An exploration of theoretical physics, for those who are not necessarily PhDs, but who don't want their physics dumbed-down.
Wednesday, June 13, 2012
The Nature of information III
In this posting I explore the probability of finding strings and establish the principle that the chace of finding a given string is independent from the elements of the string. This result is called the Asymptotic Equipartition Property. For details go to the The Nature of Information III
Friday, June 1, 2012
New place for formatted information theory.
Due to the difficulty in placing the mathematical symbols into the blog, I will encapsulate the post and provide a link to the formatted version.
In general these will be located at: http://www.madscitech.org/csg/it.html.
In general these will be located at: http://www.madscitech.org/csg/it.html.
Tuesday, May 22, 2012
The Nature of Information II
The Nature of Information II
George Hrabovsky
MAST
Introduction
The previous article was concerned primary with a sequences of events that were mutually exclusive. What happens when more than one such sequence, or scheme, are combined?
Combining Schemes—Mutually Independent Sets
Let’s say that we have two finite schemes,
and
Say that the propbability of the joint occurence of events
and
is
This property is called a mutually independent probability. In fact the set of events
forms another finite scheme. The entropy for such a scheme is,
Combining Schemes—Mutually Dependent Sets
So what if A and B are not mutually independent? Here we say that the probability of event
of the scheme B occurs assuming that event
occurs from scheme A is
of the scheme B occurs assuming that event
occurs from scheme A is
This gives us the scheme
with entropy
It turns out that
is a random variable called the expectation of H(B) in the scheme A. It is also written
is a random variable called the expectation of H(B) in the scheme A. It is also written
What does It all Mean?
The amount of information delivered by a scheme never decreases unless a another scheme is realized beforehand.
Friday, May 18, 2012
The Nature of information
The Nature of Information
George Hrabovsky
MAST
Introduction
Information can be thought of as what we do not already know. We acquire information when we learn, or perhaps it is that the act of learning is acquiring information. In either case we can consider infomration in the abstract to be a phsycial quantity and it can be measured.
Bits
How do we measure information? Like any measurement of a physical quantity we choose a fundamental unit. Then we say that something has a quantity of units, a numerical result. Something can be five meters long, or it can be 4.3 pounds of weight, or 6.1 kilograms of mass, and so on. For information we use the bit as a fundamental quantity. Thus we can say that some information is composed of a number of bits.
Characterizing Information
We will use symbols to represent bits of information. A set of symbols comprising a single bit will be represented by
two bits by
and so on, so that a set of n such symbols is the sequence
.
Schemes
If we also associate a probability that a given symbol will be sent,
The symbols of such a set must be mutually exclusive, so that the total of all probabilies is 1. We can combine them into a single symbol,
This is called a finite scheme.
Entropy
Entropy is, among other things, the measure of the disorder of a system of symbols. In the case of a scheme the entropy is given by,
We will discuss these things in more detail later.
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