Galaxy rotation curve #3 is the best curve to simulate. The speed increases lineair.
Galaxy rotation curve #4 is the most difficult to simulate. Constant C4= 0.1
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From the "Form Print" you can see that there is the large error between the target and the simulated galaxy curve.
The final target values are: 193.9 188.3 186.4 182.7 and 180.9 (decrease)
The final actual values are: 191.7 192.5 193.5 193.7 and 193.9 (flat)
The important lesson is: Galaxy rotation curves where there is a clear maximum speed and then the speed decreases can not be simulated using MOND
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Galaxy rotation curve #1 is the completely flat curve.
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Observe calculated rotation curve has the values 200.0 285.7 285.7 285.7 etc.
Most important lesson: There is no mass in the disc
This raises an each more serious problem When you measure the speed of the disc of a galaxy as being flat, than you can not explain that using MOND, because in that case there is no matter in the flat disc
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Galaxy rotation curves 1 and Black Hole
The purpose of these test is to observe the influence of a Black Hole
Test | Curve # | v | BH | loop count | error | total mass |
1 | 1 | 140 | 0 | 55 | 180 | 299850080 |
2 | 1 | 200 | 1 | 57 | 255,35 | 1229539440 |
3 | 1 | 200 | 1500 | 69 | 184,96 | 2083760232 |
4 | 1 | 200 | 15000 | 1000 | 1,227 | 15000003873 |
- Observe rotation curve has the values 140.0 200.0 200.0 200.0 200.0 etc.
- Observe rotation curve has the values 200.2 285,1 285,1 285,1 285,1 etc.
- Observe rotation curve has the values 200.0 261.6 261.6 261.6 261.6 etc.
- Observe rotation curve has the values 200.2 200.3 200.4 200.4 200.4 etc.
The important lesson is: By introducing a large BH you can get a complete flat galaxy rotation curve with MOND
Galaxy rotation curve 1 and MOND versus Newton
Test | Curve # | MOND | M Init | loop count | error | total mass |
1 | 1 | Off | | | | 111613713709 |
2 | 1 | On | Yes | 57 | 257,14 | 1248854956 |
3 | 1 | On | No | 10 | 35,863 | 116548964824 |
For test 1 the grv is: 200, 200, 200, 200, 200, 200, 200, 200, 200 and 200
For test 3 the grv is: 437, 706, 880, 1020, 1137, 1234,1319, 1385, 1440 and 1459
What can you learn from test 1 and 3 ?
- First, the main point is that the total mass and the mass distribution is identical but the rotation curve not
With Newton's Law the curve is flat but with MOND the speed increases almost lineair
- Secondly that the rotation curves, assuming the same baryonic mass distribution of a simulation based on Newton's Law compared to MOND are totally different.
Galaxy rotation curve 2 and a0 - fixed curve
The purpose of this test is to observe what happens if you MOND and the only parameter that is changed is a0. The rotation curve is the same.
Test | Curve # | a0 | loop count | error | total mass |
1 | 2 | 8 | 24 | 8,942 | 58447645 |
2 | 2 | 0.8 | 24 | 8,942 | 584476455 |
3 | 2 | 0.08 | 24 | 8,942 | 5844764551 |
What the test shows is that when you decrease a0 with a factor 10 the mass m0 is increased with a factor 10.
This behaviour is in agreement with the rule: v1 = SQR(SQR(G * m0 * a0)
This rule describes with v1 being constant when you decrease a0 with a factor 10, m0 should increase with a factor 10. And vice versa.
Important lesson: That by changing the Universal Constant a0 you can give the galaxy any mass value you like.
Galaxy rotation curve 2 and a0 - fixed mass
The purpose of this test is to demonstrate what happens with the rotation curve if you study the same mass distribution changing the parameter a0.
Starting point is rotation curve 2.
It is important that the parameter Loop count is set to -1, in order to prevent the mass calculation phase.
Test | Curve # | Mond | a0 | M init | V 1 | V 10 | loop count | error | total mass |
1 | 2 | Off | 8 | No | 200 | 200 | -1 | | 130252103693 |
2 | 2 | On | 8 | No | 216 | 1554 | -1 | 2826 | 130252103693 |
3 | 2 | On | 0.8 | No | 122 | 874 | -1 | 1360 | 130252103693 |
4 | 2 | On | 0.08 | No | 68 | 491 | -1 | 542 | 130252103693 |
5 | 2 | On | 0.008 | No | 38 | 276 | -1 | 140 | 130252103693 |
6 | 2 | On | 0.0008 | No | 21 | 155 | -1 | 234 | 130252103693 |
What can you learn from the above test?
In the tests we keep the total baryonic mass constant. MOND is tetsted by modifying a0
- With Newtons'Law we get a flat curve with speed 200.0
- With MOND we get a curve which lies below this curve
- IMO what this means is to use MOND in order to explain dark matter is highly speculative.
Galaxy rotation curve 2, # stars, MOND versus Newton
The purpose of this test is to demonstrate what the difference is between Newton and MOND when the total number of stars is different
Starting point is rotation curve 2.
Test | Curve # | # star | MOND | total mass | Mond | total mass |
1 | 2 | 25 | On | 119435874 | Off | 131093341851 |
2 | 2 | 50 | On | 58447645 | Off | 130252103693 |
3 | 2 | 100 | On | 29103195 | Off | 128614178511 |
4 | 2 | 200 | On | 14463346 | Off | 127071520697 |
What the results show is that the total mass of a Galaxy is independent of the number of stars when Newton is considered. This is as expected.
