Earlier quoted context omitted.
Not really. Even from a point of view of an experimenter with perfect information, the entropy of the system declines over time as fewer and fewer bits are needed to describe the system. For example, start with a Glas of warm water and an ice cube in it. Over time, the ice will melt and the range of different temperatures of the molecules decline. Consequently, you need fewer and fewer bits to describe the complete s…
Because ice is solid you can argue it takes less information because the particles aren't moving at all or in together in unison, so it will take less buts to encode. Furthermore, velocity is also a product of direction as much as speed, so if you take into consideration a solid object may vibrate it's particles in the same direction while a liquid can have it's particles in infinite directions, you're talking about…
It took me 10 years to understand entropy
111–120 of 295 posts
Re: It took me 10 years to understand entropy
#112Google freewall? Guess I won't read this article...
Nope.
Re: It took me 10 years to understand entropy
#113I don't understand entropy and this article did not change it. The issue I take is with the definition of "the most likely state". Think of a series of random bits that can be either 0 or 1 with equal probability. How likely is it that they are all 0 or all 1? Not very likely. There is exactly one configuration. How likely is it that they have a specific configuration of 0 and 1? Equally likely. All states are equall…
The purest mathematical justification for why low entropy means a low number of microstates probably comes from the fact that (classical) physical systems are a dynamical systems that preserve the measure induced by the standard metric of the phase space. The measure theoretic definition of entropy then implies the entropy of a partition of the phase space (i.e. a set of macrostates) is indeed the average of the logarithm of the number of microstates.
So indeed if W is the number of microstates in the current macrostate then entropy = log(W) (on average).
And using the typical set you can show that the probability that the average of log(W) over n samples is within 'epsilon' of the 'exact' entropy goes to 1 as n goes to infinity. This is the mathematical justification for the second law of thermodynamics.
The trick is that all of this is true no matter how you partition phase-space. Though that does mean that what is and isn't a high entropy state depends on your perspective.
Re: It took me 10 years to understand entropy
#114Earlier quoted context omitted.
> But if you look deeper than that averaging it stops making sense to me. It's a completely different world. I think you're less confused than you think you are! As I posted elsewhere, it helps to think of entropy as a quantity that actually depends on how much you know about the system in question. Typically when you calculate the entropy of a system at temperature X, that means all you know is that you stuck a ther…
Entropy (differences) are an objective quantity which can be measured, there is no subjectivity about it. It is not which parameters you know it is about which parameters you hold fixed.
Re: It took me 10 years to understand entropy
#115Re: It took me 10 years to understand entropy
#116I think the word entropy is science’s largest mistake.
My greatest concern was what to call it. I thought of calling it 'information,' but the word was overly used, so I decided to call it 'uncertainty.' When I discussed it with John von Neumann, he had a better idea. Von Neumann told me, 'You should call it entropy, for two reasons. In the first place your uncertainty function has been used in statistical mechanics under that name, so it already has a name. In the second place, and more important, no one really knows what entropy really is, so in a debate you will always have the advantage.'
Re: It took me 10 years to understand entropy
#117I think the word entropy is science’s largest mistake.
Shannon explained the name 'entropy' in (McIrvine and Tribus 1971): My greatest concern was what to call it. I thought of calling it 'information,' but the word was overly used, so I decided to call it 'uncertainty.' When I discussed it with John von Neumann, he had a better idea. Von Neumann told me, 'You should call it entropy, for two reasons. In the first place your uncertainty function has been used in statistic…
Re: It took me 10 years to understand entropy
#118Statistical mechanics is one way of representing entropy but you don’t need it. The second law of thermodynamics can be expressed in other much more general terms. Also it requires that the system be isolated not “thermally isolated”. There’s other types of interactions such as gravitational and electromagnetic.
I mean, come on. You know and I know that the statistical mechanics definition gets you 99% of the way there in terms of intuition. Obviously if I spin a rotor in my thermally insulated box with a magnet on the outside I can add energy to order things with, I don't think anyone is confused on that point.
Re: It took me 10 years to understand entropy
#119I don't understand entropy and this article did not change it. The issue I take is with the definition of "the most likely state". Think of a series of random bits that can be either 0 or 1 with equal probability. How likely is it that they are all 0 or all 1? Not very likely. There is exactly one configuration. How likely is it that they have a specific configuration of 0 and 1? Equally likely. All states are equall…