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© ABCC Australia 2015 new-physics.com
VISONIC TIME DILATION – OBJECT IN MOTION
Cosmic Adventure 5.8
© ABCC Australia 2015 new-physics.com
Though the situation is different
from that of the object at rest,
the results are t...
© ABCC Australia 2015 new-physics.com
𝒄 independent of Source
The speed of light is a constant
in the universe. This magni...
© ABCC Australia 2015 new-physics.com
A B
Real clock A
Actual time Actual time
Clock Image Reading on Leaving Clock B
To s...
© ABCC Australia 2015 new-physics.com
A B
Image of B
𝑐
Real clock A Real clock B
Actual time Actual timeFixed time
Clock I...
© ABCC Australia 2015 new-physics.com
Light Speed Constant
As discussed, no matter how
fast clock B will move, the
speed o...
© ABCC Australia 2015 new-physics.com
𝑣
A
Real clock A Real clock B
Situation 1
At time ∆t = 0, both clocks are at the sta...
© ABCC Australia 2015 new-physics.com
𝑣
A B
Real clock A Real clock B
Situation 2
After time = ∆𝑡1, clock B has travelled ...
© ABCC Australia 2015 new-physics.com
𝑣
A B
Real clock A Real clock BImage
𝑐
Time of image B
Reading ∆𝑡1
Situation 3 Image...
© ABCC Australia 2015 new-physics.com
𝑣
A B C
Real clock A Real clock BImage
𝑐
Situation 4
This image takes time ∆𝑡2 to re...
© ABCC Australia 2015 new-physics.com
𝑣
A B𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2
Image
C
𝑐
Real clock A Real clock B
Actual time
∆𝑡3= ∆𝑡1 + ∆𝑡2...
© ABCC Australia 2015 new-physics.com
𝑣
A BApparent position
𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2
Image
C
𝑐
Real clock A Real clock B
Actual t...
© ABCC Australia 2015 new-physics.com
Observation 1 – Actual Position & Time
The actual position of clock B is :
𝑥3 = 𝑥1 +...
© ABCC Australia 2015 new-physics.com
Observation 2 – Apparent Position & Time
The apparent position of clock B is:
𝑥1 = 𝑣...
© ABCC Australia 2015 new-physics.com
Ration of the two Times
𝐴𝑝𝑝𝑎𝑟𝑒𝑛𝑡 𝑇𝑖𝑚𝑒
𝐴𝑐𝑡𝑢𝑎𝑙 𝑇𝑖𝑚𝑒
=
∆𝑡1
1 +
𝑣
𝑐
∆𝑡1
=
1
1 +
𝑣
𝑐
𝑐
Ap...
© ABCC Australia 2015 new-physics.com
Light Speed Constancy
This result is the same as the
case where the object is at
res...
© ABCC Australia 2015 new-physics.com
Different between
Relativity & Visonics
This phenomenon exhibits an apparent
dilatio...
© ABCC Australia 2015 new-physics.com
Distance Change
Though there is no difference in
the change of time between the
obje...
© ABCC Australia 2015 new-physics.com
THE PERCEPTION
OF A LONG IMAGE
AT REST
To be continued on
Cosmic Adventure 5.9
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Cosmic Adventure 5.8 Time Dilation of Clocks in Motion in Visonics

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Time dilation phenomenon for clocks on the move in visonics. The result is the same as clocks at rest since the speed of light is not affected by the motion of the source.

Published in: Science
  • Light and its nature have caused a lot of ink to flow during these last decades. Its dual behavior is partly explained by (1)Double-slit experiment of Thomas Young - who represents the photon’s motion as a wave - and also by (2)the Photoelectric effect in which the photon is considered as a particle. A Revolution: SALEH THEORY solves this ambiguity and this difficulty presenting a three-dimensional trajectory for the photon's motion and a new formula to calculate its energy. More information on : https://youtu.be/mLtpARXuMbM https://www.slideshare.net/SalehTheory/saleh-theory?qid=e7da2b84-6d5e-409d-8b12-cae0f58a825b&v=&b=&from_search=1
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Cosmic Adventure 5.8 Time Dilation of Clocks in Motion in Visonics

