Possible Charged Particle Field
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Re: Possible Charged Particle Field
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I've retried a 9 particles in a row about 24X earlier today without seeing any overlapped particles. I don't recall ever seeing a single row with overlapped particles. I DO however, see plenty of pushed particles  particles to the right of their finish marks  occur in single rows. There's no evidence that particles have been pushed using my console settings today. I just saw velocity transfers.
I tried two rows next. 18 particles: two rows of nine particles. Both initial velocities equal 30. 20 or so times also without observing overlap. Again, I may see slightly pushed particles.
24 particles: pOne  pEight. Three rows, velocities 10,20,and 30. Finally saw two overlapped particles, shown in the gif above. Particles three and four almost entirely overlap, but separate before both lost their velocities. Particle 5 picked up the same velocity but it pushed particle 6.
Here's an image showing that pushed particle 6.
I submitted a customer service work ticket with bitbucket about twelve hours ago.
Tried using the debugger after normalization, but it would always stop at the very first collision encountered. How to make an exception? So I commented it out.
I trimmed the console output to just the top row's velocity changes. I haven't figured it out yet. The console output follows. The mix of velocity magnitudes of .999s or round integers suggest there may be an easy ( float v.sub( v1 );///? fix but I don't see a direct link between 999s, integer like #s and pushes.
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Can you reproduce the problem with only a single line of neutrons? Having so many makes it difficult to step through the code or to interpret console output. It doesn't seem like the number of neutrons should matter, but it would be interesting if it did.
I've retried a 9 particles in a row about 24X earlier today without seeing any overlapped particles. I don't recall ever seeing a single row with overlapped particles. I DO however, see plenty of pushed particles  particles to the right of their finish marks  occur in single rows. There's no evidence that particles have been pushed using my console settings today. I just saw velocity transfers.
I tried two rows next. 18 particles: two rows of nine particles. Both initial velocities equal 30. 20 or so times also without observing overlap. Again, I may see slightly pushed particles.
24 particles: pOne  pEight. Three rows, velocities 10,20,and 30. Finally saw two overlapped particles, shown in the gif above. Particles three and four almost entirely overlap, but separate before both lost their velocities. Particle 5 picked up the same velocity but it pushed particle 6.
Here's an image showing that pushed particle 6.
I submitted a customer service work ticket with bitbucket about twelve hours ago.
Tried using the debugger after normalization, but it would always stop at the very first collision encountered. How to make an exception? So I commented it out.
I trimmed the console output to just the top row's velocity changes. I haven't figured it out yet. The console output follows. The mix of velocity magnitudes of .999s or round integers suggest there may be an easy ( float v.sub( v1 );///? fix but I don't see a direct link between 999s, integer like #s and pushes.
 Code:
///////////////////////// Collision between particles 12
//// pOne velocity lost. From v1=30, v2=0.
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
//// pTwo velocity increase. v1=0, v2=30.
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///////////////////////// Collision between particles 23
//// pTwo velocity lost. From v1=30, v2=0.
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 29.999999999999996
cdm.js:769 a2: 0
cdm.js:806 v: 29.999999999999993, 0, 0
//// pThree velocity increase. v1=0, v2=30.
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 29.999999999999996
cdm.js:806 v: 29.999999999999993, 0, 0
///////////////////////// Collision between particles 34
//// pThree velocity lost. From v1=30, v2=0.
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
//// pFour velocity increase. v1=0, v2=30.
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///Pattern break.
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 29.999999999999996
cdm.js:806 v: 29.999999999999993, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 29.999999999999996
cdm.js:769 a2: 0
cdm.js:806 v: 29.999999999999993, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 29.999999999999996
cdm.js:806 v: 29.999999999999993, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 29.999999999999996
cdm.js:769 a2: 0
cdm.js:806 v: 29.999999999999993, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///////////////////////// Collision between particles 45
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///////////////////////// Collision between particles 56
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///////////////////////// Collision between particles 67
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 30
cdm.js:769 a2: 0
cdm.js:806 v: 30, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 30
cdm.js:806 v: 30, 0, 0
///////////////////////// Collision between particles 78
cdm.js:746 v1: 30, 0, 0
cdm.js:747 v2: 0, 0, 0
cdm.js:768 a1: 29.999999999999996
cdm.js:769 a2: 0
cdm.js:806 v: 29.999999999999993, 0, 0
cdm.js:746 v1: 0, 0, 0
cdm.js:747 v2: 30, 0, 0
cdm.js:768 a1: 0
cdm.js:769 a2: 29.999999999999996
cdm.js:806 v: 29.999999999999993, 0, 0
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LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
Don't worry about those 29.99999999996 type values. They are just rounding errors in the math. Nothing we can do about it that does not involve more expensive operations (by using higher precision numbers). They are annoying, and they will leave residual velocities where there shouldn't be, but they will be so small as to be unnoticeable unless you just leave it sitting there for a really long time and eventually notice that a particle you thought wasn't moving, has actually moved. They certainly aren't causing our problem.
All of that console output looks fine. Did you actually see an error happen while that output was being generated? I really need to see it when there is an error.
All of that console output looks fine. Did you actually see an error happen while that output was being generated? I really need to see it when there is an error.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
All of that console output looks fine. Did you actually see an error happen while that output was being generated? I really need to see it when there is an error.
Correct, although that output isn't fine, it's filled with many additional velocity changes, the twitches you observed in overlapped particles. The gif and console output are from the same collision error event which I observed. I still have it on my browser. I was grateful to find such a compact event. All other collision errors console outputs I observed were much longer, 1 or 2 thousand lines. It's remarkable that all such overlapping events I observed involved the same velocities  just the initial velocities from that row.
I'll try to find a collision error that involves a velocity different from the initial row velocity tomorrow.
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LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
I don't see an errors in that output. Can you point out what you see?
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
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Sorry I wasn't clear. An eight particle row without any collision errors results in 7 collisions with a total of 14 velocity changes. In the console output above, I inserted some commentary. The error involves the 36 velocity changes after "Collision between particles 34"... "pattern break" and "Collision between particles 45". All those velocity changes involve 30, 0 and 30 velocities. I suppose unequal numbers of those velocities may add up to fractional speeds, but I don't see how particles can move faster than just those velocities, so that's the error case I'll look for tomorrow.
