This piece reads to me like the output of someone who worked hard to comprehend a topic in full, without accepting the rest of society's cloudy bullshit / papered-over-confusion / historical baggage in place of answers. And in a particularly thorny case, no less. And with significant effort made to articulate the comprehension clearly and intuitively to others.
For instance: saying "if we're going to call all of these disparate concepts 'entropy', then let's call the length of the name of a microstate 'entropy' also; this will tie the whole conceptual framework together and make what follows more intuitive" is a bold move, and looks like the product of swallowing the whole topic and then digesting it down into something organized and comprehensible. It strikes me as a unit of conceptual labor.
Respect.
I'm excited to see where this goes.
I haven't read all of this yet. I like it so far. One nitpick: I would really try to avoid referring to individual microstates as having "entropy" assigned to them. I would call (or things playing a similar role) something else like "surprisal" or "information", and reserve entropy (rather than "average entropy") for things that look like or .
Of course, for macrostates/distributions with uniform probability, this works out to be equal to for every state in the macrostate, but I think the conceptual distinction is important.
(I'm as guilty as anyone of calling simple microstates "low-entropy", but I think it's healthier to reserve that for macrostates or distributions.)
From my perspective, the obvious rejoinder to "entropy is already two-place" is "insofar as entropy is two-place, cross-entropy is three-place!".
I think this is roughly where I'm at now.
After thinking a bit and peeking at Wikipedia, the situation seems to be:
The differential entropy of a probability density p is usually defined as
This is unfortunate, because it isn't invariant under coordinate transformations on x. A more principled (e.g. invariant) thing to write down, courtesy of Jaynes, is
where is a density function for some measure . We can also write this as
(Jaynes' continuous entropy of P with respect to )
in terms of a probability measure P with , which is a bit more clearly invariant.
Now we can define a cross-entropy-like thing as
(continuous cross-entropy of Q under P with respect to )
...and a small surprise is coming up. Jumping back to the discrete case, the KL divergence or "relative entropy" is
What happens when we try to write something analogous with our new continuous entropy ...
Curated. Came here to curate this and I think So8res's comment serves as good a curation notice as I might write myself:
...This piece reads to me like the output of someone who worked hard to comprehend a topic in full, without accepting the rest of society's cloudy bullshit / papered-over-confusion / historical baggage in place of answers. And in a particularly thorny case, no less. And with significant effort made to articulate the comprehension clearly and intuitively to others.
For instance: saying "if we're going to call all of these disparate concepts 'e
Thank you very much for writing this.
I have struggled with entropy since I first studied it in high school. I was taught that entropy measures "disorder" or the "chaos" in a system. I was totally disconcerted by the units (Joules/Kelvin), because I couldn't grasp it intuitively, the same way I could reason, for instance, about speed. I searched for a long time for an answer. Everything became much clearer (I remember this as a revelation) once I read "A farewell to Entropy", by Arieh Ben-Naim. According to the author, the only reason entropy is...
While I think this post overall gives good intuition for the subject, it also creates some needless confusion.
Your concept of "abstract entropy" is just Shannon entropy applied to uniform distributions. Introducing Shannon entropy directly, while slightly harder, gives you a bunch of the ideas in this post more or less "for free":
Macrostates are just events and microstates are atomic outcomes (as defined in probability theory). Any rules how the two relate to each other follow directly from the foundations of probability.
The fact that E[-log x] is th
Registering that I think "[entropy] can be used to explain the arrow of time" is bunk (I've linked 4:50, but see particularly the animation at 5:49): entropy works to explain the arrow of time only if we assume a low-entropy initial state (eg the big bang) in the past
Edit: Oh hm maybe the description isn't "time moves forward" but "time moves away from the big bang"
Is it important that negentropy be the result of subtracting from the maximum entropy? It seemed a sensible choice, up until it introduces infinities, and made every state's negentropy infinite. (And also that, if you subtract from 0, then two identical states should have the same negentropy, even in different systems. Unsure if that's useful, or harmful).
Though perhaps that's important for the noting that reducing an infinite system to a finite macrostate is an infinite reduction? I'm not sure if I understand how (or perhaps when?) that's more useful than...
