Welcome To This Web Site: Antigravitation Engine Site
The present URL: http://xczhx.c59.zgsj.com/indexEnglish.htm (beginning on 6 February 2006)
The former URL: http://xczhx.nease.net/indexEnglish.htm (expiry date: 30 June 2006)
The earliest URL: http://xczhx.diy.163.com/indexEnglish.htm
Chapter 1
An introduction to some
antigravitation engine experiments
that everyone can make
1.1 An introduction to an article
In the Chinese magazine UFO Research, No.1, 1997, Mr. Sun Fengwu, in his article "The ups and downs of the flying saucer research", pointed out that lack of the concrete evidence made researchers discouraged." Below is an introduction to an antigravitation engine experiment that everyone can make, which the readers might be interested in.
The experiment and its theory were originally carried in the article "UFO: Phenomena, theories and experiments" by the author of this Web site. (The Chinese version of this website was introduced to the Website of the Department of Physics at Peking University on August 26, 2002 by Mr. Liu Wuqing.) The article was included in the book Heaven, Earth and Man (-- Across Science And Culture, Chinese edition, chief compiler: Wu Zhijing, Popular Science Publishing House, Beijing, September, 1992). The Magazine Knowledge Is Power (Chinese edition, 1993, No. 4, p. 35) carried a brief introduction to this book and this article. The book was listed in the booklist carried by the magazine Amateur Astronomers (Chinese edition, 1994, No. 2, p. 26). The famous scientist Yan Jici (former Vice-President of the Chinese Academy of Sciences) wrote words of encouragement for the book.
1.2 A brief introduction to the antigravitational mechanical experiment and its theory
The purpose of this experiment is to verify the set of equations of the antigravitation engine (see Chapter 2 and
Chapter 5) and to verify the macroscopic quantum phenomenon (see Chapter 4). The experiment is made in the following way (see Chapter 3).
First, make an antigravitation engine, whose name is the rotary antigravitation engine, in the following way.
A small wheel (hereafter called the rotation part), driven by a toy motor, serves as the rotation device. A glass jar (for the canned fruit) with a plastic cap and grease serves as the sealing device, with which the rotation device is sealed up.
The power device behind the motor of the rotation device serves as the disturbance device, which disturbs the current of the gravitational field, and hence it also serves as the direction-determining device.
Put the above devices horizontally in the carrying device, which is an empty washbasin with a foam plastic board put horizontally in the washbasin. Rechargeable batteries of the power device supply the power.
Put the washbasin on the water in a bathtub, and the washbasin is now a "boat". This boat is the rotary antigravitation engine.
Get ready with the surveying instruments, including a reflecting revolution counter.
The experiment should be made in a shelter in which there is no wind. The wheel should not be eccentric when it rotates. Both the bottom of the washbasin and the shaft of the motor should be horizontal. The space around the experiment devices should be spacious.
Start the motor, and the experiment begins.
The following is a brief introduction to the set of equations of the rotary antigravitation engine to be verified by the experiment.
Gravitational field matter can be called "gfm" for short. The definition of the antigravitational field is the moving gfm. The current of the gfm of a body causes waves in the local gfm of the universe. Under certain conditions, such currents and waves can drag spacetime and drag the inertial frame, and can cause microscopic and macroscopic quantum phenomena. The definition of antigravitation is the effect of inertial frame dragging of the moving gfm.
The antigravitation produced by the antigravitation engine is a dissipative structure.
The set of equations of the antigravitation engine which this experiment is to verify is as follows.
a = 16π3 m r4 / ( c h T4 ) ,
when | 16 π3 m r4 / ( c h T4 ) | > | Σa' | ; (1)
a = 0 ,
when | 16 π3 m r4 / ( c h T4 ) | ≤ | Σa' | ; (2)
where m is the mass of the particle or the mass of the ball of particles which moves freely for a long distance and in good order in the rotation part.
