Illusions, Delusions and Real ..............
For the sake of Reality, the more simple the scientific theory, the more accurate and profound are the revelations and practical applications
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TIME: Many of the difficulties which we encounter in our attempt to understand the operation of the natural laws arise because of our severely restricted concept of the nature of time. Time follows the same curve of natural law which is apparent in the operation of all the basic factors of nature, and again the radius of that curvature is measured by the quantity C. Follow the example in StarSteps which puts us in a unique position from which we can, from a single point in time, observe ourselves occupying three rather widely separated positions in space. See StarSteps (time example reprinted at end)
------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------NOTE:Contemporary 100 year UNDEVELOPED concept: According to Einstein's theory of special relativity, time slows as an object approaches the speed of light. This leads many scientists to believe that traveling faster than the speed of light could open up the possibility of time travel to the past as well as to the future.
As we begin to comprehend there exists only the Moving Instant Now (all else being differentials of energy and frequency - as Einstein had pointed out in regards to matter - matter looked at closely enough and we find there is nothing but a frequency of vibration), we may ask ourselves, can forces in motion be perceived to intersect at a future point giving us a glimpse of a future probability? The evidence shows that it can, but not physically.
We may also ask if the past could be looked at through some access to a Jungian unconscious memory bank? Again, historical and evidence in consciousness studies indicate that it can.
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StarSteps Example: From a single point in time, observe ourselves occupying three rather widely separated positions in space
Almost any student of physics today, be he a beginner or a graduate scientist will argue that no man can ever travel from the earth to the star Alpha Centauri in a period of less than four years, because the laws of relativity state that matter can never move with a velocity greater than that of light.
Almost any student of physics today, be he a beginner or a graduate scientist will argue that no man can ever travel from the earth to the star Alpha Centauri in a period of less than four years, because the laws of relativity state that matter can never move with a velocity greater than that of light.
This is one of the prime fallacies which has been created by misinterpretation of the mathematics.
The mathematics do not say that man cannot travel between the earth and Alpha Centauri in less than four years. They say only that no observer on earth can ever see him do it. Let us see if we can create an example by which this statement may be more readily understood.
First we will assume that there is a planet in orbit about Alpha Centauri. (Because of Alpha's proximity to its twin star Proxima Centauri, the orbit would be a rather eccentric one, but perhaps it will do as a reference point.)
Next we will build a small space ship, in which we propose to pay a visit to this planet. Since a small space ship is not a very comfortable place to spend long periods of time, the idea of being confined to the craft for the four years, which relativity seems to say is the shortest possible time, is a distasteful one, so we cast about for means to shorten the journey.
If we do our engineering according to the rules which are known as classical mechanics or ordinary engineering practice, it will become apparent at once that we cannot use any source of energy which originates within the ship. These rules of mechanics tell us that, to accelerate a body of matter to a velocity of 3x10(10) centimeters per second (the velocity of light) will require energy equal to 9x10(20) ergs per gram of mass. Yet the rules of relativity (E=MC2) tell us that 9x10(20) ergs is the total energy contained in a gram of mass.
This means that if we wish to accelerate the space ship to the velocity of light by energy created within the ship, we would have to convert all of the matter within the ship, including our own bodies to energy. We would then achieve the velocity of light, but we would arrive at our
destination, not as matter but as electromagnetic radiation.
destination, not as matter but as electromagnetic radiation.
Since we would much prefer to arrive as matter, we must seek an accelerating force which will act from some unlimited source of energy outside the ship.
It is at once apparent that a force field originating on earth would not be successful because the rate of propagation of a field is the same as that of light, and no field can accelerate us to a velocity greater than its own rate of propagation. For the purpose of this example we will simply postulate that we have available, a supply of energy form an outside source, which we can use in any desired quantity, and which can be used to create an instantaneous velocity so high that we will reach our destination, four light years distant, in a single hour.
We will take off from a launching pad which is situated near an observatory operated by a friend of ours, who is an astronomer, and who has a telescope of unlimited power, through which he will observe our progress. Since he can only observe us through the light which we emit during the trip, we must also cause the ship to emit a very large quantity of light.
At a prearranged instant we will takeoff and at once achieve a velocity that will take us to our destination in an hour. After fifteen minutes we will have covered one quarter of the distance, but the light which we emit at that point will require one year to return to earth, and will reach the eyes of the astronomer one year and fifteen minutes after takeoff. He will note in his logbook that we required a year and fifteen minutes to reach the quarter point.
After we have traveled for thirty minutes we will have covered half the distance, but the light which we emit at that point will require two years t return to earth, and so will reach the astronomers eyes two years and thirty minutes after takeoff. After an hour has passed we will have reached our destination, but the light emitted by the craft will not reach the astronomer until four years and one hour after our departure from earth.