Reading this piece about entropy as an abstract concept reminded me of a beautiful story touching on the topic: Exhalation by Ted Chiang (wikipedia page with spoilers).
Do you think it would be easier to solve the Diamond maximizer - Arbital problem if you were trying to maximize entropy instead of diamonds, due to entropy being more abstract and less dependent on specific ontology?
This is a very thought provoking post. As far as I understand, it is an attempt of finding a unified theory of entropy.
I admit I am still somewhat confused about this topic. This is partly because of my insufficient grasp of the material in this post, but, I think, also partly because you didn't yet went quite far enough with your unification.
One point is the thinking in terms of "states". A macrostate is said to be a set of microstates. As far as I understand, the important thing here is that all microstates are presumed to be mutually exclusive, such tha...
Excellent introduction. Your examples were all very intuitive.
For those who are reading, one way to get an intuition for the difference between binary strings and bits is to look at data compression. To begin with, it's easy to create a code like ASCII, where every character is represented by a binary string of length 8 (usually referred to as 8 "bits" or one byte), allowing up to unique characters. This type of code will allow you to represent a text document in English that's 1024 characters in length with exactly 1 kB of information.
Exc...
This post, and much of the following sequence, was greatly aided by feedback from the following people (among others): Lawrence Chan, Joanna Morningstar, John Wentworth, Samira Nedungadi, Aysja Johnson, Cody Wild, Jeremy Gillen, Ryan Kidd, Justis Mills and Jonathan Mustin. Illustrations by Anne Ore.
Introduction & motivation
In the course of researching optimization, I decided that I had to really understand what entropy is.^{[1]} But there are a lot of other reasons why the concept is worth studying:
I didn't intend to write a post about entropy when I started trying to understand it. But I found the existing resources (textbooks, Wikipedia, science explainers) so poor that it actually seems important to have a better one as a prerequisite for understanding optimization! One failure mode I was running into was that other resources tended only to be concerned about the application of the concept in their particular sub-domain. Here, I try to take on the task of synthesizing the abstract concept of entropy, to show what's so deep and fundamental about it. In future posts, I'll talk about things like:
Many people reading this will have some previous facts about entropy stored in their minds, and this can sometimes be disorienting when it's not yet clear how those facts are consistent with what I'm describing. You're welcome to skip ahead to the relevant parts and see if they're re-orienting; otherwise, if you can get through the whole explanation, I hope that it will eventually be addressed!
But also, please keep in mind that I'm not an expert in any of the relevant sub-fields. I've gotten feedback on this post from people who know more math & physics than I do, but at the end of the day, I'm just a rationalist trying to understand the world.
Abstract definition
Entropy is so fundamental because it applies far beyond our own specific universe, the one where something close to the standard model of physics and general relativity are true. It applies in any system with different states. If the system has dynamical laws, that is, rules for moving between the different states, then some version of the second law of thermodynamics is also relevant. But for now we're sticking with statics; the concept of entropy can be coherently defined for sets of states even in the absence of any "laws of physics" that cause the system to evolve between states. The example I keep in my head for this is a Rubik's Cube, which I'll elaborate on in a bit.
The entropy of a state is the number of bits you need to use to uniquely distinguish it.
Some useful things to note right away:
But after you agree on a strategy for uniquely distinguishing states, the entropy of said states becomes fixed relative to that strategy (and there are often clearly most-sensible strategies) and thus, in that sense, objective. And further, there are limits on how low entropy can go while still describing things in a way that actually distinguishes them; the subjectivity only goes so far.
Macrostates
I just defined entropy as a property of specific states, but in many contexts you don't care at all about specific states. There are a lot of reasons not to. Perhaps:
In cases like these, we only care about how many possible states there are to distinguish among.
Historically, the individual states are called microstates, and collections of microstates are called macrostates. Usually the macrostates are connotively characterized by a generalized property of the state, like "the average speed of the particles" (temperature). In theory, a macrostate could be any subset, but usually we will care about a particular subset for some reason, and that reason will be some macroscopically observable property.