When the rotation part is an ordinary conductor, in the set of the above equations,
m = me
,
which is the mass of the electron, r is the radius of gyration of the metal part of the rotation part, T is the period of the rotation of the end point (hereafter called Point A) of r , a is the antigravitational acceleration which points to the front and which is produced by the electrons of the metal part of the rotation part, and a is also the antigravitational acceleration of both the gfm waves, and the de Broglie waves, of the gfm current of the metal part of the rotation part, |Sa'| is the absolute value of the resultant acceleration which is along the front direction of the rotation part and which is obtained by the electrons at point A and which is other than antigravitational acceleration, π is pi, c is the speed of light, and h is Planck's constant.
The front direction of the rotation part is from the source of disturbance helping produce the antigravitation to the rotation part. Other strong disturbances might make the disturbance device fail to determine the direction.
At the beginning of the experiment, the boat often rotates,
stays at the same place, or moves about randomly, which is obviously different
from the movement of an ordinary motor boat. This is the first stage of
movement, during which the law described by Equation (2) works.
Usually the boat gradually moves along the front or back direction of the
rotation
part in such a way that it looks like leaping once and once again. During the
movement the boat might stop, and after the stop it might move in the opposite
direction. Sometimes towards the end of the experiment the boat might suddenly
move much faster. These are movements of the second stage, during which Equation
(1) works.
From Equation (2) we know that if the boat is too heavy or moves too fast so
that the water resistance is too large, the second stage of movement will not
happen; but during the time when the second stage of movement happens, the acceleration
of the boat is not related to the total mass of the boat as far as
classical physics is concerned, and this shows the antigravitational effect.
Because of the macroscopic quantum effect, when being controlled by the gfm current, the boat is in uncertain spacetime, and hence it moves now fast, now slow, now forward, now backward, and sometimes it stops for a while.
It can be found in the experiments that besides observing quantum mechanics, antigravitation has the antigravitational quantum of action of its own, the sign of which is h' (see Section 7.10.1 in Chapter 7).
1.3 A brief introduction to the antigravitational thermal experiment and its theory
(see also Chapter 7)
In the experiment stated in Section 1.2, use a digital thermometer with minimum temperature resolution equal to or better than 0.1°C. Use a rotation device whose rotation part is so light that for the rotation part, there is h' < h (for the way to calculate h’ , see Equation (3) in Section 7.10.1).
Step 1. Record the temperature (T1) on the surface of the “boat” when the boat is moving due to antigravitation.
Step 2. Record the temperature (T2) on the surface of the boat when the antigravitation is made to disappear by stopping the boat with a rod (see the Set of Equations (16) in Chapter 2).
It can be observed that, if the thermal current fluctuations (i.e. the temperature noise) is excluded from the calculation, in most cases T1 is higher than T2 by 0.1°C or more.
This is because there exists the following relation
E’ = h’ ν , ( 1 )
where E’ is the antigravitational energy of the gfm (gravitational field matter) ball particle (see Chapter 4), h’ is the antigravitational quantum of action, and ν is the frequency of the gfm ball particle.
It can be seen from the above relation that h’ indicates the antigravitational energy level. When a particle jumps from a spacetime whose antigravitational quantum of action is h’1 to a spacetime whose antigravitational quantum of action is h’2 , if h’1 > h’2 , then the particle will release antigravitational energy (including non-present-time antigravitational energy) and the temperature of the particle will rise; if h’1 < h’2 , then the particle will absorb antigravitational energy (including non-present-time antigravitational energy) and the temperature of the particle will fall.
The gfm ball of a celestial body is very huge, and has quantized layers; h’ in its centre is larger than h’ on its surface (for the way to calculate h’ , see Equation (3) in Section 7.10.1).
1.4 A brief introduction to the antigravitational electromagnetic experiments and
its theory
(see also Chapter 7)
1.4 h' and the frequency of the change in the voltage of the electromagnetic wave signals
The voltage in the antigravitational field can be measured with a digital multimeter (DMM) with ac volts minimum resolution equal to or better than 0.1 mV.
Set the function/range switch of the above DMM to the minimum range for ac volts measurement, and the voltage value of the electromagnetic wave signals can be measured. This value changes from time to time.
1.4.1 a small h'
In the experiment stated in Section 1.2, replace the original rotation part with one whose mass is smaller. When the "boat" is moving on the water due to the antigravitation, place the DMM test probes in front of the rotation part and perpendicular to the motor axis. After about two minutes it can be observed that the frequency of the change in the voltage value is lowered. This is because, for this rotation part, h' < h (as for the way of computing h', please see Equation (3) in Section 7.10.1), which makes the electromagnetic uncertainty in the local space reduced.