All of the light which we emit at intermediate points will, of course, arrive at intermediate times so that the astronomer could observe our progress constantly from the instant of takeoff to the moment of our arrival upon the distant planet, four years and one hour later.
According to the primary postulate of relativity that we must accept the evidence of our senses as being valid, the astronomer must maintain that from his reference point we did not quite achieve the velocity of light.
The fact that we may have returned long before this, that we may be seated at his side, and may perhaps, be assisting him in his work, does not in any way affect the validity of his observations or the mathematics of relativity which he applies thereto.
Let us remember, however, the statement that, when our mathematics are
complete, then we may allow reason to deal with that which we have created. If we do this, we will not fall into the common error of confusing relativity with a concept of absolute determinism.
Let us reiterate Dr. Einstein's preface again: If we allow our reason to modify our observations before our mathematics are complete, we will be evolving a concept whose value is based entirely upon the validity of our reason rather than upon the accuracy of our observations. After our mathematics are complete, then we can allow reason to deal with the formula, but until the formula is complete, we must postulate that events which are observed simultaneously occur simultaneously insofar as that observer is concerned, and that therefore the simultaneity of events is a condition which depends entirely upon the position of the observer with respect to those events.
If we examine this concept carefully, we find that time follows the same curve of natural law which is apparent in the operation of all the basic factors of nature, and again the radius of that curvature is measured by the quantity C.
We will now create another simple analogy, in far greater detail, which may serve to make this statement more readily understood. It will put us in a unique position from which we can, from a single point in time, observe ourselves occupying three rather widely separated positions in space.
Once again, we will start today to build a space ship. We will postulate that the ship will require one year of our time to build, and that when completed, it will be capable of infinite acceleration. We will assume that a continuous supply of energy is available from an outside source, and that the craft will continue to accelerate so long as this energy acts upon it.
During the year which we spend in building the craft, light is being reflected from us into space, so that an observer with a telescope stationed at some other point in space could follow the course of its construction.
When we have completed the construction of our craft we will enter it and take off for a destination which we will assume to be a planet orbiting about Alpha or Proxima Centauri, our next nearest suns, about four light years distant. We have a telescope of unlimited power in the
rear of the craft pointed toward the earth which we are leaving, and another telescope at the front, focused upon the planet which is our destination. We will set the field strength for a constant acceleration, and seat ourselves at our telescopes to observe the result.
rear of the craft pointed toward the earth which we are leaving, and another telescope at the front, focused upon the planet which is our destination. We will set the field strength for a constant acceleration, and seat ourselves at our telescopes to observe the result.
After we have risen a few miles from the surface, we will, for the purpose of furnishing an additional reference point, eject from the craft and its field, a cannon ball or other sphere of metal which has been specially painted so that it can readily be observed from any distance with the aid of our unlimited telescopes.
Since we had not yet reached escape velocity when the ball was ejected, we will observe that it
soon begins to fall back to earth.
soon begins to fall back to earth.
As we continue to accelerate, we will observe that the kinetic energy differential which we are producing between ourselves and our points of observation is producing exactly the effect upon time which is predicted by our postulate of the curvature of natural law.
Since the distance or degree of separation between ourselves and the earth is increasing with time, the energy differential is negative, which means that the natural laws at the observed point will displaced towards the base or zero line of the sine curve, insofar as our observations are concerned.
If we reach a velocity equal to one half that of light, and then observe a clock on earth through our telescope, we will see that in ten hours of our time, only five hours have been recorded by the earth clock. If we observe the test sphere which we ejected during our take off, (assuming that it has not yet reached the ground) we will see that it is not falling at the rate predicted by our laws of gravitation, but at a rate only half as great.
We will also observe that the sphere is not accelerating at the rate predicted by our laws, nor even at half that rate. Since we ourselves are still accelerating, the observed acceleration of the sphere is diminished by a factor which is proportionate to ours.
We must remember that we can only observe events through the light which is emitted or reflected by the objects concerned with those events, and if we ourselves have a motion equal one half that velocity in the direction in which the light is moving, then a column or sequence of light impulses which were emitted from the earth during a five hour period, would require ten hours to pass our point of observation.
When the velocity of our craft reaches that of light with respect to the earth, there will be a negative energy differential, equal to the quantity C, existing between us and our point of observation.
We will observe that all natural laws upon the earth have reached zero value with respect to us. All motion and all changes have ceased.
If we observe our test sphere we will see that gravity is no longer acting upon it, since it has ceased to fall. All laws of motion are in abeyance and the factor which we call time has ceased to have any significance.