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Sorry I wasn't clear. An eight particle row without any collision errors results in 7 collisions with a total of 14 velocity changes. In the console output above, I inserted some commentary. The error involves the 36 velocity changes after "Collision between particles 34"... "pattern break" and "Collision between particles 45". All those velocity changes involve 30, 0 and 30 velocities. I suppose unequal numbers of those velocities may add up to fractional speeds, but I don't see how particles can move faster than just those velocities, so that's the error case I'll look for tomorrow.
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LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
I don't think that is correct. The output will follow the algorithm. Add another console.log at the start of the calculateCollision method that writes the index1 and index2 values for you. Then you know which particles are interacting.
console.log( 'P1: ' + index1 + ', P2: ' + index2 );
console.log( 'P1: ' + index1 + ', P2: ' + index2 );
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
Basically, the twitching happens across multiple frames, never within the same frame as your interpretation of the output would suggest.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
Unless those are the only colliding particles, then you would be correct. I don't know right now. It is suggesting that the change in velocity is not being added to the position of the particles under some circumstances. I'll have a look into that code tonight.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
No luck.
I didn't find any problems with the addition of velocities or updating the position with that velocity. I added in some console.logs to make sure that things were executing as I thought they should be, and they were. I then decided to rewrite the algorithm without using the internal memory buffers, so that it would just retrieve the position, orientation, velocity and spin from the Particle object itself (which will be faster), but that didn't help either.
The main reason I did that was because the memory buffers use a Float32Array object, which are 32bit floats, not 64bit floats, and it might be a number precision problem. It wasn't. I will probably factor that code in anyway, just for the performance gain and I don't think we can use shaders in the way that I wanted to so they are not needed. I keep finding conflicting information about using shaders and don't know what to believe at the moment.
I'm nearly at the point where I want to use a different collision algorithm.
I didn't find any problems with the addition of velocities or updating the position with that velocity. I added in some console.logs to make sure that things were executing as I thought they should be, and they were. I then decided to rewrite the algorithm without using the internal memory buffers, so that it would just retrieve the position, orientation, velocity and spin from the Particle object itself (which will be faster), but that didn't help either.
The main reason I did that was because the memory buffers use a Float32Array object, which are 32bit floats, not 64bit floats, and it might be a number precision problem. It wasn't. I will probably factor that code in anyway, just for the performance gain and I don't think we can use shaders in the way that I wanted to so they are not needed. I keep finding conflicting information about using shaders and don't know what to believe at the moment.
I'm nearly at the point where I want to use a different collision algorithm.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
With respect to your SourceTree issues, have you updated the app? Does it need an update? There is a flag in the top right corner of the app (on Windows, Mac may be different) and if it is orange, then it wants you to look at it. Sometimes it is just some question but it may be an update notification. I think there were some major updates recently and they required me to login in via the website before SourceTree would login again.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
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WARNING. A lot of ugly follows. Nevyn, you don't sound like you're enjoying yourself, maybe you shouldn't look.
Collision error. Below, A 2X5 collision grid is shown, with particles left to right P0 – P4 on the bottom row, and P5 – P9 on the top  complying with their actual index numbers as referred to in the console output. The horizontal distance between particles is 10, vertical separation is 7.5. P0 is given an initial velocity, v = 30. The top row’s leftmost particle, P5 is given an initial v = 40. The error collision – overlapped particles  occurred in the top row. The bottom row contains 3 pushed particles – a problem which doesn’t seem to be indicated by the current console output. The image below is selfexplanatory. The above gif and following closeup details show just the center portion of the top row – the area is shown by the yellow rectangle.
The particle numbers have been changed from my previous descriptions on order to agree with the console output. The thin yellow line at the bottom right shows that p2 pushed p3 before the velocity transfers occurred.
Note that p5 slides under p6 about halfway before p6 joins in and movs to the right. P7/P8 looks to be the one clean collision that occurred in the top row. Three of the four particles in the second row are pushed.
I’ll post the Console output in the next post or two.
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WARNING. A lot of ugly follows. Nevyn, you don't sound like you're enjoying yourself, maybe you shouldn't look.
Collision error. Below, A 2X5 collision grid is shown, with particles left to right P0 – P4 on the bottom row, and P5 – P9 on the top  complying with their actual index numbers as referred to in the console output. The horizontal distance between particles is 10, vertical separation is 7.5. P0 is given an initial velocity, v = 30. The top row’s leftmost particle, P5 is given an initial v = 40. The error collision – overlapped particles  occurred in the top row. The bottom row contains 3 pushed particles – a problem which doesn’t seem to be indicated by the current console output. The image below is selfexplanatory. The above gif and following closeup details show just the center portion of the top row – the area is shown by the yellow rectangle.
The particle numbers have been changed from my previous descriptions on order to agree with the console output. The thin yellow line at the bottom right shows that p2 pushed p3 before the velocity transfers occurred.
Note that p5 slides under p6 about halfway before p6 joins in and movs to the right. P7/P8 looks to be the one clean collision that occurred in the top row. Three of the four particles in the second row are pushed.
I’ll post the Console output in the next post or two.
.
Last edited by LongtimeAirman on Thu Aug 09, 2018 10:19 pm; edited 1 time in total
LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
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Console output. Each row of 5 particles should result in just 4 collisions, (51); times 2 rows, for a total of eight collisions. Given the output variables required at every collision: v1, v2, P1, P2, a1, a2, and v, every nonerror collision requires 12 console output lines. We would expect 8*12 or 96 output lines for 8 error free collisions. In this case, row 2 collisions make up 48 lines of the console output. The total number of lines, after removing the line 1 three,js, from the top the console output is exactly 1,000. That would be equal to 1000/12 = 83.33 collisions. That’s my rough summary, I no doubt have details wrong. I concentrated on presentation, I also need to study it. For example; Why is P1: 6, P2: 7 the first collision, shouldn’t it be P1: 5 and P2: 6?? I’ll place a copy of the console output into my GitFolder, but I guess it won’t be pushed for some time. So, without further ado.
