posted by tomkirbygreen

]]>C

posted by Charles

]]>posted by ShinNoNoir

]]>posted by Richard.Hein

]]>Must repeat the first episodes.

A great show as usual folks.

And: category theorists, show yourselves!

It's a pretty fun concept: real-time* theoretical investigation.

Well, it was real at the time

posted by exoteric

]]>I think there is no correspondence between this particular programming and physics sample. Let me explain why.

Programming sample:

We have functions f and g and we are exploring what happens to their composition after applying Select functor.

Here are our types:

f :: B -> C

Select :: IEnumerable<a> -> IEnumerable<b> -- maybe it should say (a->IE<a>)->(b->IE<b>), but I wanted to capture the essence

xs :: A -> IEnumerable<A> -- lets assume xs is a monadic constructor or how that thing was called

Composition (f o g) under Select...

And our covariance...*xs.Select(x => g(x)) **-- gives us IEnumerable<B>** **(or B->IE<B>)** .Select(x => f(x)) **-- gives us IEnumerable<C> **(or C->IE<C>)*

Notice that we are always in IEnumerable<a> monad.

-------------------------------------------

Now, to the physics sample:

There is our manifold P and its coordinatization (hope I spelled it right) cx which goes to our coordinate system {X} (cx: P->{X}). In the programming example image of cx would be equivalent to xs, P would be A, and {X} would be IEnumberable<A>.

Let's denote the image of cx as {X}<P>.

Now, the physics example's covariance and contravariance was about dealing with how functions p and f behave under changing the coordinate system (let's call it ToY:{X}->{Y} and ToX:{Y}->{X}).

-------------------------------------------

But going from {X}<P> to {Y}<P> is fundamentally different than going from IEnumerable<A> to IEnumberable<B> (which is happening in our example). Going from {X}<P> to {Y}<P> is more like (in my opinion) going from IEnumberable<A> to IObservable<A>.

In the physics sample we have transformations ToY :: {X} -> {Y} and ToX :: {Y} -> {X}. In the programming world we have ToObservable() (~ ToY) and ToEnumerable() (~ ToX). And what you can then explore is how certain functions behave under (after applying) ToObservable()
and ToEnumberable(). Unfortunately in this programming example with Select there is no direct correspondence between programming's f and g, and physic's p and f (because in physics P is A. Then we can say that T is B and F is C. Then g_{programming} = p^(-1)
and f_{programming} = ?). At this moment no example comes into my mind. But...

...the fundametal question is: **Why do we want to change coordinate systems in physics? **

I am no physicist, but I believe that the answer is that because sometimes it's easier to calculate stuff in system {Y} instead of in system {X}.

Well, and why do we want to change from IEnumerable to IObservable - because it's better to do some stuff in IO than in IE.

Now this, I think, is a really beautiful and fundamental corrspondence.

-------------------------------------------

Of course might be completely wrong, just wanted to share my 2 cents

posted by Kyrae

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Now that the squiggly arrow from T to {x} is reversed, I’m curious why the straight arrows only have to go from T -> P -> F where they should be able to be T <-> P <-> F (Given fuel burn rate and 2 Position calc the Time you get there) which I think should solve:

C(t) =

C(P->T)=

C((P~>{x})->({x}~>T))=

C(P)->C(T)=

Which would now make both calcs co-variant?

posted by N2Cheval

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Love this!

C

posted by Charles

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Monad. Monad. Monad.

C

posted by Charles

]]>posted by brianbec

]]>posted by brianbec

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FG :: (F A -> F B) -> (G A -> G B)

then you don't need different types of arrows. you can just traverse the blue & green graphs by composing lists of those "monad transformers" ??

posted by Spongman

]]>

But I really think the important thing is going from {X} to {Y} and back as going from IE to IO.

posted by Kyrae

]]>posted by Kyrae

]]>I think that we should operate not on values but on functions, and there should be different type constructors when we're talking about time and fuel.

Something like this, e.g. for fuel CF<P,C(P)> = (P -> F) -> (C(P) -> F) .

Values of such types should describe how function from position to fuel changes when we switch coordinate system from P to C(P)

And then we should prove that corresponding functor is co-variant.

Or, probably that's overcomplicated. Maybe type constructor CF<P> = P -> F is sufficient. Then to define functor we need mapping CF:: P -> (P -> F) that is for each coordinate system we should have function from position to fuel. And then we need to show that CF:: (P -> CP) -> ((P->F) -> (CP->F)) is co-variant functor. Hm, type parameter P is in input position. There should be contra-variance then.

posted by Gregory81

]]>posted by staceyw

]]>

In time, grasshopper.