Two basic strategies for distinguishing states
I would say that any method used to distinguish states forms a valid sub-type of entropy. But there are a couple really fundamental ones that are worth describing in detail. The first one I'll talk about is using finite binary strings to label each individual state. The second one is using yes/no questions to partition sets until you've identified your state. (Note that both these methods are defined in terms of sets of discrete states, so later I'll talk about what happens in continuous spaces. A lot of real-world states have real-valued parameters, and that requires special treatment.)
Binary string labels
In order to be able to say which of the possible states a system is in, there has to be some pre-existing way of referring to each individual state. That is, the states must have some kind of "labels". In order to have a label, you'll need some set of symbols, which you put in sequence. And it turns out that anything of interest to us here that could be done with a finite alphabet of symbols can also be done with an alphabet of only two symbols,^{[4]} so we will spend the whole rest of this sequence speaking in terms of binary.^{[5]}
It would be parsimonious to use the shortest descriptions first. Fewer symbols to process means faster processing, less space required to store the labels, et cetera. So we'll label our states starting from the shortest binary strings and working our way up.
Here's where we can see one way in which entropy is subjective. For any given set of states, there are many ways to give labels to the individual elements – you can always just swap the labels around. In contexts where quantities of entropy are treated as objective, that's because the context includes (explicitly or implicitly) chosen rules about how we're allowed to describe the states. On top of that, while you can swap labels, there are limits to how few bits we can use overall. You could always choose a state-labeling scheme that uses more bits, but there is a minimum average number of bits we can use to describe a certain number of states (i.e. the number we get by using the shortest strings first). Often, when talking about entropy, it's an implicit assumption that we're using a maximally efficient labeling.
Let's get a tiny bit more concrete by actually looking at the first several binary strings. The first string is the "empty" string, with no characters, which therefore has length 0. Next, there are only two strings which have a length of 1: the string 0 and the string 1. This means that, no matter what my system is, and no matter how many states it has, at most two states could be said to have an entropy of 1. There are twice as many strings with length 2: 00, 01, 10, and 11. Thus, there are (at most) four states that could be said to have entropy 2. For every +1 increase in entropy, there are twice as many states that could be assigned that entropy, because there are twice as many binary strings with that length.^{[6]}
I think it's easy for people to get the impression that the rarity of low-entropy states comes from something more complex or metaphysical, or is tied to the nature of our universe. But it turns out to be from this simple math thing. Low-entropy states are rare because short binary strings are rare.
To be more concrete, consider the Rubik's Cube. As you turn the faces of a Rubik's Cube, you change the position and orientation of the little sub-cubes. In this way, the whole cube could be considered to have different states. There's no law that dictates how the cube moves from one state to the next; you can turn the faces however you want, or not at all. So it's not a system with a time-evolution rule. Nonetheless, we can use the concept of entropy by assigning labels to the states.
Intuitively, one might say that the "solved" state of a Rubik's Cube is the most special one (to humans). Turning one side once yields a state that is slightly less special, but still pretty special. If you turn the sides randomly twenty times, then you almost certainly end up in a state that is random-looking, which is to say, not special at all. There are about 4.3⋅1019 possible Rubik's Cube states, and the log of that number is about 65.2^{[7]}. Thus, a random Rubik's Cube state takes about 65 bits to specify.^{[8]}
According to our above string-labeling, the solved state would have zero entropy. Similarly intuitively, almost-solved states would have almost-zero entropy. So if you turned one side a quarter turn, then maybe that state gets labeled with one bit of entropy. Perhaps we could carry on with this scheme, and label the states according to how many moves you need to restore the cube from that state to the solved state.^{[9]} There's nothing normative here; this just seems like a useful thing to do if you care about discussing how to solve a Rubik's Cube. You could always randomly assign binary strings to states. But we rarely want that; humans care a lot about patterns and regularities. And this is how entropy comes to be associated with the concept of "order". The only reason order is associated with low entropy is because ordered states are rare. The set of ordered states is just one particular set of states that is much smaller than the whole set. And because it's a smaller set, we can assign the (intrinsically rare) smallest strings to the states in that set, and thus they get assigned lower entropy.