I hope you'll be requesting position locations next?
Thanks for that Sourcetree idea, I'll look into it.
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Console output. Each row of 5 particles should result in just 4 collisions, (51); times 2 rows, for a total of eight collisions. Given the output variables required at every collision: v1, v2, P1, P2, a1, a2, and v, every nonerror collision requires 12 console output lines. We would expect 8*12 or 96 output lines for 8 error free collisions. In this case, row 2 collisions make up 48 lines of the console output. The total number of lines, after removing the line 1 three,js, from the top the console output is exactly 1,000. That would be equal to 1000/12 = 83.33 collisions. That’s my rough summary, I no doubt have details wrong. I concentrated on presentation, I also need to study it. For example; Why is P1: 6, P2: 7 the first collision, shouldn’t it be P1: 5 and P2: 6?? I’ll place a copy of the console output into my GitFolder, but I guess it won’t be pushed for some time. So, without further ado.
 Code:
cdm.js:748 v2: 0, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 0
cdm.js:807 v: 40, 0, 0
cdm.js:746 P1: 6, P2: 7
cdm.js:747 v1: 40, 0, 0
cdm.js:748 v2: 0, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 0
cdm.js:807 v: 40, 0, 0
cdm.js:746 P1: 7, P2: 6
cdm.js:747 v1: 0, 0, 0
cdm.js:748 v2: 40, 0, 0
cdm.js:769 a1: 0
cdm.js:770 a2: 40
cdm.js:807 v: 40, 0, 0
cdm.js:746 P1: 5, P2: 6
cdm.js:747 v1: 40, 0, 0
cdm.js:748 v2: 40, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 40
cdm.js:807 v: 80, 0, 0
cdm.js:746 P1: 6, P2: 5
cdm.js:747 v1: 40, 0, 0
cdm.js:748 v2: 40, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 40
cdm.js:807 v: 80, 0, 0
cdm.js:746 P1: 5, P2: 6
cdm.js:747 v1: 40, 0, 0
cdm.js:748 v2: 40, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 40
cdm.js:807 v: 80, 0, 0
cdm.js:746 P1: 6, P2: 5
cdm.js:747 v1: 40, 0, 0
cdm.js:748 v2: 40, 0, 0
cdm.js:769 a1: 40
cdm.js:770 a2: 40
cdm.js:807 v: 80, 0, 0
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I hope you'll be requesting position locations next?
Thanks for that Sourcetree idea, I'll look into it.
.
LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
I am thinking about changing the way these functions are called. They are currently implemented to look for a collision that has just occurred but I want to change it to look for collisions that are about to occur.
Unfortunately, that is a bit difficult. The problem is that I have specified velocities in world units, such as m/s (the seconds is what matters), and I adjust the actual velocity used for a given frame by using the amount of time since the last frame. So if 1/60th of a second has past since the last frame, then I use 1/60th of the velocity. This has the advantage of using the correct amount of velocity for the given time (even if it was 1/45th of a second or 1/73.563). To look for a collision that might happen, I need to know the actual velocity being used, not the real world value, because I need to project into the future to see what will happen.
I just need to find a way around that. I will probably need to pass in the frame time to these methods to do so.
There probably isn't much point to you debugging this issue. Of course, it's a great exercise in finding problems and it really makes you figure out what the code is really doing and why, so you can continue if you want.
I really appreciate the effort you have put in. Also for pushing when you weren't happy with my responses. I haven't been thinking clearly, as my conflicting posts show, so it has been a savinggrace that you haven't just accepted whatever I say or just sat back and waited for me to fix it. Even if I am correct, you need to understand why I am correct and the same thing applies to me. We aren't just building an application, the real important stuff is transferring information and skills, and you have not let yourself down by being a passive student.
Unfortunately, that is a bit difficult. The problem is that I have specified velocities in world units, such as m/s (the seconds is what matters), and I adjust the actual velocity used for a given frame by using the amount of time since the last frame. So if 1/60th of a second has past since the last frame, then I use 1/60th of the velocity. This has the advantage of using the correct amount of velocity for the given time (even if it was 1/45th of a second or 1/73.563). To look for a collision that might happen, I need to know the actual velocity being used, not the real world value, because I need to project into the future to see what will happen.
I just need to find a way around that. I will probably need to pass in the frame time to these methods to do so.
There probably isn't much point to you debugging this issue. Of course, it's a great exercise in finding problems and it really makes you figure out what the code is really doing and why, so you can continue if you want.
I really appreciate the effort you have put in. Also for pushing when you weren't happy with my responses. I haven't been thinking clearly, as my conflicting posts show, so it has been a savinggrace that you haven't just accepted whatever I say or just sat back and waited for me to fix it. Even if I am correct, you need to understand why I am correct and the same thing applies to me. We aren't just building an application, the real important stuff is transferring information and skills, and you have not let yourself down by being a passive student.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
.
I saw that flag in Sourcetree. Click on it and it says Tell us what you think. So I ignored it since. This time I saw that yes, a sourcetree update was available, so I did. After restarting I tried to Push and experienced the same error as before. No joy.
I repeat, this is a great learning opportunity. Frame breaking isn't that difficult, but I'm nowhere near understanding how you've got this application wired else I'd have given you even more grief. I need to study it, even if you don't end up using it. As far as ideas go, I don't like the particle charge emission range = 10. You might consider a charge range limit, based on an angular limit  like the moon and the sun are apparently the same size. Monitor distance^2 just within smaller or closer groups. Or what about gravity? Just messin' with ya.
I admit, part of my effort is to motivate you. You've held up easily, doing a huge amount of work I'm barely able to appreciate. Relax and get your thoughts in order.
.
I saw that flag in Sourcetree. Click on it and it says Tell us what you think. So I ignored it since. This time I saw that yes, a sourcetree update was available, so I did. After restarting I tried to Push and experienced the same error as before. No joy.