C

posted by Charles

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I think that what maybe needed is a "coordinization" which takes coordinates from {x} to coordinates in {y} that is to say a functor which takes the function of a->b to a function using their coordinates in x and y. (Otherwise the coordinatization of T and F both to the same coordinate system will obviously just give exactly the same coordinates.)

Roughly speaking...

(function) TimeToFuel= T->F

(function) XcoordsOfTimeToYcoordsOfFuel = xCoordFromTime(T)->yCoordFromFuel(F) = xToYFunctor[ T->F ]

then also the reverse: timeToFuelFunctor[ x->y] = timeFromXCoord(T) -> fuelFromYCoord(F)

The coordinization in your video (C) would here be the xToYFunctor.

Something like that anyway.

In code it might be(???) wildy guessing here:

complexVectorToPolarArray = Vector<complex> --> Array<polar> = vectorToArray[ complex->polar ]

I give up.

posted by zoobar

]]>

I think the diagram doesn't serve you well. How I visualise it would be more like a childs pivoting see-saw. (Can't seem to get a image to insert here.) Where T is on the left end of the horizontal bar and F is on the right and P is an equilateral triange pivot in the middle. So a change in T are two end points in the y-axis and change in F are the same on the right. (think vertical up and down double ended arrows) The change in P though are the two end points of the bottom side of the triangle. (so bigger distance = bigger triangle.)

So with that in mind, covarince would be same change in the y-axis of both T and F due to the change in the height of P (ie. the shorter the distance reduces the time and fuel burn in the same vertical direction) and contravariance would be keeping the same distance P but changing the fuel burn F (or time when you get fast enough) to inversely change time T.

I hope that makes sense. Now to think of how to display the functional code for it... maybe my part 3?!?

posted by N2Cheval

]]>I would have to agree that the "coordinization" of P to {x} feels a lot like the case of going from T to IEnumerable<T>. The only problem is that it may be from a collection of instances of T not the actual class of T itself.

P is a set of landmarks, which is ordered, discrete, and cannot be used for calculating differentials or integrals. You can however convert each member of P into a LatLongAlt coordinate representation and then fill in the gaps between point
using a path approximation function. The path approximation function lets you turn a discrete list of landmarks into a continuous infinite set of points that can be used for calculations.

In the programming world T represents a Class, not a set of instances of that class. Once you have a set of ordered, distinct instances of T you could use an IEnumerable to go from the distinct set to a continuous set where interim results
between distinct points are calculated using some predefined function that takes the previous and next discrete instances of T as it's input parameters and produces an estimated output value between the to points. The problem is that {x} is an infinite set/function
based on time where as IEnumerable is a bounded set with fixed increments of time (ie: each call to Next() corresponds to 1 second)

The part that still confuses me is Erik's remark about "Operations on non-coordinated things" and "Operations on coordinated things" being commutable. The coordinated things simply means you have a value (real or computed) for all inputs,
which basically means the IEnumerable would always return a value when calling Next() and would never throw an exception. But what is the correlation for operations on non-coordinated (discrete) things in programing? The only operations I could think of are
type casting, which take a T and return a new type. If so then you are looking for an operation in physics that takes P and turns it into something else. Does P -> F count?

I would have to agree that the "coordinization" of P to {x} feels a lot like the case of going from T to IEnumerable<T>. It may however be from a collection of instances of T not the actual class of T itself. P is a set of landmarks, not the definition or "class type" of a landmark. This is easier to see for the other two sets which have well defined class types, such as F which is a set of real numbers corresponding to fuel consumption (ie: contains instances of the real number class)

P is a set of landmarks, which is ordered, discrete, and cannot be used for calculating differentials or integrals. You can however convert each member of P into a LatLongAlt coordinate representation and then fill in the gaps between points using a path approximation function. The path approximation function lets you turn a discrete list of landmarks into a continuous infinite set of points that can be used for calculations.

In the programming world T represents a Class, not a set of instances of that class. I guess you could view T as the abstract set of all possible instances of T, but that would really be comparable to the domain of all landmarks not the set of specific landmarks described by P in the example. Once you have a set of ordered, distinct instances of T you could use an IEnumerable to go from the distinct set to a continuous set where interim results between distinct points are calculated using some predefined function that takes the previous and next discrete instances of T as it's input parameters and produces an estimated output value between the to points. The problem is that {x} is an infinite set/function based on time where as IEnumerable is a bounded set with fixed increments of time (ie: each call to Next() corresponds to 1 second). You would end up with something like:

var x =PositionFromTime(t); if(x != null){ if(x == EndPosition){ return PositionToCord(x); } else { yield return PositionToCord(x); } } else { yield return ComputeCord(LastPosition, NextPosition, tFromLastPosition); }

The part that still confuses me is Erik's remark about "Operations on non-coordinated things" and "Operations on coordinated things" being commutable. The "coordinated things" simply means you have a value (real or computed) for all inputs, which basically means the IEnumerable would always return a value when calling Next() and would never throw an exception. But what is the correlation for operations on non-coordinated things (discrete instance) in programing? The only operations I could think of are type casting, which take a T and return a new type. If so then you are looking for an operation in physics that takes P and turns it into something else. Does P -> F count?

