The New Theory of Opportune Time by Emil Núñez Rojas

8/10/2019 The New Theory of Opportune Time by Emil Nez Rojas

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THE NEW THEORY OF OPPORTUNE TIME

Mathematical Principles of the free will of

the motion of bodies

DISCOVERED BY Emil Nez Rojas

Patented in Prague in 2000


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THEORY OF OPPORTUNE TIME: Mathematical Principles of free well of the motion of bodies.

Second Edition

Printed in Peru

Legal deposit in the National Library of Peru

N 2011-15653

ISBN: 978-612-00-0749-5

Are strictly prohibited without written permission of the copyright holders under the

penalties provided by law, the total or partial reproduction of this work by any means or

process, including photocopying and computer processing and the distribution of copies of

the authorization same for hire or public loan.

It was printed April 1, 2014

Lima-19 Carretera Central km

Copyright 2013 by Emil Nez Rojas

[email protected]

Lurigancho Chosica - Nana - The Age Mz - lte 1-C

[email protected]

All rights reserved
mailto:[email protected]:[email protected]:[email protected]


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CONTENTS

Introduction: Historical Movement

Chapter 1:the laws of the opportune time for solids and particles.

Chapter 2:Stationary event in an opportune time

Free will of the movement of bodies. The away opportune. Union of twoevents by an attractor.

Chapter 3:The free will of motions of atomic particles.

Chapter 4:Journey of a particle in an opportune time.

Chapter 5:Non stationary Event in an opportune time.

Universal law of transformation of opportune time into space.


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INTRODUCTION

HISTORICAL MOVEMENT

Confrontation unscheduled event

There are two different words: the future and "come." There is a future which

is predictable, programmed, planned or forced, but there is a future "coming"

which comes completely unexpectedly. This is the real future.

If simultaneity or collision of two cars which were not scheduled to happen,

however, that both cars have the clash occurred even pace or movement such

period they must have approached to the collision is timely.

Two examples. When a person becomes distant place where even get to know

your partner. If one of them had come at a time before or after the

appropriate time interval, or outside the exact time that the event is met,

perhaps the event with them had not been met. This part of the story had not

been given.

For this last event occurs both should have moved to the start of the event to

an appropriate motion, that is, that although the distance is short or long, the

pace of travel to reach the time when the event begins to take its rhythms or

periods must do everything possible to achieve concurrency between them.

Note that we are interested in describing the situation without the distance

that is talk about the event itself, its beginning or end of that period plus or

rhythm of movement that would require the two to meet at the start of the

event. Two moving objects coming from different places and rhythm suitable

periods so that their confrontation they occur in a particular timely while the

event is happening: In general it is described as follows.

This event is called the opportunity for the body to move, but not the

movement produced at that time. Actually which are not material but

confronting events ie opportunities bodies. It's a confrontation that although

times are relative to the difference in their due time all will be part of that

simultaneity of events, which will be a single geometric structure of events.


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LAW OF MECHANICAL MOVEMENT OF BODIES

CHAPTER I

THE LAWS OF TIMELY FOR SOLIDS AND PARTICLE

The opportune time is the duration of the interaction between the molecular

or atomic particles of bodies, either in its resting state, without the

intervention of an external force, or the intervention of her.

First Law.

Collectiveand individual energy.

In any conservative system, the particles are constantly moving continuously

interacting with each other in a minimum time 0- = and their

environment in order to maintain its minimum energy0

. This

minimum energy is called collective energy.This motion is uniform state

unless an external force to the system to change the state of uniform motion.

If an external force changes its state of constant motion so that creates some

need for recovery, then the particles will go out of state energy time being

they are not necessarily out of its original space. Exit out of state energy time

means leaving your dosed state which retains the minimum time or minimum

energy your collective energy distributed among all particles.

Now if one or more particles come out of your time energy region. They will

spend energy0

u-uu greater than the collective energy or at a time

0t - t =t and minimum energy greater than the minimum time . That is:

t > is also described by:

t > 1

And the relationship between the energy differences for:

u> 1

Of course in this case the interaction continues but this time spend more time

interacting with other particles in order to maintain their state of minimum

energywas at first.


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A clear example is the game of football. Suppose a group is playing only with

passes. In this game we call collective. Suppose there is a minimum of a pass

from a teammate and player at that minimum time is spent minimal energy.

However. In reality it does not. Because there is also the side where players

used to defend what they call the "dribbling" or the individual struggle for power

and this slows down the pass energy and energy increases and individual type

and is not collective. Now if a football player just entering the game with the

same minimum time and passes the ball to his partner, then it is said that

both players are simultaneously in the same event. As stated the following

law.