I repeat, this is a great learning opportunity. Frame breaking isn't that difficult, but I'm nowhere near understanding how you've got this application wired else I'd have given you even more grief. I need to study it, even if you don't end up using it. As far as ideas go, I don't like the particle charge emission range = 10. You might consider a charge range limit, based on an angular limit  like the moon and the sun are apparently the same size. Monitor distance^2 just within smaller or closer groups. Or what about gravity? Just messin' with ya.
I admit, part of my effort is to motivate you. You've held up easily, doing a huge amount of work I'm barely able to appreciate. Relax and get your thoughts in order.
.
LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
I did exactly the same thing with that orange flag, until a colleague pointed out that it had an update in it.
After updating SourceTree, go to the BitBucket website and login there. Then restart SourceTree and see if you can push. Also, reenter your password to SourceTree, just in case it has lost it (Tools > Options > Authentication tab).
I agree about that emission range. It is a temporary approximation and will be replaced by a 1/r^4 type calculation. Some of the charge interaction code will need to change for the same reason. It is just a rough approximation at the moment and can be made better now that we know the rest of the algorithm works. The current charge code is a linear progression as you move further away from the emitter, which is clearly not right. I was focused on the equator to pole relationship of charge emission and how to process that, so the actual charge calculations were just rough calculations to get something close to what I wanted.
I did some research into the proper math and ran into a problem, which also applies to gravity at this level. Miles' work on that stuff is based on planets and moons. We are working with protons and other tiny particles. Miles takes some time to explain that the 1/r^2 relationship of gravity is actually an outcome of time/distance separation. It takes more time for the charge from the Sun to reach Saturn than it does the Earth, therefore at the exact same moment, Saturn sees older charge (which came from a smaller Sun) than the Earth does. We do not have such time/distance separations and I need to know how to remove such assumptions from the equations.
After updating SourceTree, go to the BitBucket website and login there. Then restart SourceTree and see if you can push. Also, reenter your password to SourceTree, just in case it has lost it (Tools > Options > Authentication tab).
I agree about that emission range. It is a temporary approximation and will be replaced by a 1/r^4 type calculation. Some of the charge interaction code will need to change for the same reason. It is just a rough approximation at the moment and can be made better now that we know the rest of the algorithm works. The current charge code is a linear progression as you move further away from the emitter, which is clearly not right. I was focused on the equator to pole relationship of charge emission and how to process that, so the actual charge calculations were just rough calculations to get something close to what I wanted.
I did some research into the proper math and ran into a problem, which also applies to gravity at this level. Miles' work on that stuff is based on planets and moons. We are working with protons and other tiny particles. Miles takes some time to explain that the 1/r^2 relationship of gravity is actually an outcome of time/distance separation. It takes more time for the charge from the Sun to reach Saturn than it does the Earth, therefore at the exact same moment, Saturn sees older charge (which came from a smaller Sun) than the Earth does. We do not have such time/distance separations and I need to know how to remove such assumptions from the equations.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
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Hey Nevyn, you may have noticed I Pushed to Bitbucket. Customer Service recommended I install a windows bug fix Git Credential Manager for Windows 1.17.0 and remove all bitbucket credentials from my Windows Credential Manager. It worked!
I'm looking at separation distances for the collision errors and was aghast at the overlap distances  for nonerror collisions too. The easiest fix may be improved collision detection. I wonder if I could import the console output into excel or R and do this sort of thing automatically.
Tracking the time necessary for separation distances fixes the scale of particle interaction. I agree, a larger scale requires more time. I would assume we have a constant scale for any given particle configuration.Whether we simulate proton or planet, we are adjusting time differentials to account for the motions that we are creating. Sorry if I'm missing the gist.
.
Hey Nevyn, you may have noticed I Pushed to Bitbucket. Customer Service recommended I install a windows bug fix Git Credential Manager for Windows 1.17.0 and remove all bitbucket credentials from my Windows Credential Manager. It worked!
I'm looking at separation distances for the collision errors and was aghast at the overlap distances  for nonerror collisions too. The easiest fix may be improved collision detection. I wonder if I could import the console output into excel or R and do this sort of thing automatically.
Tracking the time necessary for separation distances fixes the scale of particle interaction. I agree, a larger scale requires more time. I would assume we have a constant scale for any given particle configuration.Whether we simulate proton or planet, we are adjusting time differentials to account for the motions that we are creating. Sorry if I'm missing the gist.
.
LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
Yeah, that's basically it. A planet is a long distance from its star, so it takes time for the charge to reach that planet, even at the extreme speed that charge moves at. But it takes virtually no time for a charge photon to move from one proton to another if they are close enough to be interacting. So we don't need to include the distance separation in that way.
I have been playing with numbers again, and I think I see a way to calculate the charge strengths we want. Instead of a 1/r^4 calculation, it will be a 1/r^3 based equation. That is because it only uses the reduction in volume associated with that distance and not the time, which would bring in the distance again and give us r^4.
Volume of a Sphere: (4*Pi*r^3)/3
A radius of 1 represents the boundary of the emitter. That is the highest charge strength or charge density, which ever way you want to look at it.
A radius of 10 represents the furthest point away from the emitter in this dataset. Note that the radius is from the center of the emitter, not the boundary.
What we are looking at here is how and why the charge diminishes with distance. The particle only emits a certain amount of charge, at any given time or over some set time period, and that is constant (for our purposes here, it can change if the ambient field density changes but would still be a constant for us as we are working relative to the ambient field). So as that charge moves away from the particle, it inhabits a larger volume. The same amount of charge in a greater volume means less density.
So we want to look at how that volume changes as we use a greater radius. You can perform a little bit of calculus on it and find that the 3rd derivative, which is the constant derivative, has a value of 25.1327412287. That doesn't really tell us anything though. So let's take some ratios and see what it tells us.
Firstly, we will divide each volume by the first volume to see how many of the initial volume can fit into the larger volumes. In essence, this is making all volumes relative to the first volume.
A few of those numbers look familiar, and a quick analysis shows that each value is r^3. That wasn't too surprising, since we are using an r^3 equation, but I thought it worth showing as a stepping stone to the next part of this analysis.