To make these observations, of course, we would require one of the new telescopes which operate on the retention of vision principle, where the last image to arrive remains upon the viewing screen until a new light image arrives to change it.
When we reach the velocity C, no new light will arrive, hence the picture will not change until we change our velocity.
Since we postulated at the beginning of this analogy that our craft was capable of unlimited acceleration, and since the postulated force continues to act, our velocity will continue to increase and we will have between ourselves and the earth, a rate of increase in the degree of separation which is greater than that specified by the quantity C. We can do this from our point of reference although, as will be explained later, we cannot do it from the point of view of an observer upon the earth.
When we have passed through the velocity C, a startling change occurs in our observations. We no longer observe the earth from the telescope at the rear of the craft. The earth now appears in the telescope at the front, and we are no longer leaving the earth, we are now approaching it.
We will see a craft which is identical to ours, and which is indeed our own craft, detach itself from us and move back toward the earth ahead of us at a rate which is proportionate to our excess over the velocity C.
If we observe the earth, we discover that all natural laws are operating in reverse.
If we observe the test sphere we will see that it is now falling away from the earth rather than towards it. Gravity between the earth and the sphere has become negative with respect to our point of reference as have all the natural laws.
We observe this through the forward telescope rather than that at the rear, because we are now
overtaking the light which had passed us before we had reached the velocity C, and since we are now overtaking it, we encounter first the light which had passed us last.
overtaking the light which had passed us before we had reached the velocity C, and since we are now overtaking it, we encounter first the light which had passed us last.
All events occur in reverse, just as would the scenes in a motion picture film which is being run backwards.
If we complete our journey to the planet which is our destination, at an average velocity equal to 4 times C, we will arrive with an elapsed time of one year as measured by the clocks on our own craft. During the journey, however, we will observe the elapse of five years of time upon the planet which we are approaching, and the elapse of three years of negative time upon the earth which we are leaving.
In other words we will arrive at our destination three years before we left the earth.
If immediately upon our arrival we seat ourselves at a telescope of sufficient power to observe the earth at close range, we will see ourselves going about the daily tasks which we performed two years before we began to build the space craft in which we made the journey.
If we then focus the telescope upon the proper point in space we will see ourselves in our space craft, flying backwards toward the earth.
We are now in a position from which we can observe the sine curve nature of all natural law, and to measure precisely the radius of the curvature.
If we observe the earth, we see that time there is positive. That is: it is moving in the direction which we consider normal. Since there is no significant energy differential, the time rate is essentially the same, but because of the degree of spatial separation there will be a displacement along the time curve, between the observer and the point which he is observing.
According to our theory of the curvature of natural law, this displacement should be equal to D divided by C, where D is the distance and C is our basic factor.
In the case of our present observation the distance is equal to 4.C.years, which if divided by C will equal 4 years, which is precisely the degree of displacement which we observe.
If we now turn our attention to the space craft, we find that we are observing it through an energy differential which exceeds the quantity C and therefore the craft is within the negative portion of the curve, and all natural laws will be operating in reverse at that point.
We are now in a unique position, in that we now can, from a single point in time or at least from a single point in the only dimension of time of which we are conscious, observe ourselves occupying three rather widely separated positions in space.
First: our position at the telescope as the observer. At this point time is positive.
Second: our position on the surface of the earth. Here time is also positive but has a negative displacement upon the time curve which is equal to four years.
Third: our position in the space craft: here time is negative, as demonstrated by the fact that we
observe it flying backwards toward the earth, and all actions taking place within it occur in reverse order. This is, of course, due to the fact that the craft had a velocity greater then that of C and so was constantly leaving behind the light which was emitted or reflected from it.
observe it flying backwards toward the earth, and all actions taking place within it occur in reverse order. This is, of course, due to the fact that the craft had a velocity greater then that of C and so was constantly leaving behind the light which was emitted or reflected from it.
As we observe the craft from our new reference point, the last light which it emitted arrives first.
If we continue to observe for several years, we will eventually see ourselves build the craft and take off into space.
At the same time we can see ourselves in the same craft hurtling backward through space toward the inevitable meeting point where the past and the future join to become the present.
Since we are observing ourselves simultaneously occupying three different positions in space, we can readily see that we are forced to a concept of time which includes more than one dimension.
If we continue to observe the two craft, we will see that the one which is moving away from us is constantly slowing down, while the one coming toward us from the earth is accelerating. At the instant in which the velocity of the receding craft reaches zero, the approaching craft will reach it, coincide with it, and both craft will disappear completely from view.
Our lateral excursion into time has completed its curve and we have returned to the starting point of our unidimensional concept.