1.4.2 a larger h'
If a rotation part whose mass is larger is used in the above experiment, then it can be found that when h' is larger, the frequency of change of the voltage value of the electromagnetic wave signals in the local space is higher. This is because when h' is larger, the electromagnetic uncertainty in the local space increases.
1.5 A brief introduction to the antigravitational magnetic experiment and its theory
(see also Chapter 7)
1.5.1 A gfm eddy can enlarge a magnetic field
During the transition, a particle releases or absorbs the gfm eddy whose energy is h’ν.
The gfm eddy itself has no magnetic field, but since it has the effect of inertial frame dragging, when there is an initial magnetic field, the eddy can separate the positive and the negative ions (according to the left-hand rule), and since the moving speed of the centre of the eddy is larger than that of its edge, the gfm eddy can enlarge the initial magnetic field (according to the right-hand screw rule), for example, the initial magnetic field due to the electromagnetic uncertainty relation.
The secrets of UFOs and the Bermuda Triangle may be related to this. Please see Sections 6.22 and 6.21 in Chapter 6.
1.5.2 Antigravitational magnetic experiment
In the experiment stated in Section 1.2, put a compass in front of the rotation part (at the head of the boat). The boat should be horizontal, and the batteries should be newly charged.
Step 1. Make the rotation part rotate clockwise. The head of the boat points southeast. When the boat moves due to the antigravitational field, after about 2 minutes, it can be observed that the south pole of the compass needle deflects westwards by about 2° .
Step 2. Make the rotation part rotate anticlockwise. The head of the boat points southeast again. When the boat moves due to the antigravitational field, after about 2 minutes, it can be observed that the south pole of the compass needle deflects westwards by about 2° .
Step 3. Make the rotation part rotate anticlockwise. The head of the boat points southwest. When the boat moves due to the antigravitational field, after about 2 minutes, it can be observed that the south pole of the compass needle deflects eastwards by about 2° .
Step 4. Make the rotation part rotate clockwise. The head of the boat points southwest again. When the boat moves due to the antigravitational field, after about 2 minutes, it can be observed that the south pole of the compass needle deflects eastwards by about 2° .
The above experiment demonstrates that the gfm eddy of the rotation part enlarges the initial magnetic field which comes from the terrestrial magnetic field (Near the north pole of the earth is the south geomagnetic pole, while near the south pole of the earth is the north geomagnetic pole).
1.6 A brief introduction to the antigravitational optical experiment and its theory
(see also Chapter 7)
1.6.1 The change in h' causes the change in the energy levels of the particles
In the experiment stated in Section 1.4, stop the motion of the boat with a rod to make the antigravitation disappear (please see the Set of Equations (16) in Chapter 2), and after about two minutes it can be found that the voltage value of the electromagnetic wave signals in front of the boat falls a little.
This is because before the motion of the boat is stopped, the boat is in the antigravitational field and h' < h ; hence the energy levels of the particles in the local space is raised and there is a population inversion, and then another kind of laser is produced.
This might be related to the phenomenon of the rainbow body found in Tibet.
1.6.2 The change in h' causes the refractive index change effect
In the experiment stated in Section 1.2, put a rod in front of the boat into the water, turn on a desk lamp behind the boat, and one can find that, when the boat is moving on the water due to antigravitation, after about two minutes, the shadow on the side of the bathtub under the water surface moves slightly in the direction of the window. (During the experiment, the door of the laboratory should be shut and the computer in the laboratory should be shut down.)
This is because in the local space in front of the boat, h' < h . Near the window the voltage value of the electromagnetic wave signals is smaller, which makes h' easier to dominate in the local space. Hence the refraction index of the medium in the local space above the water in the direction of the window is the smallest, and that under the water in the opposite direction of the window the largest. The light refracts in the direction of the optically dense medium; that is, the light moves in the opposite direction of the window, and hence the shadow moves in the direction of the window.
Sometimes, however, the voltage value of the electromagnetic wave signals is larger near the window than that in the inner part of the room; then in the experiment it can be found that the shadow moves in the opposite direction of the window.