Maybe someone should post this to MathOverflow.net and see if they can come up with anything

posted by gbrayut

]]>1) similarity of definitions of co- and contravariance in physics and programming

2) similarity of coordinatization to going to Monad

It should be possible to prove first without considering second. When we do Select on IEnumerable<> we're allowed to change type of element. Coordinatization might be treated similarly to such type change.

If we're talking about second then we probably need to take into account not only coordinatization of positions but also linear approximation needed to make continuous versions of
*f* and *p.*

posted by Gregory81

]]>I've been watching C9 for a long time and a big fan.

if possible, waiting for another E2E with other field area to discuss ( who knows what will get out !?!?! )

posted by LD

]]>I suspect that the "key" of the Beckman category is in the physical domain.

At first sight, the properties of this category seem similar to the Wave/Particle duality (http://en.wikipedia.org/wiki/Wave–particle_duality)

The key => particles are "enumerable" and waves are "observable".

Both domains (the Schrodinger domain for particle and Maxwell for waves) are using the "curl" operator but in a dual (and not compatible) way.__In the physical domain__

The only things what we know on a (long living) particle is his space-coordinate (http://en.wikipedia.org/wiki/Identity_of_indiscernibles and http://en.wikipedia.org/wiki/Indistinguishable_particles) =>

coordinization (first sense) = "position enumeration"

In the "wave domain" the referential are transparent (time relative) => the wave doesn't have a local position-state but only a timing (for wave events such wave absorption and wave emission).

=> the root observer is the type "T" (the basic observation = computer clock = now and everywhere)

(composing observers = dividing the clock)

=> the root enumerator is the type "P" (the basic enumeration = here and every time)

(composing enumerator = filling the memory)

The flight path permits to convert "locally" the type T and P and F (but not globally)

posted by paxal

]]>

So now we want to express this idea in terms of functions and types. Following Brian’s idea that “coordinitization” is the functor in this problem:

public class Vector { }

public delegate double[] ToCoords<in TBasis>(Vector vector, TBasis basis);

Here Vector is the type for coordinate-free vectors, and ToCoords maps a vector to a set of vector coordinates given a vector basis (i.e. a coordinate system). This delegate type is contravariant in both the basis and vector arguments.

Now suppose we have a ToCoords<A> for a certain vector basis A. What happens if we apply a transformation from basis A to basis B? We want to compute ToCoords<B> in order to obtain vector coordinates for the new basis. Here’s how ToCoords changes with a change in basis:

public static ToCoords<B> TransformCoords<A, B>(this ToCoords<A> toCoordsA, Func<B, A> basisB2A)

{

return (vector, basis_b) => toCoordsA(vector, basisB2A(basis_b));

}

Notice that in order to go from a ToCoords<A> to a ToCoords<B> we need a function from basis B to basis A. This is the inverse of the A -> B transformation we applied to start things off.

Now suppose we apply two transformations in a row, one from A to B and then one from B to C. In order to “back out” the change to the vector coordinates, we need to apply the inverse transformations in reverse order. So the following two expressions are equivalent:

ToCoords<C> tcc1 = tca.TransformCoords<A, C>(x => f(g(x)));

ToCoords<C> tcc2 = tca.TransformCoords(f).TransformCoords(g);

This is the opposite behaviour under composition to that of Enumerable.Select that Erik gave in the video, since Select is covariant in T and ToCoords is contravariant in TBasis.

Now there are some more “exotic” things in physics that are covariant with respect to a change in basis. They are called variously covectors, pseudovectors, dual vectors, row vectors, bivectors (my personal favourite), or even “linear functionals”. The last of these is probably the easiest to explain.

