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THE NEW THEORY OF OPPORTUNE TIME

Mathematical Principles of the free will of the motion of bodies

DISCOVERED BY Emil Núñez Rojas

Patented in Prague, 2000

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THEORY OF OPPORTUNE TIME: Mathematical Principles of the free will of the motions 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 Núñez Rojas

noverbal@hotmail.com

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

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All rights reserved

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CONTENTS

Introduction: Historical Movement

Chapter 1: the laws of the appropriate time for solids and particulates.

Chapter 2: Event stationary in a opportune time.

Freewill the movement of an event. Opportune time away. Union of two events by an attractor.

Chapter 3: Free Will of the motion of bodies

Chapter 4: Journey of a particle in an opportune time

Chapter 4: Event nonstationary in an opportune time

Universal law of transformation of 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 right 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.

Collective and individual energy.

In any conservative system, the particles are constantly moving continuously

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

environment in order to maintain its minimum energy 0 . 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 energy 0u-uΔu greater than the collective energy or at a time

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

Δt >Δ is also described by:

Δt> 1

Δ

And the relationship between the energy differences for:

Δu> 1

Δ

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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 energy was at first.

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 they happen at the same time energy region that is if:

Δt= 1

Δ and

Δu= 1

Δ

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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:

m

Un

or

n

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Where n is the number of total enermass.

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 the system 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.

Where 1

11

m

U is the coefficient of mass energy of the body mass 1m and

2

22

m

U is the coefficient of mass energy of the body mass 2m

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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."

Itisdefined 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 toU

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 tC

C C C

2

2

Δm=

CU

nt

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

Δm=

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. Theequationisbestexpressed as follows:

2

2

0

Δm=

CU

n

Where C

v =n

is the transfer rate m

U and:

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 Núñez Rojas

noverbal@hotmail.com

emilnunezrojas7@gmail.com

(+051) 954 638 125