That number tells us how much charge we could fit into each volume if we wanted to keep the charge density constant. But we don't want to keep the density constant, we want to keep the amount of charge constant and allow the density to change. So we are looking for the inverse of that value. We want to know how a given amount of charge will fit into a larger volume so we want to divide the first volume by each other volume.
Now we have a number that means something to us. We can take that number and multiply it by the charge strength at the particle boundary and get the charge strength at that volume. We will actually use the 1/r^3 equation to find the value for any radius. I did think about using a lookup table like this but the equation isn't that expensive so it isn't worth it. Precision is more important.
So my initial guess of the maximum charge emission range being 10 radii is pretty good. At that distance, the charge strength should be 1000 times less than at the particle boundary. Is it a coincidence that the Earth's chargepause, which sets the magnetopause and others, is also at 11 to 12 radii? I think not. In fact, I know not because it is the same reasons for both. If I had realised that when I created the constant in the code I would have used 11 or 12 instead.
So now we have an equation to calculate the charge at a given distance: C(d) = C(1)/d^3
Please note that I am using an equation within an equation. C is an equation to calculate the charge density or strength given a radius. So that equation explicitly states: The charge density at d is equal to the charge density at 1 divided by d^3. The charge density equation could be as simple as mass times volume, maybe mass times surface area or it could be more convoluted.
This is a quantum equation. It does not apply to macroscale numbers. We are ignoring time because the particles are close enough to do so, stars, planets, and moons are not, so it becomes a d^4 equation instead.
I have been playing with numbers again, and I think I see a way to calculate the charge strengths we want. Instead of a 1/r^4 calculation, it will be a 1/r^3 based equation. That is because it only uses the reduction in volume associated with that distance and not the time, which would bring in the distance again and give us r^4.
Analysis of Volume
Volume of a Sphere: (4*Pi*r^3)/3
Radius  Volume 
1  4.1887902048 
2  33.5103216383 
3  113.0973355292 
4  268.0825731063 
5  523.5987755983 
6  904.7786842339 
7  1436.7550402417 
8  2144.6605848506 
9  3053.6280592893 
10  4188.7902047864 
A radius of 1 represents the boundary of the emitter. That is the highest charge strength or charge density, which ever way you want to look at it.
A radius of 10 represents the furthest point away from the emitter in this dataset. Note that the radius is from the center of the emitter, not the boundary.
What we are looking at here is how and why the charge diminishes with distance. The particle only emits a certain amount of charge, at any given time or over some set time period, and that is constant (for our purposes here, it can change if the ambient field density changes but would still be a constant for us as we are working relative to the ambient field). So as that charge moves away from the particle, it inhabits a larger volume. The same amount of charge in a greater volume means less density.
So we want to look at how that volume changes as we use a greater radius. You can perform a little bit of calculus on it and find that the 3rd derivative, which is the constant derivative, has a value of 25.1327412287. That doesn't really tell us anything though. So let's take some ratios and see what it tells us.
Firstly, we will divide each volume by the first volume to see how many of the initial volume can fit into the larger volumes. In essence, this is making all volumes relative to the first volume.
Radius  Volume  V(n) / V(1) 
1  4.1887902048  1 
2  33.5103216383  8 
3  113.0973355292  27 
4  268.0825731063  64 
5  523.5987755983  125 
6  904.7786842339  216 
7  1436.7550402417  343 
8  2144.6605848506  512 
9  3053.6280592893  729 
10  4188.7902047864  1000 
A few of those numbers look familiar, and a quick analysis shows that each value is r^3. That wasn't too surprising, since we are using an r^3 equation, but I thought it worth showing as a stepping stone to the next part of this analysis.
That number tells us how much charge we could fit into each volume if we wanted to keep the charge density constant. But we don't want to keep the density constant, we want to keep the amount of charge constant and allow the density to change. So we are looking for the inverse of that value. We want to know how a given amount of charge will fit into a larger volume so we want to divide the first volume by each other volume.
Radius  Volume  V(n) / V(1)  V(1) / V(n) 
1  4.1887902048  1  1 
2  33.5103216383  8  0.125 
3  113.0973355292  27  0.037037037 
4  268.0825731063  64  0.015625 
5  523.5987755983  125  0.008 
6  904.7786842339  216  0.0046296296 
7  1436.7550402417  343  0.0029154519 
8  2144.6605848506  512  0.001953125 
9  3053.6280592893  729  0.0013717421 
10  4188.7902047864  1000  0.001 
Now we have a number that means something to us. We can take that number and multiply it by the charge strength at the particle boundary and get the charge strength at that volume. We will actually use the 1/r^3 equation to find the value for any radius. I did think about using a lookup table like this but the equation isn't that expensive so it isn't worth it. Precision is more important.
So my initial guess of the maximum charge emission range being 10 radii is pretty good. At that distance, the charge strength should be 1000 times less than at the particle boundary. Is it a coincidence that the Earth's chargepause, which sets the magnetopause and others, is also at 11 to 12 radii? I think not. In fact, I know not because it is the same reasons for both. If I had realised that when I created the constant in the code I would have used 11 or 12 instead.
So now we have an equation to calculate the charge at a given distance: C(d) = C(1)/d^3
Please note that I am using an equation within an equation. C is an equation to calculate the charge density or strength given a radius. So that equation explicitly states: The charge density at d is equal to the charge density at 1 divided by d^3. The charge density equation could be as simple as mass times volume, maybe mass times surface area or it could be more convoluted.
This is a quantum equation. It does not apply to macroscale numbers. We are ignoring time because the particles are close enough to do so, stars, planets, and moons are not, so it becomes a d^4 equation instead.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
I haven't thought this too far through yet, and I might be shooting my mouth off before I see it clearly enough, but I am hesitantly going to say that I don't think the macro equation should be an r^4 equation either. I think that I have the correct equation above.
It needs to be changed for use in the macro setting, though. We need to include the change in size of the emitter. Since the receiver is so far away, the charge that it receives was emitted at a time in the past. Using expansion theory, this means that the radius of the emitter was smaller when it emitted that charge. Well, my equation has a radius for the emitter right there. So let's use it for this purpose and see what happens.
