four pieces: right half of parabola, left half of parabola, positive y-axis, negative y-axis.

We can maybe guess that since a + b + c = 0 implies a, b, c collinear, that the two pieces of the y-axis form a subgroup for the group law we are after (also, these two pieces together should suggest the two halves of the multiplicative group of nonzero reals \mathbb{R}^*, but don’t jump to conclusions how this works!). If so, then we notice that if a and b lie on the parabola, then the line between them intersects the y-axis at a point c, so then the parabolic part would not be closed under multiplication.

One is then led to consider that the group structure of this cubic overall is isomorphic to the group \{-1, 1\} \times \mathbb{R}^*, with the linear part identified somehow with the subgroup \{1\} \times \mathbb{R}^*, and the parabolic part with \{-1\} \times \mathbb{R}^*.

I claim that the abelian group structure on the punctured y-axis should be defined by

(0, x) + (0, y) := (0, - x y)

so that the identity element on the cubic is (0, -1), and the inverse of (0, x) is (0, 1/x). The remainder of the abelian group structure on the cubic is defined as follows:

(s, s^2) + (t, t^2) := (0, -1/(s t))

(0, x) + (s, s^2) := (-s/x, s^2/x^2)

Undoubtedly this group law looks a bit strange!  So let’s do a spot check. Suppose (0, a), (s, s^2), and (t, t^2) are collinear. Then it is easily checked that a = -s t, and each of the two equations

(0, a) + (s, s^2) = (t^{-1}, t^{-2}) = -(t, t^2)

(s, s^2) + (t, t^2) = (0, 1/a) = -(0, a)

is correct according to the group law, so the three collinear points do add to the identity and everything checks out.

All right, let’s retrieve John’s example as a special case. Take R = (1, 1) as a red point, B = (-1, 1) as a blue point, and -(B + R) = (0, 1) as blocking point. Take a point P “sufficiently close” to the identity, say (0, -1/2). Then

R + i P = (1, 1) + (0, -1/2^i) = (2^i, 2^{2i})

B + j P = (-1, 1) + (0, -1/2^j) = (-2^j, 2^{2j})

which was John’s solution.

Another long post from yours truly. I was sorry no solutions came from our readers, but if you’d like another problem to chew on, here’s a really neat one I saw just the other day. Feel free to discuss in comments!

Exercise: Given a point on a circle, show how to draw a tangent to the point using ruler only, no compass. Hint: use a mystic hexagon where two of the points are “infinitesimally close”.

Added July 25: As edited in above, Joel Rosenberg also had a hand in the elliptic curves solution, playing an instrumental role in establishing some of the conjectures, such as that r + b - 1 is the minimal number of blocking points under certain assumptions, and (what is very nice) that the elliptic curves solution is the most general solution under certain assumptions. I thank Joe Buhler for transmitting this information.

There is quite a buzz on the physics (and also math) blogospheres over the release of seven videotaped lectures, which were delivered by Richard P. Feynman as part of Cornell University’s Messenger Lecture Series of November 1964. The videos have been released by Microsoft Research with quite a few enhancements, though, I believe, they have been around on YouTube for quite some time.

I watched the first two video lectures, titled ‘Lecture 1: The Law of Gravitation – An Example of Physical Law‘ and ‘Lecture 2: The Relation of Mathematics and Physics‘. It goes without saying that they are spell-binding and brilliant! Of course, the textbook ‘The Feymnan Lectures on Physics‘ (which was followed later by a problem-solving supplement that I highly recommend) is such a joy to read, but if you wish to learn physics “face to face” from the master, then I exhort, nay implore, you to watch those video lectures.

(I came to know about the existence of the videos released by the Microsoft Research group from Terence Tao.)

It’s been an awfully long time since I’ve posted anything; time to finally break the silence.

This problem appeared elsewhere on the internet some months ago; some of you may have already seen it. I don’t want to say right away where I saw it, because there was some commentary which included some rough hints which I don’t want to give, but I’ll be sure to give credit when the solution is published. I’ll bet some of you will be able to find a solution, and will agree it’s quite cute. Here it is:

Given integers m, n \geq 1, show that it is possible to construct a set of m + n points in the plane, let’s say x_1, \ldots, x_m, y_1, \ldots, y_n, so that no three points of the set are collinear, and for which there exist points z_1, z_2, \ldots, z_{m+n-1}, all lying on a straight line, and arranged so that on the line between any x_i and any y_j, some z_k lies between them.