You might object that ordered states are a very special set! I would agree, but the way in which they are special has nothing to do with this abstract entropy (nor with the second law). The way in which they are special is simply the reason why we care about them in the first place. These reasons, and the exact nature of what "order" even is, constitute a whole separate subtle field of math. I'll talk about this in a future post; I think that "order" is synonymous with Kolmogorov complexity. It's somewhat unfortunate how often entropy and order are conflated, because the concept of order can be really confusing, and that confusion bleeds into confusion about entropy. But it's also worth noting that any reasonable definition of order (for example, particles in a smaller box being more ordered than particles in a bigger box, or particles in a crystal being more ordered than particles in a gas) would be a consistent definition of entropy. You'd just be deciding to assign the shorter labels to those states, and states that are "ordered" in some other way (e.g. corresponding to the digits of π) wouldn't get shorter labels. But this is fine as long as you remain consistent with that labeling.
The binary string labeling scheme constitutes a form of absolute lower bound on average (or total) entropy. We can calculate that bound by summing the lengths of the first W binary strings and dividing by W.^{[10]} Let SW be the entropy of a set of W states, and let l(i) be the length of the ith binary string. Then the average is by definition
⟨SW⟩=∑Wi=0l(i)W.By looking at the above image of the first 31 binary strings, we can see that for W=2n−1,
W∑i=0l(i)=n−1∑l=02l⋅l,which is to say that you can sum all the lengths l(i) by breaking it up into terms of each length l times the number of strings of that length (2l). Next, it can be shown by induction that that sum has a closed form;
n−1∑l=02l⋅l=2n(n−1)−2n+2.Substituting back in n=log(W+1), dividing by W, and doing algebraic manipulation, we get that
⟨SW⟩≤log(W+1)−2+log(W+1)W.This is a very tight inequality. It's exact when W=2n−1, and ⟨SW⟩ is monotonic, and log grows very slowly.
The three terms are ordered by their big-O behavior. In the limit of large numbers of states, we really don't care about the smaller terms, and we use ⟨SW⟩=O(logW). Thus, the average entropy grows as the length of the longest strings in the set.
Yes/no questions
There's another very natural way we could use bits to distinguish one state from a set of states (especially when all the states are the same to us). This method is identical to the kids' game Guess Who?. In this game, you and your opponent each pick a person card from a fixed set of possible person cards. Then you try to guess which card your opponent has picked by asking yes-or-no questions about the person, like, "Do they have blonde hair?". You each have a board in front of you with copies of all the cards, so you can flip down the ones you've eliminated (which is highly satisfying). The way to minimize the expected number of questions you'll need to guess the person^{[11]} is to ask questions that eliminate half^{[12]} the remaining possible cards. If you start with W=2n cards, then this will require n questions, and therefore you'll use n bits of information to pinpoint a state, making your entropy equal to n=log(W). This is your entropy for every specific card; you never assign a card zero entropy.
This way of measuring entropy is usually more useful for macrostates, because typically we have a huge number of microstates in a macrostate, and we don't care about any of the individual ones, just how many there are. So to assign entropy to a microstate in this case, we just look at which macrostate it's in (e.g. check its temperature), calculate the number of possible microstates that are consistent with that macrostate, and take the log.
If a Rubik's Cube is in the macrostate of being one move away from solved, then (since there are 12 such (micro)states) according to the yes/no questions method of assigning entropy, that macrostate has an entropy of log(12)=3.58 bits. The number of microstates in the macrostate "one face is solved" is much, much higher, and so that macrostate has a much higher entropy. As we'll talk about in a later post, increased temperature means an increased number of possible microstates, so a higher-temperature object has higher entropy.
How they compare
You may notice that while the binary string model gives us O(logW) entropy, the yes/no question model gives us exactly log(W)^{[13]}. This reveals an underlying subtlety about our models. The label-assignment form of entropy is somewhat less than the binary questions form of entropy. Both are formalizations of the number of bits you need to describe something. But the question-answering thing seems like a pretty solidly optimal strategy; how could you possibly do it in fewer bits?
Imagine that the questions are fixed. For every state (e.g. Guess Who? card), the answers to the series of questions are just a list of yeses and nos, which is the same as a binary string. So each state could be said to be labeled with a binary string which is log(W) bits long. This is now just like our previous binary string strategy, except that setup uses the strings of all lengths up to log(W), and this one uses only strings of exactly length log(W).