1.7 A brief introduction to the antigravitational
time experiment and its
theory
(see also Chapter 7)
In the antigravitational experiment the time shown on a stopwatch sometimes pauses.
1.7.1 Steps of the experiment
(1) Prepare three identical quartz stopwatches (chronograph capabilities: dive watch, 1/100 second precision to 24 hours). Let them be Stopwatch A, Stopwatch B and Stopwatch C respectively.
(2) Start Stopwatch A and Stopwatch B simultaneously. In the experiment stated in Section 1.2, lay Stopwatch B in front of the rotation part of the antigravitation engine, at the head of the boat (without the washbasin). The boat (without the washbasin) is put horizontally on the water in a bathtub.
In order to make the speed of the boat not equal to zero, the water in the bathtub should be fresh and clean, the batteries should be newly charged, and the weather should be clear.
Turn on the motor. Put Stopwatch A on a table in another room.
After 16 hours, place Stopwatch A and Stopwatch B side by side. Shoot a video of the readings of the two stopwatches, and take at least 10 photos of them. When the photos are taken, the shutter speed is 1/1000 s.
(3) Start Stopwatch A and Stopwatch C simultaneously. Lay Stopwatch C in front of the rotation part of the antigravitation engine, at the head of the "boat". Put the boat on a stool. Turn on the motor. Since the frictional resistance of the stool surface is large, the antigravitation is zero according to Eq. (2) in Section 1.2 of Chapter 1. Put Stopwatch A on a table in another room.
After 16 hours, place Stopwatch A and Stopwatch C side by side. Shoot a video of the readings of the two stopwatches, and take at least 10 photos of them. When the photos are taken, the shutter speed is 1/1000 s.
1.7.2 The result of the experiment
(1) The video playing in slow motion and playing step by step shows that, compared with the time shown on Stopwatch A and that shown on Stopwatch C, the time shown on Stopwatch B sometimes pauses. (Please click here to view the video. On the left is Stopwatch A. On the right is Stopwatch B, with an adhesive plaster on it. To save the time, please click Save instead of Open.)
(2) When Stopwatch A is close to Stopwatch B, Stopwatch A will be affected by Stopwatch B and hence the uncertainty in the time shown on Stopwatch A will slightly increase.
1.7.3 Theory
(1) In the antigravitational field, a different antigravitational quantum of action corresponds to a different uncertainty in the spacetime, and hence corresponds to a different spacetime.
In the antigravitational field, when the mass and the velocity of a particle vary due to the uncertainty relation of quantum mechanics and due to the change in the quantum state, the particle has different antigravitational quanta of action (see Eq. (3) in this section), and hence it is in different spacetimes.
Hence in the antigravitational field, different quantum states often belong to different spacetimes.
Therefore, in the antigravitational field, at some moments Stopwatch B is in a quantum state of another spacetime, and hence the time shown on the stopwatch pauses.
When it has left the antigravitational field, Stopwatch B will keep the above feature for a short time.
(2) According to mechanics,
Delta E = (1/2) m v2 . ( 1 )
According to Equation ( 2 ) of Section 7.10.1,
m = M v2 / (c2) , ( 2 )
where m is the mass of the gfm (gravitational field matter) ball particle of the rotation part of the antigravitation engine.
According to Equation ( 3 ) of Section 7.10.1,
h' = 0.27 G M2 v / (c2) , ( 3 )
where h' is the antigravitatioinal quantum of action.
According to Equation ( 2 ) of Section 6.8,
(Δ t) (Δ E) ≥ h' / (4 ) . ( 4 )
Substitution of Equations ( 1 ), ( 2 ) and ( 3 ) into Equation ( 4 ) yields
Δ t ≥ 0.135 G M / ( v3) ,
(v is not equal to 0), ( 5 )
where Delta t is the uncertainty in the time, G is Newton's gravitational constant, M is the mass of the rotation part of the antigravitation engine, and v is the speed of the boat moving due to the antigravitational field.
In the above experiment, M = 0.00315 kg, v is about 0.00004 m/s , and Δ t is about 0.14 s .