C(d) = C(1)/d^3
That tells us the reduction in charge density based on volume only. The radius of the emitter is used in 2 places, although only one of them actually represents the emitter radius.
The d variable is used to represent the distance of the receiver from the emitter. It should be the distance of the point of measurement from the center of the emitter. This is likely to be the boundary of the receiver from the center of the emitter.
The other place it is used is as the number 1. In this case, it represents the radius of the emitter. Before, we only needed the number 1 as everything was relative and based on 1. Now, we want to change that value so we make it a variable. Let's call it r, for radius of the emitter.
C(d) = C(r)/d^3
Now we just need to know what r was when the charge was emitted. To find that, we need the distance it has traveled, which is d, since we know that it had a velocity of c, then we can determine how long it took that photon to travel to this point.
v = d/t > vt = d > t = d/v
v = c = 300, 000, 000m/s
t = d/c
Now we need to know how much a particle expands, per unit time, or unit time squared if it is an acceleration. Unfortunately, I don't know what that is. I don't even have a good guess. Maybe we can tease it out but I'll use a placeholder here instead. I'll create another equation for it and we can fill it in later.
Let R(n) be a function that calculates the radius of a sphere, given a value, n, that represents the time difference. When n=0, the current radius is returned. When n>0, a future radius is returned with n being the number of seconds into the future. When n<0, a past radius is returned with (the absolute value of) n being the number of seconds into the past.
Therefore, putting it back into our equation, we get:
C(d) = C( R(d/c) )/d^3
That is a general equation that can be used at the micro or macro scale, but more useful at the macro. Maybe you could call it a relativistic equation, since it takes Relativity into account. It does contain 2 other equations, or functions, that need to be provided in order to find the actual equation.
Not a bad days work, eh?
It needs to be changed for use in the macro setting, though. We need to include the change in size of the emitter. Since the receiver is so far away, the charge that it receives was emitted at a time in the past. Using expansion theory, this means that the radius of the emitter was smaller when it emitted that charge. Well, my equation has a radius for the emitter right there. So let's use it for this purpose and see what happens.
C(d) = C(1)/d^3
That tells us the reduction in charge density based on volume only. The radius of the emitter is used in 2 places, although only one of them actually represents the emitter radius.
The d variable is used to represent the distance of the receiver from the emitter. It should be the distance of the point of measurement from the center of the emitter. This is likely to be the boundary of the receiver from the center of the emitter.
The other place it is used is as the number 1. In this case, it represents the radius of the emitter. Before, we only needed the number 1 as everything was relative and based on 1. Now, we want to change that value so we make it a variable. Let's call it r, for radius of the emitter.
C(d) = C(r)/d^3
Now we just need to know what r was when the charge was emitted. To find that, we need the distance it has traveled, which is d, since we know that it had a velocity of c, then we can determine how long it took that photon to travel to this point.
v = d/t > vt = d > t = d/v
v = c = 300, 000, 000m/s
t = d/c
Now we need to know how much a particle expands, per unit time, or unit time squared if it is an acceleration. Unfortunately, I don't know what that is. I don't even have a good guess. Maybe we can tease it out but I'll use a placeholder here instead. I'll create another equation for it and we can fill it in later.
Let R(n) be a function that calculates the radius of a sphere, given a value, n, that represents the time difference. When n=0, the current radius is returned. When n>0, a future radius is returned with n being the number of seconds into the future. When n<0, a past radius is returned with (the absolute value of) n being the number of seconds into the past.
Therefore, putting it back into our equation, we get:
C(d) = C( R(d/c) )/d^3
That is a general equation that can be used at the micro or macro scale, but more useful at the macro. Maybe you could call it a relativistic equation, since it takes Relativity into account. It does contain 2 other equations, or functions, that need to be provided in order to find the actual equation.
Not a bad days work, eh?
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
I think that equation is a bit misleading. It seemed a good way to represent it as I wrote it, but now I see that the C(d) part is a bit confusing because the same function is used on the other side of that equation but it turns out that they are not really the same function.
What I should say is that the left hand side, C(d), is not actually a function call, but on the right hand side, C(1) or C( R(d/c) ), it is a function call. That is because the right hand side is the implementation of the left hand side. Which means that they are not really the same function.
So let's clear that up.
Let:
R(t) be a function that must return the radius of a particle given a time differential, t, where t is in unittime, for example, the number of seconds. When t=0, the current radius is returned. When t>0, a future radius is returned. When t<0, a past radius is returned.
C(r) be a function that returns the charge density at the boundary of a particle with radius r.
D(d) be a function that returns the charge density of a particle, measured at a distance, d, from its center.
c be the speed of light.
Therefore, the equation becomes:
D(d) = C( R( d/c ) ) / d^3
I have also had some thoughts on the function C. If my memory serves me, then Miles has stated that the charge density of a body (he was talking about stars, planets and moons) is its mass times by its density. Quite literally a charge density or mass density. I am not so sure that I want the same equation because that assumes you want the total charge of the body. I don't really want that, although I could work with it.
You see, we are not only trying to find the charge density at a distance, we are also trying to find the charge density over a certain area which is defined by the receiver. So far, we have not taken the receiver into account at all but it is part of this interaction and so it must be represented.
To combat that, I thought the charge density function, C, could return the mass, of the emitter, divided by its surface area. This gives us a charge density per unit area. Now, this unit area is small on the emitter, but it could be extremely large at the receiver. How do we deal with that?
Well, we could not do what I have just mentioned (divide by the emitters surface area) and instead, we calculate the total charge output of the emitter, for a complete sphere, reduce it based on the distance to the receiver, and then divide it by the surface area of the sphere that is centered on the emitter, but with a radius equal to the distance of the measurement point (receiver). If the receiver is a volume, rather than a point, then we might multiply that result by the surface area of the receiver (or maybe half of it) to find the total charge density across the receiver.
I think this is very important stuff. I have not only found an equation that sits along side Einsteins' equations, which he had no way of knowing was needed, but I have also found a way to use Expansion Theory without actually expanding the radii of particles. In fact, I am really using it to contract the radii, but only when calculating a charge density, not during the normal run of the model.