The difference is that, if you had the states labeled with the shorter strings, and you were playing the game by asking a series of questions (equivalent to "Is the card's label's first bit 0?"), then you would sometimes reach the end of a binary string before you'd asked all log(W) questions. If the state happened to be the one labeled with just a 0, and your first question was, "Is the first bit a 0?" then the answer would be "yes" – but also, there would be further information, which is that there were no more bits left in the string. So in this formulation, that's equivalent to there being three pieces of information: "yes", "no" and "all done". If you were expecting only two possible answers, this could be considered a type of cheating, smuggling in extra information. It's as if all the finite binary strings need to have a special terminating character at the end.
So, the minimum average number of bits you need to distinguish a state depends on whether you're handed a whole label all at once (and know that's the whole label), or whether you need to query for the label one bit at a time (and figure out for yourself when you've received the whole label).
Exactly what is a bit?
In the opening definition of entropy, I used the word "bit", but didn't define it. Now that we've talked about cutting sets of states in half, it's a good time to pause and point out that that is what a bit is. It's often very natural and useful to think of bits as thing-like, i.e. of bits as existing, of there being a certain number of bits "in" something, or of them moving around through space. This is true in some cases, especially in computer storage, but it can be confusing because that's not really how it works in general.^{[14]} It's often not the case that the bits are somewhere specific, even though it feels like they're "in there", and that can contribute to them (and entropy) feeling elusive and mysterious.
For a state to "have" a bit "in" it just means that there was another way for that state to be (which it is not). If a state has a degree of freedom in it that has two possible values, then you can coherently think of the bit as being "in" that degree of freedom. But note that this relies on counterfactual alternatives; it is not inherently inside the specific state.
Concretely, a state could have a simple switch in it (or a particle with up or down spin, or an object which could be in either of two boxes). If half of the entire set of possible states has the switch on, and the other half has the switch off, then I think it's fair to say that the bit is in the switch, or that the switch is one bit of entropy (or information). However, if 99% of states have the switch on and 1% have it off, then it contains significantly less than one bit, and if all states have the switch on, then it is zero bits.
As a simple example of a bit not being clearly located, consider a system that is just a bunch of balls in a box, where the set of possible states is just different numbers of balls. One way to divide up the state space is between states with an even number of balls versus states with an odd number of balls. This divides the state space in half, and that constitutes a bit of information that does not reside somewhere specific; it can be "flipped" by removing any single ball.
Thus, you can also see that just because you've defined a bit somewhere, it doesn't mean that feature must represent a bit. Though the quantity "the number of times you can cut the state space in half" is an objective property of a state space, the exact ways that you cut the space in half are arbitrary. So just because your state contains a switch that could be flipped does not mean that the switch must represent a bit.
Probabilities over states
In all of the above discussion of average entropies, we implicitly treated the states as equally likely. This is not always true, and it's also a problematic premise if there are infinitely many states. If you want to get the average entropy when some states are more likely than others, then you can just take a standard expected value:
E[SX]=∑x∈Xp(x)S(x).Here, S is our entropy, X is the set of possible states x, and p(x) is the probability of each state. If p is uniform and the size of X is W, then the minimum average entropy is the thing we already calculated above. If p is not uniform, then the best thing we could do is give the most likely states the shortest strings, which could give us an average entropy that is arbitrarily small (depending on how non-uniform p is).
That's what we could do in the binary string labels model. But what about in the yes/no questions model? What if, for example, we know that our friend likes picking the "Susan" card more often? If the cards aren't equally likely, then we shouldn't just be picking questions that cut the remaining number of cards in half; instead we should be picking questions that cut the remaining probability mass in half. So, if we know our friend picks Susan half the time, then a very reasonable first question would be, "Is your card Susan?".