1.8 Antigravitational
non-local
spacetime
experiment and its theory
(see also Chapter 7)
1.8.1 Theory
1.8.1.1
From Section 7.10.1 and Section 7.24.3 it can be known that there exit the following relations:
h' = 0.27 G M2 v / (c2) ,
(a ¹0) , (1)
Δt ≥ 0.135 G M / ( v3) ,
(a ¹0) , (2)
and
Δx ≥ 0.27 G M / ( 4 v2 ) ,
(a ¹0) , (3)
where a is the antigravitational acceleration (see Section 2.3), h' is the antigravitational quantum of action, M is the mass of the object, and v is the speed of the object.
Hence it can be known that in the antigravitational field the spacetime location of an object is varying.
For example, in the following experiments, approximately there are the following values:
M = 0.00315 kg ,
v = 0.00004 m/s ,
h' = 7.96×10-38,
Δt≥1.4×10-1 s,
Δx≥2.8×10-6 m.
1.8.1.2
The antigravitational expansion of the universe is accelerating. The earth and the objects on the earth are in the antigravitational field of the universe. M, the mass of the universe, is extremely large. According to Hubble's law, at the place of an object on the earth, v, the speed at which space of the universe is expanding, is extremely small, and at the place of the observer, both v and (dv/dt) are zero.
Hence it can be known from the relations at the beginning of this section that in the antigravitational field which causes space of the universe to expand, objects outside the observer have extremely large uncertainty in the spacetime location, and hence have present spacetime and non-present spacetime.
1.8.1.3
It is another thing, however, with an observer on a boat which is moving due to the work of the antigravitation engine. The antigravitational acceleration of the observer is not zero. And hence it can be known from the relations at the beginning of this section that the observer has comparatively large uncertainty in the spacetime location, and has both the present and the non-present spacetime, and hence can interact with objects both in the present spacetime and in the non-present spacetime.
Hence an antigravitational boat is a spacetime tunnel connecting the present spacetime and the non-present spacetime.
In the experiments described in Section 7.26.2, the scraps serve as the observers.
Hence, when
h' = 0 ,
the observer finds the object local in spacetime;
when
h' ≠ 0 ,
the observer finds the object non-local in spacetime;
where h' is the antigravitational quantum of action of the observer.
1.8.1.4
The Δt of an observer is somewhat similar to exposure time and aperture in photography. If the Δt Observer A is larger than that of Observer B, then, compared with the case of Observer B,
(1) the interaction between Observer A and an object which is in the non-present spacetime is stronger and more evident;
(2) Observer A observes that the Δt and Δx of an object are larger, and hence the object that Observer A observes is more blurred and fainter.
1.8.1.5 Let the uncertainty in time caused by the work of the antigravitation engine be Δt , then the uncertainty in time of the spacetime regions around the antigravitation engine will become nearer to Δt ; this will make the uncertainty in time of the objects in these spacetime regions become either smaller or larger so as to approach Δt ; in other words, the work of the antigravitation engine has a two-way effect.
1.8.2 Experiments
1.8.2.1 Experiment 1
Click here to view the picture.
1.8.2.1.1 Steps of the experiment
(1) Prepare a scrap of blank squared paper which is to be placed at an upper position and hence is called the upper scrap hereafter.
(2) On the front of the upper scrap draw an image of the numeral 2 with a black gel pen. Click here to view the picture.
(3) Lay the upper scrap face up at the inside bottom of the glass jar (see Section 1.2), under the base of the motor.
(4) Prepare a plastic box for holding a 3.5 inches floppy disc (hereafter called the disc box).
(5) Prepare a scrap of blank squared paper which is to be placed at a lower position and hence is called the lower scrap hereafter. Lay the lower scrap face up in the disc box. Close the disc box.
(6) Place the disc box and the batteries on a foam plastic board. Place the glass jar on the disc box.
(7) Place the foam plastic board on the water in a bathtub. With the help of a level gage, adjust the positions of the disc box and the batteries to make the foam plastic board horizontal.
(8) Start the motor, and the experiment begins. Click here to view the video.
In order to reduce |Σa'| (see Section 2.3 of Chapter 2), or in other words, in order to prevent the antigravitational acceleration from becoming zero too often, the experiment should not be long exposed to strong light.
