By the way i changed the numbers in my post to make it less instantly trivial regarding the 100 to 1 bet example.
Keep in mind i am the guy that doesnt choose camps here, lol. I choose logic and science and math education instead so that you know each time what you can use best depending on what information is available or suspected.
That something has 90% chance to come out in some particular way (ie heads for a coin) in some event means to most people that if you run the event a large number of times and you accept these are identical experiments (not changing the conditions to make the trial not a repeated similar trial but individual events of their own unique properties) the frequency of occurrence will converge to 90% of total. If that cannot be the case ie you cannot repeat a complex event then its a number some theory you have proposes to assign preference/prediction bias (eg some champion top team A will win the first round elimination double match combo in some cup vs a very weak team with 90% chance or a star will explode as supernova with 90% chance in the next 10 mil years). In those cases all you can do to test how good your model that assigns such probabilities is is to apply it many times in different situations that the same theory is used and see what the results are.
You can see probability as frequency something happens in cases that are clean enough to be seen as identical or as a local preference value.
I can also see probability in complex enough systems that the trials are never identical but the mixing is so interesting and universal in its properties moreover the chaos that the frequency interpretation still proves the same over time.
Predicting a supernova will explode with 90% chance in the next 10 mil years is a one time event proposition and may be the result of simulations for example that when repeated in different sets still converge to the same result even if each trial is different than the one before in the details of how it got there. Ie i run 10 mil simulations and then run another 10 mil later and they use different rnd feeds and still i get identical (within statistical error) distributions of the explosion time. Each time the star is left to evolve the trajectory is not identical but all those different paths result in the same distribution eventually with common avg (ie 10 mil years) say for eg the 90% confidence level.
Also see
http://en.wikipedia.org/wiki/Probability
"Probability is the measure of the likeliness that an event will occur.[1]
Probability is used to quantify an attitude of mind towards some proposition of whose truth we are not certain.[2] The proposition of interest is usually of the form "Will a specific event occur?" The attitude of mind is of the form "How certain are we that the event will occur?" The certainty we adopt can be described in terms of a numerical measure and this number, between 0 and 1 (where 0 indicates impossibility and 1 indicates certainty), we call probability.[3] Thus the higher the probability of an event, the more certain we are that the event will occur. A simple example would be the toss of a fair coin. Since the 2 outcomes are deemed equiprobable, the probability of "heads" equals the probability of "tails" and each probability is 1/2 or equivalently a 50% chance of either "heads" or "tails".
These concepts have been given an axiomatic mathematical formalization in probability theory (see probability axioms), which is used widely in such areas of study as mathematics, statistics, finance, gambling, science (in particular physics), artificial intelligence/machine learning, computer science, and philosophy to, for example, draw inferences about the expected frequency of events. Probability theory is also used to describe the underlying mechanics and regularities of complex systems."
You cannot have probability without repetition (either real repetition or implied in some parallel world sense like the star example) in the most simple cases people apply probability theory to but a more elaborate formal approach in terms of axioms is also another way to see things.
At some point when you have no prior knowledge or a hypothesis to test all you have is the trials and hopefully that they are clean enough to be seen as identical. Then with them you develop the concept of probability. Later you can use various methods to test if what you are now proposing based on these observations is reasonable or it has started to have problems.
To give you an idea, i have no knowledge whether the quantum experiments that try to see how random QM is are so far clean enough all these decades to eliminate pseudorandom number generator issues. By that i mean a fully deterministic non local theory of hidden variables can be deciding the results of experiments each time to make them look random without being exactly random. For example and i am not suggesting this is the case, what if the decay behavior of radioactive nuclei depends on solar activity (recent claims) . What if the spin of some electron measured is a function of some far away system that is so chaotic that makes the spin look random in measurements. We need methods to test properly whether QM is indeed truly random and find if any correlations exist actually that nobody noticed. In that sense a purely frequency approach will fail to see the structure. However if correlations exist we can potentially uncover them with experiments and proper hypothesis testing.
Notice also how close to the frequency understanding most people have of probability, the resulting theorems prove ie
http://en.wikipedia.org/wiki/Law_of_large_numbers
http://en.wikipedia.org/wiki/Central_limit_theorem
See also
http://en.wikipedia.org/wiki/Probability_axioms
http://en.wikipedia.org/wiki/Cox%27s_theorem
http://en.wikipedia.org/wiki/Bayesian_probability
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Non free will signature. 2+2 community, BruceZ, 2+2 leaders etc, all with your choices give back BruceZ and others you "chase" away to this discussion and the ones that will follow. We are all in this interactions learning game together.
Last edited by masque de Z; 10-01-2014 at 02:09 PM.