But now our labels are not the same lengths. This feels like it's bringing us back to the binary string model; if they're not the same length, how do we know when we've asked enough questions? Don't we need an "end of string" character again? But a subtle difference remains. In the binary string model, the string 0 and the string 1 both refer to specific states. But in our game of Guess Who?, the first bit of all the strings refers to the answer to the question, "Is your card Susan?". If the answer is yes, then that state (the Susan card) just gets the string 1. If the answer is no, then the first bit of all the remaining states (i.e. the non-Susan cards) is 0 – but there's a second question for all of them, and therefore a second bit. No card has the string that is just 0.
The generalization here is that, in the yes/no questions model, no binary string label of a state can be a prefix of another state's binary string label. If 1 is a state's whole label, then no other label can even start with a 1. (In the version of the game where all states are equally likely, we just use equally-sized strings for all of them, and it is the case that no string can be a prefix of a different string of the same size.)
This is how you can use different-sized labels without having an additional "all done" symbol. If the bits known so far match a whole label, then they are not a prefix of any other label. Therefore they could not match any other label, and so you know the bits must refer to the label they already match so far. And using different-sized labels in your "prefix code" lets you reduce your expected entropy in cases where the states are not equally likely.
There are infinitely many prefix codes that one could make (each of which could have finitely or infinitely many finite binary strings).^{[15]} It turns out that for a given probability distribution p(x) over states, the encoding that minimizes average entropy uses strings that have one bit for every halving that it takes to get to p(x) (e.g. if p(x)=14, that's two halvings, so use two bits to encode the state x). In other words we can use labels such that
S(x)=log1p(x),and therefore,
E[SX]=∑x∈Xp(x)log1p(x),which is minimal. (This is also how we can assign an entropy to a macrostate of unequally-likely microstates; we still want it to represent the number of yes/no questions we'd have to ask to get to a specific microstate, only now it has to be an expected value, and not an exact number.)
This definition, formally equivalent to Shannon entropy and Gibbs entropy, is often considered canonical, so it's worth taking a step back and reminding ourselves how it compares to what else we've talked about. In the beginning, we had a set of equally-likely states, and we gave the ones we "liked" shorter binary string labels so they required fewer bits to refer to. Next, we had sets of equally likely states that we didn't care to distinguish among, and we gave them all equally long labels, and just cared about how many bits were needed to narrow down to one state. Here, we have unequally-likely states, and we're assigning them prefix-codes in relation to their probability, so that we can minimize the expected number of bits we need to describe a state from the distribution.
All of these are ways of using bits to uniquely distinguish states, and thus they are all types of entropy.
Negentropy
Negentropy is the "potential" for the state (micro or macro) to be higher entropy – literally the maximum entropy minus the state's entropy:^{[16]}
J(x)=Smax−S(x).Note that while the entropy of a state is something you can determine from (a labeling of) just that state, the negentropy is a function of the maximum possible entropy state, and so it's determined by the entire collection of states in the system. If you have two systems, A and B, where the only difference is that B has twice as many states as A, then any state in both systems will have one more bit of negentropy in system B (even though they have the same entropy in both systems).
When we have a finite number of states, then Smax is just some specific binary string length. But for systems with an infinite number of states (and thus no bound on how long their labels are), Smax is infinite, and since S(x) is finite for every state x, every specific state just does actually have infinite negentropy.
If we're using entropy as the number of yes/no questions, and all the states are equally likely, then they all have equal entropy, and therefore zero negentropy. If they have different probabilities and we've assigned them labels with a prefix code, then we're back to having a different maximum length to subtract from.
If we're considering the entropy of a macrostate, then what is the maximum "possible" entropy? I'd say that the maximum entropy macrostate is the whole set of states.^{[17]} Therefore the negentropy of a macrostate M is how many halvings it takes to get from the whole set of states to M.
If the system has an infinite number of microstates, then a macrostate could have finite or infinite negentropy; a macrostate made of a finite number of microstates would have infinite negentropy, but a macrostate that was, say, one-quarter of the total (infinite) set of states would have a negentropy of 2. As above, if the states are not equally likely, then the generalization of macrostate negentropy is not in terms of number of microstates but instead their probability mass. Then, the negentropy of a macrostate M is
J(M)=log1p(M).One concrete example of negentropy would be a partially-scrambled Rubik's Cube. Using the distance-from-solved entropy discussed above, a cube that is merely 10 moves from solved is far from the maximum entropy of 26 moves from solved, and thus has large negentropy.