If I can find a way to do the same thing with gravity, I will have the basis of an Expansion Model.
What I should say is that the left hand side, C(d), is not actually a function call, but on the right hand side, C(1) or C( R(d/c) ), it is a function call. That is because the right hand side is the implementation of the left hand side. Which means that they are not really the same function.
So let's clear that up.
Let:
R(t) be a function that must return the radius of a particle given a time differential, t, where t is in unittime, for example, the number of seconds. When t=0, the current radius is returned. When t>0, a future radius is returned. When t<0, a past radius is returned.
C(r) be a function that returns the charge density at the boundary of a particle with radius r.
D(d) be a function that returns the charge density of a particle, measured at a distance, d, from its center.
c be the speed of light.
Therefore, the equation becomes:
D(d) = C( R( d/c ) ) / d^3
I have also had some thoughts on the function C. If my memory serves me, then Miles has stated that the charge density of a body (he was talking about stars, planets and moons) is its mass times by its density. Quite literally a charge density or mass density. I am not so sure that I want the same equation because that assumes you want the total charge of the body. I don't really want that, although I could work with it.
You see, we are not only trying to find the charge density at a distance, we are also trying to find the charge density over a certain area which is defined by the receiver. So far, we have not taken the receiver into account at all but it is part of this interaction and so it must be represented.
To combat that, I thought the charge density function, C, could return the mass, of the emitter, divided by its surface area. This gives us a charge density per unit area. Now, this unit area is small on the emitter, but it could be extremely large at the receiver. How do we deal with that?
Well, we could not do what I have just mentioned (divide by the emitters surface area) and instead, we calculate the total charge output of the emitter, for a complete sphere, reduce it based on the distance to the receiver, and then divide it by the surface area of the sphere that is centered on the emitter, but with a radius equal to the distance of the measurement point (receiver). If the receiver is a volume, rather than a point, then we might multiply that result by the surface area of the receiver (or maybe half of it) to find the total charge density across the receiver.
I think this is very important stuff. I have not only found an equation that sits along side Einsteins' equations, which he had no way of knowing was needed, but I have also found a way to use Expansion Theory without actually expanding the radii of particles. In fact, I am really using it to contract the radii, but only when calculating a charge density, not during the normal run of the model.
If I can find a way to do the same thing with gravity, I will have the basis of an Expansion Model.
Nevyn Admin
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Re: Possible Charged Particle Field
I know I am getting pretty far off track, but this is so important that I just need to get it out. I need to run with it while it is fresh in my mind.
Nevyn Admin
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Re: Possible Charged Particle Field
Note the differences between the quantum equation and the relativistic one.
1) D(d) = C(1)/d^3
2) D(d) = C( R( d/c ) )/d^3
Equation 1 only has the value 1 inside of the C function call. This represents the current radius of the emitter.
Equation 2 has R( d/c ) inside of the C call, which represents the radius of the emitter at some time in the past.
If we look at the definition of the R function, we find that when its argument is equal to 0, it will return the current radius.
When d is extremely small, the ratio of d to c approaches 0. It will never actually equal 0, but it will get so close as to be irrelevant.
Therefore, the relativistic equation reduces to the quantum equation at small distances.
1) D(d) = C(1)/d^3
2) D(d) = C( R( d/c ) )/d^3
Equation 1 only has the value 1 inside of the C function call. This represents the current radius of the emitter.
Equation 2 has R( d/c ) inside of the C call, which represents the radius of the emitter at some time in the past.
If we look at the definition of the R function, we find that when its argument is equal to 0, it will return the current radius.
When d is extremely small, the ratio of d to c approaches 0. It will never actually equal 0, but it will get so close as to be irrelevant.
Therefore, the relativistic equation reduces to the quantum equation at small distances.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
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You've definitely hit something, you've got to run with it. Including gravity would win you a seat beside Miles. The only thing I see missing is spin, then you can combine it with your angular motion and spin level velocity formulas.
Being critical, I might point out that emission fields aren’t spherical. The charged particle’s emission field is planar, like a disc, not a sphere. Actually, I would insist that a particle’s emission field may be better described as dual discs  due to the separate +/30deg emissions. Or a neutron’s polar charge emissions have the least amount of energy since it receives no angular emission from the spinning particle, what’s the charge density range for polar emissions? My point is the particle’s emission field is more complicated than a spherical volume. I’ve insisted charge emission is a function of latitude. When we add the components necessary in order to arrive at a complete description of the particle’s emission field we may end up with a charge lookup table.
Good stuff Nevyn.
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Ok, I'll try to read them. The charge density felt at distance d, depends on the emitter’s radius and the change in the emitter’s size in the time it took for light to reach the distance being measured, relativistic charge emission. d/c approaches 0 for the quantum scale. Together, both equations combine the micro or macro scales based on an analysis of spherical volume. It reminds me of the fact that spherical surface area is used to describe the inverse relationship of gravity, how after doubling a radius, what was a unit area becomes an area four time as large. Not a bad days work at all. More like an epiphany, the particle scaling relationship you’ve been looking for.Quantum. D(d) = C(1)/d^3
Relativistic. D(d) = C( R( d/c ) )/d^3
You've definitely hit something, you've got to run with it. Including gravity would win you a seat beside Miles. The only thing I see missing is spin, then you can combine it with your angular motion and spin level velocity formulas.
Being critical, I might point out that emission fields aren’t spherical. The charged particle’s emission field is planar, like a disc, not a sphere. Actually, I would insist that a particle’s emission field may be better described as dual discs  due to the separate +/30deg emissions. Or a neutron’s polar charge emissions have the least amount of energy since it receives no angular emission from the spinning particle, what’s the charge density range for polar emissions? My point is the particle’s emission field is more complicated than a spherical volume. I’ve insisted charge emission is a function of latitude. When we add the components necessary in order to arrive at a complete description of the particle’s emission field we may end up with a charge lookup table.
Good stuff Nevyn.
.