With Newton when the number of stars is increased with a factor of two, the mass of each star is decreased with a factor of two and this has no influence on the overall rotating curve of the galaxy.
For MOND the result is different. The total mass decreases when the # of stars increases.
With MOND when the number of stars is increased with a factor of two, the mass of each star is decreased with a factor of four, in order to explain that the total mass decreases with a factor of two and as such has no influence on the overall rotating curve of the galaxy.
At the same time if you assume that the total mass stays constant (like with Newton) than an increases in the number of stars with MOND will change the overall speed pattern of the Galaxy.
Extended disc with Newton - Curve 6
Curve #6 is special. In this case the galaxy mass is directly calculated. This allows to compare the same mass distribution under different circumstances i.e the visibility of the stars.
Test | #ring | #star | Mond |
Ext disk | Con C6 | V nr | dens nr | Total mass |
1 | 10 | 50 | Off | 1 | 1 | 221.4 |
4.27 | 144590730173 |
2 | 10 | 50 | Off | 1 | 3 | 144 |
0.57 | 73078628956 |
3 | 10 | 50 | Off | 1 | 1.6 | 177.3 |
2.34 | 112955607832 |
4 | 20 | 50 | Off | 2 | 1 | 183.6 |
0.76 | 199868406309 |
5 | 20 | 50 | Off | 2 | 1.6 | 141.6 |
0.23 | 136172354007 |
- Test 1 demonstrates the observed galaxy rotation curve. the grc is almost flat.
- Test 2 shows the calculated grc. Test 2 is based on the observed stars and based on visibility the "observed" mass. The difference.
When you compare the two there is a missing matter of roughly 7 * 10^10 solar masses or roughly 50.
- In the following tests improved visibility is studied.
Test 3 shows the calculated grc when the number of observed stars and "observed" mass increases.
The amount of missing matter roughly 4 * 10^10 solar masses or roughly 28%.
- At the same time when the visibility is improved also the size of the disc increases.
Test 4 demonstrates the observed galaxy rotation curve.
- Test 5 demonstrates the observed galaxy rotation curve.
The amount of missing matter roughly 6.3 * 10^10 solar masses or roughly 31%.
Important lesson: When observation equipment improves the amount of missing matter to explain the observed galaxy rotation curve decreases.
Program Evaluation - With simulation
The following are tests are all done with a real simulation.
Starting point are the standard parameters.
Ater the message:
- Perform Simulation ?
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Select Yes Command
In the following table are 6 tests. The parameter disp # is at the top right corner of the display form. The value 1 means that only 1 star in each ring is displayed.
Test | Curve # | Ext Disk | Mond | disp # | # ring | # stars | chaos | loop count | error | total mass |
1 | 2 | 1 | Off | 100 | 10 | 25 | 60 | | | 131093341851 |
2 | 2 | 1 | On | 100 | 10 | 25 | 400 | 24 | 9,852 | 119435874 |
3 | 5 | 1 | Off | 100 | 10 | 25 | 90 | | | 121112362053 |
4 | 5 | 1 | On | 100 | 10 | 25 | 2000 | 29 | 0,138 | 185041948 |
5 | 2 | 1 | Off | 1 | 10 | 25 | 60 | | | 131093341851 |
6 | 2 | 1 | On | 1 | 10 | 25 | 400 | 24 | 9,852 | 119435874 |
7 | 5 | 1 | Off | 1 | 10 | 25 | 90 | | | 121112362053 |
8 | 5 | 1 | On | 1 | 10 | 25 | 2000 | 29 | 0,138 | 185041948 |
9 | 4 | 2 | Off | 2 | 20 | 30 | 90 | | | 532103053781 |
10 | 4 | 2 | On | 2 | 20 | 30 | 2000 | 29 | 0,138 | 1229720034 |
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The tests 1 to 4 have a display number of 100. That means the simulation shows all the stars.
When you start each simulation you will observe that all the stars follow each other in circles.
This stabble pattern will continue for some time until you will observe that some stars will move away, are jected and "chaos" start at a certain angle. This angle is the parameter chaos in the above table. This chaotical pattern is strictly a behaviour of the accuracy of the simulation and not so much a physical phenomena. When you compare MOND with Newton than MOND is more stable.
A whole different issue is at stake in the tests 5 to 8. In that case only one star is displayed (because disp # = 1). In test 5 and 6 ( with curve # = 2) after the start of the simulation you will observe an almost flat galaxy rotation curve as expected.
The most difficult issue with MOND is that you cannot simulate the solar system.
A similar problem is that you cannot simulate a Galaxy Rotation curve which after the bulge reaches its maximum speed and than very slowly starts to decrease. In such a case with MOND the curve stays flat and there is no mass at all in the disc. This is a serious problem.
A whole different problem that when two stars merge with Newton this has almost no influence on the stars in its neighbourhood.
See also: Philosophical considerations about galaxy simulations
See also: Scientific American September 2015. How Einstein reinvented Reality
Reflection 2 - Visual Basic 5.0 versus Visual Studio 2010
When you compare Visual Basic with Visual Stodio than Visual Basic is the winner.
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Created 18 September 2015
Updated 22 March 2016
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