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.

1. 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
1

2. THEORY OF OPPORTUNE TIME: Mathematical Principles of the
free will of the motions of bodies.
2
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
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3. 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.
3

4. 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.
4

5. 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.
5
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 0 Δu  u - u greater than the collective energy  or at a time
0 t - 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

6. 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:
6
Δt

=1
Δ
and
Δu

=1
Δ

7. GENERAL LAW OF ATTRACTION OF
SOLID BODIES
7
Definition I
In all matters there is an energy ratio:
U
 
m
"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:
U
m
  n
or
  n

8. 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:
 
 F
  is the coefficient of mass energy of the body mass 2 m
8


t
 and t the time of particle
motion at your option.
1
2 
2
Otherwise attract as if your community is greater.
Where
1
1 m
1
U
  is the coefficient of mass energy of the body mass 1m and
2
2
U
2 m

9. 9
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:
2 U v

=
m
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.

10. 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:
10
U
P =
C
n
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:
U
P =MV =
C
n
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 =
nL
C
+ 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:

11. M x = L m
Later. Substituting the above equations and solving the latter m. We have:
  
U
11

   
2
2
nn t
M x nMVt n
m=
L
U
C U t
C C C
2

Δm
2
=
C
U
n
t
This indicates that an amount of mass m contains an amount of energy U
t
depends on the number of photons emitted in the opportunity 
= . That

is:
Δm

2
2
=
C
U
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
C
2
0

Δm
=
U
n
Where
C
v =
n
is the transfer rate
m
and:
2
C
 
 
 
2
U n v
= =
 
m
Therefore enermass quantity is equivalent to:
2 U v

=
m
The transfer rate is the speed at which a body approaches to the other end of
the box:

12. 12
U
m
v


C
n=
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