LongtimeAirman Admin
 Posts : 1080
Join date : 20140810
Re: Possible Charged Particle Field
LongtimeAirman wrote:
You've definitely hit something, you've got to run with it. Including gravity would win you a seat beside Miles.
I think including gravity will earn me a seat next to Einstein. Maybe even above Einstein! I'm not trying to make myself sound great or anything, there's still so much I don't know, but if I do that, then I have actually done what Einstein said that he did, but didn't quite get it correct, or at least complete.
But I'm still doubting myself at this point. I keep rereading it to make sure I haven't missed anything or buggered something up. I don't care about being compared to Einstein, just that we figure out Physics before it's too late. I am standing on the shoulders of both Miles and Einstein here, and give that credit where it is due. There is absolutely no way that I would have reached this position without Miles work behind me. None at all.
LongtimeAirman wrote:
The only thing I see missing is spin, then you can combine it with your angular motion and spin level velocity formulas.
Ah, but as we have already implemented in this app, spin comes from measuring the charge interactions from multiple places on the receiver and applying them in the correct fashion. We've already completed that step!
LongtimeAirman wrote:
Being critical, I might point out that emission fields aren’t spherical. The charged particle’s emission field is planar, like a disc, not a sphere. Actually, I would insist that a particle’s emission field may be better described as dual discs  due to the separate +/30deg emissions. Or a neutron’s polar charge emissions have the least amount of energy since it receives no angular emission from the spinning particle, what’s the charge density range for polar emissions? My point is the particle’s emission field is more complicated than a spherical volume. I’ve insisted charge emission is a function of latitude. When we add the components necessary in order to arrive at a complete description of the particle’s emission field we may end up with a charge lookup table.
Totally true and well done for seeing it so quickly. However, we have already fixed that problem in this app too! My charge density algorithm, already in use, takes care of the latitude differences. That algorithm would be inside of the C function used in those equations. It does need more work, though, especially around the polar regions. It would also be nice if I could reduce it to an equation rather than an algorithm. I'm not sure that is possible.
My main concern at this point is the R function. I'm just not sure how to go about implementing that. While I have some idea of what the C function looks like, figuring out the radius changes is a bit more difficult. I am hoping that I find that gravity is not really a 1/r^2 relationship. I am hoping that I find the same thing I did here, that one of those distances is actually a time separation and will not be required in the math, in that way. Miles has already said as much, but I don't think he has taken that concept down to the equations like I am trying to here.
To bring this back down to Earth, and demonstrate that I don't have an expanding ego, all I am doing here is analyzing geometry. I decided to go back to basics to determine how charge diminishes so that I could find the spot that I needed to change it, and have found a few things in the process. I am not doing anything that would be considered great, or of high intelligence. How many times has Miles said that science has gotten so far ahead of itself and just needs to get back to basics? And again we find it here. Physics doesn't need intelligence, it only needs mechanics. When you have the mechanics, the math just falls out of it. The mechanics controls the math. It provides the boundaries that the math must follow. It gives you the concepts that the math must implement.
So the next time you hear a Physicist say that the 'math is everything', you know they are lying. If the mechanics control the math, then the mechanics is more important than the math. That is because the mechanics represents reality and if your math is not tied to reality, then it is not Physics.
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
Something else I would like to point out is that it is Expansion Theory that has allowed me to find this stuff. By reducing gravity to a changing radius, a real motion of real entities, Miles has provided the basis for the mechanics that I needed. All I did was notice that I needed a smaller radius to represent the past (again provided by Miles), and that I had a radius in such a position. So I ran with it and am pretty happy with where I have ended up.
There is still a lot of work required, but what I have found, in only a few hours, is a great start. I not only have the general structure of the equation, I also have the placeholders for future work. And they are not just undefined placeholders either, they are clearly defined. While I don't know their exact implementations right now, I do know what they need to do.
When was the last time you saw that in mainstream Physics?
Aaaaaand, my ego is expanding again. Does anyone have a pin?
There is still a lot of work required, but what I have found, in only a few hours, is a great start. I not only have the general structure of the equation, I also have the placeholders for future work. And they are not just undefined placeholders either, they are clearly defined. While I don't know their exact implementations right now, I do know what they need to do.
When was the last time you saw that in mainstream Physics?
Aaaaaand, my ego is expanding again. Does anyone have a pin?
Nevyn Admin
 Posts : 1399
Join date : 20140911
Re: Possible Charged Particle Field
Jesus, Nevyn.
I'll be that pin, but only because you've been my pin in the past. Consider it returning the favor!
But this is some good shit right here. I'm not at all familiar with the ins and outs of the app or the script you're using, but ALL of the expansion equations here and your explanation makes sense to me. You're attacking it in a way that would have never occurred to me. It's definitely what you think, an extension of Miles and Einstein and all the other works but in a revolutionary way here. I think you need to keep going, and only wish I had the capacity to help aside from cheerleading. But it's something I might be able to plop into Maya as well, since it's so straightforward! Perhaps all of this scripting can be fairly easily converted to Python or Pymel, and save me all the headaches I've had with the Ndynamics "Nucleus" solver (ironic since it can't handle an actual nucleus!).
Allow yourself some patience though too! But as is your wont, run with it as far and fast as you can. You can always refine it later.
I'll be that pin, but only because you've been my pin in the past. Consider it returning the favor!
But this is some good shit right here. I'm not at all familiar with the ins and outs of the app or the script you're using, but ALL of the expansion equations here and your explanation makes sense to me. You're attacking it in a way that would have never occurred to me. It's definitely what you think, an extension of Miles and Einstein and all the other works but in a revolutionary way here. I think you need to keep going, and only wish I had the capacity to help aside from cheerleading. But it's something I might be able to plop into Maya as well, since it's so straightforward! Perhaps all of this scripting can be fairly easily converted to Python or Pymel, and save me all the headaches I've had with the Ndynamics "Nucleus" solver (ironic since it can't handle an actual nucleus!).
Allow yourself some patience though too! But as is your wont, run with it as far and fast as you can. You can always refine it later.
Jared Magneson Posts : 444
Join date : 20161011
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