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&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&lt;br /&gt;
cobaltfjord@aol.com (CobaltFjord) wrote in message news:&amp;lt;b21nju$t59$1@panther.uwo.ca&amp;gt;...&lt;br /&gt;
&lt;br /&gt;
I will respond in the order of importance&lt;br /&gt;
&amp;gt; High entropy randomness is not the same kind of&lt;br /&gt;
&amp;gt; randomness as QM randomness, right?  What is&lt;br /&gt;
&amp;gt; the difference?&lt;br /&gt;
&amp;gt;&lt;br /&gt;
No.  Classical randomness is not the same as quantum randomness.&lt;br /&gt;
&lt;br /&gt;
Roughly speaking, classical randomness is a way to account for the unknown  input variables.&lt;br /&gt;
&lt;br /&gt;
For example, classically,  you are 100% allowed to keep track of the particles in a gas.  It&amp;#039;s just it is easier to deal with them if you catagorize them random.&lt;br /&gt;
&lt;br /&gt;
For example, think of rolling a ball down the valley. Classically, the more and more you can account for every ups and downs and friction of the cliff, you may be able to predict the &amp;#039;exact&amp;#039; position where the ball is going to fall.&lt;br /&gt;
&lt;br /&gt;
On the other hand, you can choose a model of the valley by choosing a probabilitistic model of the distribution of the bumps. From that model, you will be to calculate, the average position where the ball stops and the probability that it lands x distance away from that average position.&lt;br /&gt;
&lt;br /&gt;
On the other hand, quantum mechanically, no matter, how hard you try, you will never know all properties of the particle exactly. This knowledge is forbidden by the uncertainty principle. In a way, even though you may be able to build powerful instruments or powerful computational devices, you will never know what will &amp;#039;exactly&amp;#039; happen in the next instant.&lt;br /&gt;
&lt;br /&gt;
&amp;gt; Couldn&amp;#039;t we predict motion of a single molecule over&lt;br /&gt;
&amp;gt; some arbitrarily small distance, over some arbitrarily&lt;br /&gt;
&amp;gt; small time period?&lt;br /&gt;
Within the classical paradigm, this is possible. However,  quantum mechanics tells you this cannot be done.&lt;br /&gt;
&lt;br /&gt;
&amp;gt; Do molecules in Brownian Motion take a 100% random&lt;br /&gt;
&amp;gt; walk, or is their motion just causal, but unpredictable,&lt;br /&gt;
&amp;gt; deterministic chaos?&lt;br /&gt;
Chaos is a good word to describe it. Deterministic systems can also behave compeletely chaotically.&lt;br /&gt;
&lt;br /&gt;
An example is Windows 98. Since Windows 98 runs a computer, the flow of the program is determinstic. However, it does &amp;#039;randomly&amp;#039; crash from time to time for &amp;#039;unknown&amp;#039; reasons. It is possible, that with enough variables, you can figure out when it is going to crash. However, it is easier to model it as a random system ;-)&lt;br /&gt;
&lt;br /&gt;
&amp;gt;&lt;br /&gt;
&amp;gt; Don&amp;#039;t molecules in a liquid or a gas move as a result&lt;br /&gt;
&amp;gt; of the forces they encounter?  Or do they move, as if&lt;br /&gt;
&amp;gt; Newton&amp;#039;s First and Second Laws of Motion did not exist?&lt;br /&gt;
&amp;gt; Are Newton&amp;#039;s First and Second laws of motion refuted&lt;br /&gt;
&amp;gt; by the laws of thermodynamics?&lt;br /&gt;
&lt;br /&gt;
http://scienceworld.wolfram.com/physics/BrownianMotion.html&lt;br /&gt;
&lt;br /&gt;
&amp;gt; Obviously, Newton&amp;#039;s&lt;br /&gt;
&amp;gt; Laws refer to single bodies, and thermodynamics refers&lt;br /&gt;
&amp;gt; to a very large number of bodies, but doesn&amp;#039;t there&lt;br /&gt;
&amp;gt; need to be any consistency between the two?&lt;br /&gt;
&amp;gt;&lt;br /&gt;
&lt;br /&gt;
They are not inconsistant, as far as i know and have come to know. For example, think of the following relation.&lt;br /&gt;
&lt;br /&gt;
1/2 m &amp;lt;v&amp;gt;^2 = 1/2 kT&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;gt;&lt;br /&gt;
&amp;gt; George Gamow wrote that liquid and gas molecules do,&lt;br /&gt;
&amp;gt; in effect, take a random walk and that we can calculate&lt;br /&gt;
&amp;gt; the probability of all the air in any room suddenly gathering&lt;br /&gt;
&amp;gt; to some random place in the room, in some arbitrarily&lt;br /&gt;
&amp;gt; small volume. Do air molecules move contrary to&lt;br /&gt;
&amp;gt; Newton&amp;#039;s First and Second Laws of Motion, ignoring&lt;br /&gt;
&amp;gt; the repellent electrical forces of their atomic shells?&lt;br /&gt;
&amp;gt; What am I missing?&lt;br /&gt;
&amp;gt;&lt;br /&gt;
Not really, George Gamow, carefully chose his words. Remember that he tell that you can calculate the &amp;#039;&amp;#039;&amp;#039;&amp;#039;&amp;#039;&amp;#039;probability&amp;#039;&amp;#039;&amp;#039;&amp;#039;&amp;#039;&amp;#039; that all air molecules suddenly gather in arbitarily small volume.&lt;br /&gt;
&lt;br /&gt;
To translate his statement (into some else&amp;#039;s statement), giving 1000 monkeys, a 1000 typewriters, for a 1000 000 000 years, there is probability that one of those monkey will have typed &amp;#039;to be or not to be&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
&amp;gt; Is it theoretically possible for all the matter and&lt;br /&gt;
&amp;gt; energy in the universe to suddenly gather into&lt;br /&gt;
&amp;gt; some arbitrarily small volume?  If air molecules&lt;br /&gt;
&amp;gt; can overcome the repellent electrical forces&lt;br /&gt;
&amp;gt; of their atomic shells without any external force&lt;br /&gt;
&amp;gt; being applied, can&amp;#039;t matter and energy overcome&lt;br /&gt;
&amp;gt; the forces that hold things together?&lt;br /&gt;
&lt;br /&gt;
Keyword is &amp;#039;possible&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
&amp;gt; In fact,&lt;br /&gt;
&amp;gt; if I am not mistaken, I think Roger Penrose makes&lt;br /&gt;
&amp;gt; this claim.  It seems he looks at matter and&lt;br /&gt;
&amp;gt; energy in the universe as being completely&lt;br /&gt;
&amp;gt; determined by the laws of chance, that all the&lt;br /&gt;
&amp;gt; energy and matter could suddenly find itself in&lt;br /&gt;
&amp;gt; the same place, and produce a big bang, this&lt;br /&gt;
&amp;gt; possibility occupying a certain position in some&lt;br /&gt;
&amp;gt; probabilistic phase space.&lt;br /&gt;
&amp;gt;&lt;br /&gt;
&amp;gt;&lt;br /&gt;
-suresh&lt;br /&gt;
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