(9) In order to observe the scraps of paper and to replace the batteries with newly charged ones, the experiment can be paused for a short while, which should be excluded from the duration of the experiment.
(10) Hold the scraps up to the light. Observe the scraps as if observing the banknote watermark.
Rotate the scraps 90°, 180°, or 270°clockwise or counterclockwise, and then observe them.
1.8.2.1.2 Experimental results
(1) When the experiment has lasted 28 hours, it can be seen in the front of the lower scrap that in the centre there is an image of the numeral 2 looking like a watermark. As the duration of the experiment is longer and longer, the watermark-like image of the numeral 2 becomes clearer and clearer.
(2) When the experiment has lasted 48 hours, it can be seen that to the left of the watermark-like image of the numeral 2 mentioned above there appears a smaller watermark-like image of the numeral 2.
(3) To the upper right of the fairly large watermark-like image of the numeral 2 there appears a small watermark-like image of the numeral 3. Click here to view the picture. (The background light behind the scrap is the incandescent light, which is quite red.) (Click here to view the picture of a control sample.)
(4) During the course of the experiment, when the position of one scrap with respect to the other scrap has been slightly changed, the image on the upper scrap can still find the position of the watermark-like image in the lower scrap (i.e. automatic tracking), which makes the watermark-like image become clearer and clearer.
This shows that the watermark-like image has its own spacetime curvature, and hence has its own mass. This means that the watermark-like image is not only information but is also matter.
(5) When the "boat" has begun to move because of the work of the antigravitation engine, it may stay near the edge of the bathtub for a long time. In fact the boat is now moving in the potential barrier region (see Section 7.3.1), and its antigravitational acceleration, though very small, is not zero, in which case the experimental results mentioned above will still happen.
1.8.2.1.3 Experimental analysis
The time location and the space location of the upper and the lower scraps have all changed in the antigravitational field of the "boat". Hence in the non-present spacetime there is interaction between the two scraps (see also Section 6.13), and it looks as if the image of the numeral 2 on the upper scrap went through the glass jar, a layer of draught excluders stuck on the outside bottom of the jar (click here to view the picture), and the plastic disc box, and reached the lower scrap.
1.8.2.2 Some variations on Experiment 1
1.8.2.2.1 Experiment 2
(1) On a lower scrap draw an image of the numeral 3 with a black gel pen (Click here to view the picture). The upper scrap is a scrap of blank squared paper.
The picture of the upper scrap shows the results of the experiment, which lasted 163 hours. Click here to view the video.
(2) Experimental results (Click here to view the picture.)
In the lower left-hand part of the upper scrap there appears a fairly large dark watermark-like image of the numeral 3.
To the upper left of the tweezers there is a dark watermark-like image of a word "age" (antigravitation engine). The image of the word age was written in an earlier experiment, which was before the above Experiment 1, on a scrap (click here to view the picture taken afterwards), which, in that experiment, was placed under the outside bottom of the glass jar, between two blank scraps, and the three scraps had been taken away 28 days 4 hours before Experiment 2 began, or 8 days 17 hours before Experiment 1 began. The scraps used in Experiment 2 are two other scraps.
At the top right margin of the upper scrap there is a light watermark-like image of "ⓢ". The image of "ⓢ" was originally the image drawn on the lower scrap in a later experiment beginning 118 hours 45 minutes after Experiment 2 had finished (Click here to view the picture). The image was used because it looked somewhat like the Taiji symbol.
(3) Some events described above are listed below in date order.
(3.1)
26 February 2007 The image of the word age was written on a scrap.
26 February 2007—28 February 2007 The experiment in which there was the scrap with the image of “age” written on it.
28 February 2007 The scrap with the image of “age” written on it was taken away.
(3.2)
8 March 2007—15 March 2007 Experiment 1.
(3.3)
28 March 2007—5 April 2007 Experiment 2.
5 April 2007 The scraps used in Experiment 2 were taken away.
(3.4)
10 April 2007 The image of the circled letter S was drawn on a scrap.
10 April 2007—15 April 2007 The experiment in which there was the scrap with the image of the circled letter S drawn on it.