So no x_i can “see” any y_j, because there’s always some z_k blocking the view. As the proposer observed, the problem would be easy if we had m n z‘s to play with, one for each pair (x_i, y_j). But here there are only m+ n-1 z‘s, so some of them will have to do more than their fair share, blocking the view between quite a few (x, y)-pairs simultaneously. Thus, you have to arrange the x‘s and y‘s so that a lot of the lines between them will be coincident at a point z, and subject to the constraint I italicized above.

Please submit solutions to topological[dot]musings[At]gmail[dot]com by Friday, July 17, 11:59 pm (UTC); do not submit solutions in Comments. Everyone with a correct solution will be inducted into our Hall of Fame! We look forward to your response.

High-school students and undergraduates are (almost) always taught the following definition of an equivalence relation.

A binary relation R on a set A is an equivalence iff it satisfies

  • the reflexive property: for all a  in A, a R a,
  • the symmetric property: for all a, b in A, if a R b, then b R a, and
  • the transitive property: for all a, b, c in A, if a R b and b R c, then a R c.

However, there is another formulation of an equivalence relation that one usually doesn’t hear about, as far as I know. And, it is the following one.

A binary relation R on a set A is an equivalence iff it satisfies

  • the reflexive property: for all a  in A, a R a, and
  • the euclidean property: for all a, b, c in A, if a R b and a R c, then b R c.

Exercise:  Show that a binary relation R on a set A is reflexive, symmetric and transitive iff it is reflexive and euclidean.

Welcome to the 54th Carnival of Mathematics, and Happy Fourth of July to our American readers! Indeed, the carnival should have been hosted yesterday, and I apologize for being a day late.

Trivia: Today, we have the 234th Independence Day celebrations in the  US, and ours is the 54th carnival. 2+3+4 = 5+4, see? Boy, do I feel so clever!

Ok, let’s begin, now!

We start off with a post, submitted by Shai Deshe, that presents a collection of YouTube videos explaining different kinds of infinities in set theory, causality vs conditionality in probability and some topology. The videos are the kind of ones that “math people” could use to explain a few mathematical concepts to their friends, family members and colleagues who may not be enamored of math very much but may still possess a lingering interest in it.

Experimental philosophy, according to the Experimental Philosophy Society, “involves the collection of empirical data to shed light on philosophical issues“. As such, a careful quantitative analyses of results of experiments are used to shed light on many philosophical issues/debates. Anthony Chemero wrote a post titled, ‘What Situationist Experiments Show‘, that links to a paper with the same title that he coauthored with John Campbell and Sarah Meerschaert. In the paper, the authors, through quantitative analyses of actual experimental data, argue that virtue ethics has not lost to the siuationist side, whose critiques of virtue theory are far from convincing.

Next, I would like to bring the readers’ attention to two math blogs that came into existence somewhat recently and which I think have a lot of really good mathematical content. They are Annoying Precision and A Portion of the Book. In my opinion, their blog posts contain a wealth of mathematical knowledge, especially for undergraduates (and graduate students too!), who, if inclined toward problem-solving, will enjoy the posts even more. Go ahead and dive into them!

At Annoying Precision, a project aimed at the “Generally Interested Lay Audience” that Qiaochu Yuan started aims “to build up to a discussion of the Polya enumeration theorem without assuming any prerequisites other than a passing familiarity with group theory.” It begins with GILA I: Group Actions and Equivalence Relations, the last post of the series being GILA VI: The cycle index polynomials of the symmetric groups.

Usually, undergrads hardly think integrals have much to do with combinatorics. At A Portion of the Book, Masoud Zargar has a very nice post that deals with the intersection of Integrals, Combinatorics and Geometry.

Tom Escent submitted a link to an article titled, “Introduction to Nerds on Wall Street“, which actually provides a very small snapshot of the book named, Nerds on Wall Street: Math, Machines and Wired Markets whose author is David J. Leinweber. I haven’t read the book yet, but based on generally good reviews, it seems like it chronicles the contribution of Quant guys to Wall Street over the past several decades. Should be interesting to Math and CS majors, I think.

Let’s have a post on philosophy and logic, shall we? At Skeptic’s Play, there is a discussion on Gödel’s modal ontological argument regarding the possibility of existence of God. As someone who has just begun a self-study of modal logic, I will recommend Brian K. Chellas’ excellent introduction to the subject, titled Modal Logic: An Introduction.

Then, there is the Daily Integral, a blog dealing with solving elementary integrals and which I think may be particularly useful for high-school students.

Let me close this carnival by asking the reader, “What do you think is the world’s oldest mathematical artifact?” There are several candidates, and according to The Number Warrior, candidate #1 is The Lebombo Bone, found in the Lebombo Mountains of South Africa and Swaziland, that dates back to 35,000 BC!

That’s all for now! Thanks to everyone who made submissons.

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