Another example shows that negentropy could be considered the potential bits of information you could store in the state than you currently are. If your file is 3 KB in size, but can be losslessly compressed to 1 KB, then your file has about 1 KB of entropy and 2 KB of negentropy (because the highest-entropy file you can store in that space is an incompressible 3 KB).
What's next
At the risk of over-emphasizing, all the above is (if my understanding is correct) the definition of entropy, the very source of its meaningfulness. Any other things that use the term "entropy", or are associated with it, do so because they come from the above ideas. In a future post I try to trace out very explicitly how that works for several named types of entropy. In addition, we will show how these ideas can meaningfully carry over to systems with continuous state spaces, and also consider moving between states over time, which will allow us to work out other implications following directly from the abstract definition.
The quickest gloss is that optimization is a decrease in entropy. So it's a pretty tight connection! But those six words are hiding innumerable subtleties.
Something like "the entropy of a closed system tends to increase over time"; there are many formulations.
Some contexts will use "nats" or "dits" or whatever. This comes from using logarithms with different bases, and is just a change of units, like meters versus feet.
I've justified the use of binary before. There's a lot of interesting detail to go into about what changes when you use three symbols or more, but all of the heavy-lifting conclusions are the same. Turing machines that use three symbols can compute exactly the set of things that Turing machines with two symbols can; the length of a number n is O(logn) whether it's represented in binary or trinary; et cetera.
Binary strings are usually written out with 0s and 1s, and I'll do that in the text. But I personally always visualize them as strings of little white and black squares, which is what I'll use in the illustrations. This is probably because I first learned about them in the context of Turing machines with tapes.
Note that the entropy of a state is the length of its label, and not the label itself; the specific layout of 0s and 1s just serves to distinguish that label from other labels of the same length.
Justification for merely taking the log comes from the derivation at the end of this section, though you may have been able to intuit it already!
Again, this is assuming you're using a binary string labeling scheme that uses all the smaller strings before using bigger strings. You could always decide to label every state with binary strings of length 100.
The typical minimal notation for describing Rubik's Cube algorithms has one letter for each of the six faces (F, B, L, R, U, D), and then an apostrophe for denoting counter-clockwise (and a number of other symbols for more compact representations). This means that six of the one-move states have a label of length one, and six others have length two. This all comes out in the big-O wash, and the label lengths will end up differing by a constant factor, because e.g. log6(x)=log2(x)log2(6)=0.387⋅log2(x).
I'll have bits of math throughout this sequence. This is a pretty math-heavy concept, but I still don't think that most of the actual equations are essential for gaining a useful understanding of entropy (though it is essential to understand how logarithms work). So if you feel disinclined to follow the derivations, I'd still encourage you to continue reading the prose.
None of the derivations in this sequence are here for the purpose of rigorously proving anything, and I've tried to include them when the structure of the equations actually helped me understand the concepts more clearly.
Wikipedia informs me that this is not technically the optimal strategy for winning the game, because if you are behind and your opponent plays optimally, then you're better off guessing specific people and hoping to get lucky.
Or as close to half as you can get.
Again, only exact when W is a power of 2, but in any case, the binary string one is strictly less than the yes/no questions one, which is what we want to resolve here.
For this reason I've been careful not to use the phrase "bit string", instead sticking with "binary string". For our purposes, a binary string is a bit string if each of those symbols could have been the flipped value (for some relevant definition of "could").
Examples of finite prefix codes: {0, 1}, {0, 10, 11}, {00, 01, 10, 110, 1110, 1111}
Example of an infinite prefix code: {0, 10, 110, 1110, 11110, ... }
Note that for many systems, most states have maximum or near-maximum entropy, such that the negentropy is virtually the same as the average entropy minus the state's entropy; this would also mean that most states have virtually zero negentropy.
You could argue that the maximum entropy macrostate is just the macrostate that contains only the highest entropy state(s). I think the spirit of macrostates is that you don't consider individual states, and thus it would be "cheating" to pick out specific states to form your macrostate. In the spirit of S=log(W), the way to maximize S is to maximize W, that is, include all states into W.