|
T, log U
V,
with another constant: T + V = CONSTANT. for kinetic energy
, T and potential energy, V.
Result: Langrnage's Principle, derived from The Antitonic Principle. PL Hamilton's
Principle derived from the Antitonic Principle (PL), and d'Alembert's Principle derived
from Newton's Law , with antitonic form.
supSn*/(2 log log n)½ = 1.
x < 1, x = 0.a1a2. Such
decimal expansions connect with Bernoulli trials (PL) with probability p =
1/10, such that digit zero represents success and all ofther digits represent failure
. Thus, in the sample space (PL) of Bernoulli trials, the event "success at nth trial" is
represent by all real numbers x whose n
th decimal is zero. Thus, all limit theorems for Bernoulli trials for p = 1/10 translate into theorems about decimal expansions, so that "with
probability one" translates into "for almost all x" or "almost everywhere". In measure
theory (PL) language, the weak law of large number (PL) asserts that S
n(x)/n
1/10 in measure, while the strong law of large numbers
asserts that Sn(x)/n
1/10 almost
everywhere. Then, Kinchine theorem asserts lim sup (Sn(x) -
n/10)/(n log log n)½ = (0.3)
2, for almost all
x. (This answers a problem formulated in a series of papers initiated by
Hausdorff in 1913 and by Hardy and Littlewood in 1914.)
X f dm for measure
space X and measure m
.
Sk(ak, bk)
of disjoint intervals has the measure, m
L(S)
Sk(bk
- ak). A closed set S'
[a, b] -
Sk(ak, bk has measure
mL(S')
(b - a)Sk(bk - ak). (A unit line segment
has Lebesgue measure of one; the Cantor set (PL) has Lebesgue measure zero; the Minkowski measure
(PL) of a bounded closed set is the same as its Lebesgue measure.)
d
. (PL limit (as antitone). The series S
sn has such a limit iff its sequence of partial sums s1, s1 + s2, s1 + s2 + s
1, ... has such a limit.