  1. 1. © ABCC Australia 2015 new-physics.com VISONIC TIME DILATION – OBJECT IN MOTION Cosmic Adventure 5.8
  2. 2. © ABCC Australia 2015 new-physics.com Though the situation is different from that of the object at rest, the results are the same due to the constancy of light speed. Same as Clock at Rest
  3. 3. © ABCC Australia 2015 new-physics.com 𝒄 independent of Source The speed of light is a constant in the universe. This magnitude is independent of the emitting source or the reflecting object. This property is obvious in the following example. 𝑣 = 100 km/sec 𝑣 = 100,000 km/sec 𝑣 = 0 km/sec 𝑐 𝑐 𝑐
  4. 4. © ABCC Australia 2015 new-physics.com A B Real clock A Actual time Actual time Clock Image Reading on Leaving Clock B To start with, we have two clocks that are well synchronized and are placed in the same spot to start with. Both clocks register the same time 𝑡 = 0. Real clock B
  5. 5. © ABCC Australia 2015 new-physics.com A B Image of B 𝑐 Real clock A Real clock B Actual time Actual timeFixed time Clock Image Reading on Leaving Clock B As clock B leaves, it still keep on sending its images back to A. There is an image at every instant and we choose only one of them for demonstration purposes. Here we choose one sent at time = ∆𝑡 1. The clocks are still ticking normally, but the image only shows a fixed time of the moment. 𝑣 𝑥1 = 𝑣∆𝑡 1 ∆𝑡 1
  6. 6. © ABCC Australia 2015 new-physics.com Light Speed Constant As discussed, no matter how fast clock B will move, the speed of the image emitted will not be affected. It is 𝑐 all the time. So this situation is the same when clock B is stationary in. Both being stationary or moving will have no affect the speed of light. Speed of image of B 𝑐 Speed of real clock B 𝑣 The speed of clock B does not have any effect on the speed of its light image which is always c
  7. 7. © ABCC Australia 2015 new-physics.com 𝑣 A Real clock A Real clock B Situation 1 At time ∆t = 0, both clocks are at the starting position A. Clock A is at rest while clock be is moving at velocity 𝑣. Distance 𝑥 = 0 Time ∆t = 0
  8. 8. © ABCC Australia 2015 new-physics.com 𝑣 A B Real clock A Real clock B Situation 2 After time = ∆𝑡1, clock B has travelled to B, covering a distance 𝑥1 = 𝑣∆𝑡1. Both clocks now register the same time, that is, ∆𝑡1. 𝑥1 = 𝑣∆𝑡1 ∆𝑡 1
  9. 9. © ABCC Australia 2015 new-physics.com 𝑣 A B Real clock A Real clock BImage 𝑐 Time of image B Reading ∆𝑡1 Situation 3 Image Emission At this moment of time = ∆𝑡1, clock B sends an image (registering time ∆𝑡1) towards clock A, while keeps on traveling away from B. Clock B goes on
  10. 10. © ABCC Australia 2015 new-physics.com 𝑣 A B C Real clock A Real clock BImage 𝑐 Situation 4 This image takes time ∆𝑡2 to reach A at speed c. At the same time clock B has reached C with BC= ∆𝑥1= 𝑣∆𝑡2. The time is then ∆𝑡3 = ∆𝑡1 + ∆𝑡2 𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2 ∆𝑥1= 𝑣∆𝑡2
  11. 11. © ABCC Australia 2015 new-physics.com 𝑣 A B𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2 Image C 𝑐 Real clock A Real clock B Actual time ∆𝑡3= ∆𝑡1 + ∆𝑡2 Apparent time = ∆𝑡1 Situation 5 Actual time ∆𝑡3= ∆𝑡1 + ∆𝑡2 ∆𝑥 = 𝑣∆𝑡2 = 𝑣∆𝑡1 × 𝑣/𝑐
  12. 12. © ABCC Australia 2015 new-physics.com 𝑣 A BApparent position 𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2 Image C 𝑐 Real clock A Real clock B Actual time ∆𝑡3= ∆𝑡1 + ∆𝑡2 Apparent time = ∆𝑡1 Final Situation 6 Actual time ∆𝑡3= ∆𝑡1 + ∆𝑡2 ∆𝑥 = 𝑣∆𝑡2 = 𝑣∆𝑡1 × 𝑣/𝑐 Actual position 𝑥3 = 𝑣∆𝑡1 + 𝑣∆𝑡2
  13. 13. © ABCC Australia 2015 new-physics.com Observation 1 – Actual Position & Time The actual position of clock B is : 𝑥3 = 𝑥1 + ∆𝑥 = 𝑣∆𝑡1 + 𝑣∆𝑡1 𝑣/𝑐 = 1 + 𝑣 𝑐 𝑣∆𝑡1 = 1 + 𝑣 𝑐 𝑥1 The actual time of B is (same as A): ∆𝑡3 = ∆𝑡1 + ∆𝑡2 = 1 + 𝑣 𝑐 ∆𝑡1 Real clock A 𝑣 Real clock B
  14. 14. © ABCC Australia 2015 new-physics.com Observation 2 – Apparent Position & Time The apparent position of clock B is: 𝑥1 = 𝑣∆𝑡1 = 𝑐∆𝑡2 The clock reading of image B is ∆𝑡1. So the apparent time is: ∆𝑡1 Image of Clock B 𝑐
  15. 15. © ABCC Australia 2015 new-physics.com Ration of the two Times 𝐴𝑝𝑝𝑎𝑟𝑒𝑛𝑡 𝑇𝑖𝑚𝑒 𝐴𝑐𝑡𝑢𝑎𝑙 𝑇𝑖𝑚𝑒 = ∆𝑡1 1 + 𝑣 𝑐 ∆𝑡1 = 1 1 + 𝑣 𝑐 𝑐 Apparent [Image] time = ∆𝑡1 Actual [Clock A & B] time = 1 + 𝑣 𝑐 ∆𝑡1 𝑣
  16. 16. © ABCC Australia 2015 new-physics.com Light Speed Constancy This result is the same as the case where the object is at rest. It simply demonstrates the fact the speed of light is not affected by the motion of its sources. 𝑣 = 0 km/sec 𝑐 𝑣 = 1000 km/sec 𝑐
  17. 17. © ABCC Australia 2015 new-physics.com Different between Relativity & Visonics This phenomenon exhibits an apparent dilation of time. So it is called ‘time dilation’ in the theory of Special Relativity. But there is a difference. In Relativity, it is a real event. Time does slows down and leads to absurd events such as ‘twin paradox’. In visonics, this is an optical phenomenon, just like looking at clocks on distant stars in classical physics.
  18. 18. © ABCC Australia 2015 new-physics.com Distance Change Though there is no difference in the change of time between the object being at rest or in motion, a change in the position of the object is involved. We have to get the change in length to see the difference.
  19. 19. © ABCC Australia 2015 new-physics.com THE PERCEPTION OF A LONG IMAGE AT REST To be continued on Cosmic Adventure 5.9

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