A linear functional is a function that takes a set of vector coordinates and returns a scalar (a number) through a process that looks a lot like a dot product of vectors. It’s easier to explain in code:

public delegate double LinearFunctional<out TBasis>(Vector vector, ToCoords<TBasis> toCoords);

public static LinearFunctional<TBasis> CreateLinearFunctional<TBasis>(TBasis basis, double[] coords)

{

return (vector, toCoords) => toCoords(vector, basis).Zip(coords, (x, y) => x * y).Sum();

}

Instead of providing the linear functional with a set of vector coordinates to operate on, I provided a vector and a way of getting coordinates from the vector in the form of a ToCoords delegate.

Notice that LinearFunctional is covariant in TBasis (i.e. <out TBasis>). This is due to the fact that ToCoords is <in TBasis> and I’m passing one in. Somehow two ins make an out. Maybe Erik can explain that...

So what happens to LinearFunctional<A> under a basis change from A to B? This one writes itself:

public static LinearFunctional<B> TransformLinearFunctional<A, B>(this LinearFunctional<A> lfa, Func<A, B> basisA2B)

{

return (vector, toCoords) => lfa(vector, TransformCoords(toCoords, basisA2B));

}

In order to go from a LinearFunctional<A> to a LinearFunctional<B> we need a function from A to B. This is the opposite of ToCoords. The behaviour under composition is also opposite to ToCoords (and the same as Select). The following expressions are equivalent:

LinearFunctional<C> lfc1 = lfa.TransformLinearFunctional(x => g(f(x)));

LinearFunctional<C> lfc2 = lfa.TransformLinearFunctional(f).TransformLinearFunctional(g);

Now once you get to tensors you can get even more exotic things that have both covariant and contravariant parts. I suspect this is the kind of thing Brian was trying to work with.

What have I missed? Is this too simplistic?

Steve.

posted by SC Taylor

]]>

May it be that we are missign the coordinization of TIME and FUEL?

Let's make more simple:

10:00 AM : LONDON

11:00 AM : PARIS

12:AM : ROME

In this case TIME is not a "continous variable", it's discrete.

So, to be able to move to algebra to make calculus we need a function to move TIME frome discrete to continous, as we did with the POSTISIONS (cities).

EDIT: to clarify. TIME in the timesheet is only a set of values. We can call them TIME_A, TIME_B, TIME_C. We need to apply a coordinization to TIME and FUEL as well. I think that the misleading is that that function is identity.

So to answer Erik question:

F :: (A -> B) -> (FA -> FB)

i think A -> B is the lookup table itself.

Then FA -> FB is the function that allows to compute position from time in the algebric way.

In this way F, the coordinization, should be well defined.

P.S.: sorry if i mispelled somthing, but is the first time ever that i talk math in english

P.S.S.: sorry if i wrote a lot of rubbish.

posted by bonfo

]]>posted by ProtoBytes

]]>I tried to come up with some comparable examples in code. We have already seen covariance in the shows, but I think what I believe is a contrvariant example is interesting because it has a pattern similar to the physics examples.

// Here is a simple select to get the fuel spent

fuelUsed = times.Select(ToLatLon).Select(FuelSpentAt);

// Now suppose the function we have the get the fuel spent needs XYZ

// then we can compose FuelSpentAt with ToXYZ

fuelUsed = times.Select(ToLatLon).Select(latLon => FuelSpentAt(ToXYZ(latLon)));

// Now if we separate the composition we see it is covariant (yes this was already covered)

fuelUsed = times.Select(ToLatLon).Select(ToXYZ).Select(FuelSpentAt);

// FuelSpentAt • ToXYZ • ToLatLon

IEnumerable<XYZ> orderedXYZs;//IEnumerable<LatLon> orderedLatLon;

// Now lets say we want to get the XYZs ordered by the rate that fuel was being consumed at that point. This is pretty straight forward with a function that takes XYZ and returns a rate.

orderedXYZs = times.Select(ToXYZ).OrderBy(FuelRateAt);

// Suppose though we only have a FuelRateAt function that takes LatLon in this case we can compose ToLatLon with FuelRateAt inside the OrderBy

orderedXYZs = times.Select(ToXYZ).OrderBy(xyz => FuelRateAt(ToLatLon(xyz)));

// If we separate the composition we get the following. Now I beliebe OrderBy is contravariant since IComparable is contravariant, but I might be wrong. But the interesting thing is that this pattern is like the pattern Brian Beckman had in the physics example

orderedXYZs = times.Select(ToXYZ).Select(ToLatLon).OrderBy(FuelRateAt).Select(ToXYZ);

// ToXYZ • FuelRateAt • ToLatLon • ToXYZ

// Note the inverse (ToXYZ) is composed to the left of the FuelRateAt function

posted by Its_Bryan

]]>https://twitter.com/TopologyFact/status/944239945148960773

posted by Brian Beckman

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