Second Law.Upon simultaneity.

Two particles are simultaneous with respect to the same energy state if theyhappen at the same time energy region that is if:

t= 1

and

u= 1


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GENERAL LAW OF ATTRACTION OF

SOLID BODIES

Definition I

In all matters there is an energy ratio:

m

U

"Enermass" throughout the body where each amount of energy U there is a

ratio of mass m .

Definition II

Within a small amount of body mass system of the same element there is a

large amount of energy where enermasa is the same for the whole system.

Definition III

The sum of all the same enermass of a group of particles is called

"enermota". It is defined as:

mUn

or

n

Where n is the number of total enermass.


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Definition IV

The interaction of bodies occurs in a minimum time called "opportune time

"

The system "identifies" the number of bodies or particles that make up thesystem for the opportune time for them to take in their energy and mass. So

just enermasa particles attract and repel different enermasa.

These particles but become the minimum time that the whole system

completely changes are expelled. represents an opportunity to attract the

particles within an appropriate time. Where:

t

and t the time of particle

motion at your option.

2

21

F

Otherwise attract as if your community is greater.

Where1

1

1

m

U is the coefficient of mass energy of the body mass

1m and

2

2

2

m

U is the coefficient of mass energy of the body mass

2m and is a

constant.


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Third Law

Equivalence of mass energy at an opportune time and transfer rate.

"For all solid body or system of particles is satisfied that an amount of

enermasa is proportional to the rate of conversion of mass to energy or vice

versa and inversely proportional to the chance of the body or the particle

system for this transformation is realized."

It is defined by:

For example. In a football game, a group seeks to achieve its original state,ie, attempts to recover their collective energy(minimum) and struggle

actually against its opposite (the other group) is nothing but the struggle to

travel the roads his opponents let him pass.

Each player looks at his path, the path that leaves its opposite in minimal time

and concentrate on the road with minimum time that this leaves him. And if

the path changes, it will change the direction looking for the minimum

time. The group thus attempts to preserve the structure.

Where are all the structure of players to return to the collective energy, the

minimum mass with minimal energy in the same proportion and those

without this proportion has come together when the right time will be the

right time and mass the group of several players quickly gather to see that are

needed. As in volleyball, lack 1 in 5 or 6 to balance the minimum time, also the

group of football come together until the energy per player come together

and is minimal and when this happens the mass of few players will be

transformed into a large amount of energy called collective energy.

2U v=

m


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The same is true for the conservation of mass in the interior of a moving

body. For example a box. The amount of movement that the number of

photons emitted from one place to another a box is:

UP =

Cn

Where n the number of photons with momentum equal to

U

p = C . As the

momentum is conserved in any system, then, with the emission of light waves

group box must go back to a speed V defined by its momentum by:

UP = MV =

Cn

It is true that the velocity V is constant but time dependent motion of mass

. When the latter comes to be realized then the amount of mass m will also

come to completion. So the recoil velocity of the box comes at a time:

t =

x

V

While the transfer time of the light waves must equal the total time that a

distance L n number of photons at the speed of light traveling.

1 2 n= t =C

nL+ t + ... + t

The transfer of light waves is converted to an amount of sufficient mass so

that the center of mass is maintained. That is:


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M x = L m

Later. Substituting the above equations and solving the latter m. We have:

2

2

nn tM x nMVt n

m =L

U

U tCC C C

2

2

m=

CU

n t

This indicates that an amount of mass m contains an amount of energy U

depends on the number of photons emitted in the opportunity

t= . That

is:

2

2

m=

CU

n

Now. The number of photons are complete when the time . This indicates

that in the equation n is actually the number of initial photons. The equation

is best expressed as follows:

2

2

0

m=

CU

n

WhereC

v =n

is the transfer ratem

Uand:

2

2

C

U vn= =m

Therefore enermass quantity is equivalent to:

The transfer rate is the speed at which a body approaches to the other end of

the box:

2U v=

m


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m

Uv

Cn =v

.

Also n is the refractive index of the speed of light in vacuum and the relative

speed with respect to another media.

The following parts of the content and the equations of each part

In the following equations presented by Emil Nunez will release the other

issues that are in the table of contents of the book New Theory of opportune

time

Emil Nez Rojas

[email protected]

(+051) 954 638 125
mailto:[email protected]:[email protected]

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The New Theory of Opportune Time by Emil Núñez Rojas