(3.5)
18 May 2007 The dark watermark-like image of the word "age" was found in the upper scrap used in Experiment 2.
27 May 2007 The light watermark-like image of the circled letter S was found in the upper scrap used in Experiment 2.
(4) The antigravitation engine has changed the non-present-spacetime images of the word age and the circled letter S into the present-spacetime images (see Section 7.26.1.5).
1.8.2.2.2 Experiment 3
Replace the glass jar with an airtight food storage container; and the batteries are also placed in this container.
The similar experimental results can be obtained.
1.8.2.2.3 Experiment 4
Place a double-sided mirror or a light aluminium basin (click here to view the picture) on the disc box.
The similar experimental results can be obtained.
1.8.2.3 Control experiments
Instead of putting the foam plastic board on the water in a bathtub, place the foam plastic board on the upper edge of a small basin full of water, or place the foam plastic board on a cushion on a table.
The other steps are the same as those in Experiment 1.
The experimental results described above can not be obtained in the control experiments.
1.8.3 Analyses
The experimental phenomena mentioned above can be resolved into the following phenomena which happen in an unusual way: going through a wall, moving things, fetching things, changing the shape, seeing through a wall, remote sensing, replicating oneself, automatic tracking, reappearing, preappearing, and changing the density of matter (the paper fibre).
1.9 Antigravitational non-local mathematics experiment
1.9.1 Steps of the experiment
Click here to view the picture.
(1) Prepare a scrap of blank squared paper which is to be placed at an upper position and hence is called the upper scrap hereafter.
(2) Lay the upper scrap face up at the inside bottom of the glass jar (see Section 1.2), under the base of a motor.
(3) Prepare a plastic box for holding a 3.5 inches floppy disc (hereafter called the disc box).
(4) Prepare a scrap of blank squared paper which is to be placed at a lower position and hence is called the lower scrap hereafter.
On the lower scrap write “3+2=?” with a black gel pen.
Click here to view the picture.
Lay the lower scrap face up in the disc box. Close the disc box.
(5) Place the disc box and the batteries on a foam plastic board, and place the glass jar on the disc box, in front of the batteries.
(6) Place the foam plastic board on the water in a bathtub. With the help of a level gage, adjust the positions of the things on the board to make the board horizontal.
(7) Start the motor, and the experiment begins.
In order to reduce |Σa'| (see Section 2.3 of Chapter 2), or in other words, in order to prevent the antigravitational acceleration from becoming zero too often, the experiment should not be long exposed to strong light.
(8) In order to observe the scraps of paper and to replace the batteries with newly charged ones, the experiment can be paused for a short while, which should be excluded from the duration of the experiment.
(9) When the experiment finishes, hold the upper scrap up to the light. Observe the scrap as if observing the banknote watermark. Take pictures of the upper scrap.
(10) If the message in the picture is not clear enough, the image in the picture can be processed by using Photoshop's Image > Adjust > Brightness/Contrast command, Image > Adjust > Posterize command, and Window > Channels > Green or Blue or Red command.
(11) Use Photoshop's Rotate command to rotate the image 90°, 180°, or 270° counterclockwise or clockwise, and then observe the image.
1.9.2 Experimental result
The picture of the upper scrap shows the result of the experiment, which lasted 135 hours 31 minutes.
Please click here to view the raw picture of the upper scrap. The image is unprocessed.
The background light behind the scrap is the incandescent light, which is quite red.
It can be seen in the upper scrap that there is an image of the numeral 5 looking like a watermark.
1.10 Concluding remarks
The above experiments demonstrate a variety of measurable effects of the gravitational field matter (see Chapter 2). In nature these effects can be observed in flying saucers and in foggoid (see Chapter 6).
As for experiment pictures, please see Chapter 8.
Let's make these experiments and carry forward the study of the flying saucer.
Chapter 1 An introduction to some antigravitation engine experiments that everyone can make
Chapter 2 The setting up of the set of equations of the antigravitation engine
Chapter 3 Know-how of the antigravitational mechanical experiment and range of application
Chapter
4 Data
analysis (to verify the macroscopic quantum mechanical phenomenon)
Chapter 5 Data analysis (mainly to verify Eq. (1) in Chapter 1)
Chapter 6 A new state of matter: foggoid state
Chapter 7 More about antigravitational experiments
