Re: [Vo]:ref QED

2009-03-27 Thread mixent
In reply to  Horace Heffner's message of Fri, 27 Mar 2009 10:50:56 -0800:
Hi,
[snip]
>> In my model, the spin angular momentum of the electron is not a  
>> "magical
>> quantum" property at all, and can in fact be less than h_stripe /  
>> 2. Each
>> successive sub_ground state orbital has less angular momentum, and the
>> difference between that and the angular momentum of higher orbitals  
>> (up to the
>> "ground state") is always less than h_stripe, making photon  
>> emission impossible,
>> and neatly explaining the stability of the ground state to normal  
>> radiation.
>
>You are of course assuming radiation can only come from spin flipping.

Since in standard QM the photon carries h_stripe of angular momentum, and a 1S
orbital (all S orbitals?) electron only *has* spin angular momentum, that's all
that is available.
IOW only a spin flip supplies the required amount.

In my model, there is essentially no "spin" property, just orbital angular
momentum, and the change in the value thereof below the  ground state is less
than that required by a photon.
One might however argue that the angular momentum can change from e.g. a small
positive value to a large negative value, thus allowing for an h_stripe
difference. In my model, the actual allowed values are smaller and smaller
fractions, hence the differences are never a full h_stripe. It is actually this
fact rather than absolute "quantity" which prevents radiation.

>
>
>>
>>> thus guaranteeing Larmor radiation.  In fact, some molecular orbitals
>>> exist in a figure 8 configuration, where the center of the 8 is the
>>> nucleus, thus guaranteeing constant nuclear traverses.  I think
>>> ordinary Newtonian point particle models just can't explain the lack
>>> of radiation.
>>
>> I think that if you calculate the angular momentum of an electron  
>> in/near the
>> nucleus, you may get a surprise. The "r" part of "mvr" is very small.
>
>Yes, but as r->0 we have energy->inf and the energy available to  
>Larmor radiation goes to infinity.  Stable orbital conditions no  
>longer apply.  If a spin zero electron enters a nucleus then all bets  
>are off regarding angular momentum and the Coulomb force interaction  
>of the components.  Once within the nucleus the "spin zero" means  
>nothing.  It is not a "direct hit" on any specific charged particle  
>because the nucleus has multiple charged particles, including quarks.  
>Any collision "off center" has an inherent angular momentum, and the  
>initial "spin zero" is irrelevant.  It is not possible to be "on  
>center" to multiple targets.

Try actually calculating the maximum off-center angular momentum.
This occurs when the distance from the nucleus, or any particle within it, is
perpendicular to the path followed by the electron, so you can set r = distance
from center of charge, which can also be used to calculate the potential energy,
and hence the maximum velocity that the electron can have.
I get the formula sqrt((Z*q^2*r*me)/(2*Pi*epsilon_0)).
Since r appears in the numerator, and all other values are constants, it shrinks
with r (rather than getting larger as one might intuitively expect from
increasing energy). A "more central" collision has even less angular momentum,
and a central collision has no angular momentum at all.

>
>> I suspect that Larmor radiation is only possible when the electron  
>> comes from
>> outside the atom.
>
>That then is an assumption outside the boundaries of my statement  
>which explicitly assumed "ordinary Newtonian point particle  
>models" (i.e. implying your model appears to assume this), and thus  
>proves my point.


Say what??? Whether or not an electron comes from outside an atom, has no
relevance to whether or not it is a point particle, and hence has nothing to do
with the boundaries of your argument. 

>
>Best regards,
>
>Horace Heffner
>http://www.mtaonline.net/~hheffner/
>
>
>
Regards,

Robin van Spaandonk

http://rvanspaa.freehostia.com/Project.html



Re: [Vo]:ref QED

2009-03-27 Thread Horace Heffner


On Mar 25, 2009, at 6:10 PM, mix...@bigpond.com wrote:

In reply to  Horace Heffner's message of Wed, 25 Mar 2009 11:46:46  
-0800:

Hi,
[snip]


On Mar 23, 2009, at 1:05 PM, mix...@bigpond.com wrote:


I think the electron doesn't spiral into the nucleus because it
doesn't have
enough angular momentum to create a photon, hence it can't radiate,
which means
it can't lose energy.



This argument must not be true.  There is a finite probability of
finding the electron near or within the nucleus.
If viewed as a point
particle and not a wave function, the acceleration can thus become
arbitrarily high, as can the kinetic energy and angular momentum,


In standard QM the angular momentum of any given orbital is a  
constant. For the
1S orbital there is no orbital angular momentum, only spin angular  
momentum.
In theory therefore, the electron could radiate by flipping it's  
spin back and

forth, and dropping into ...what? This apparently doesn't happen.

In my model, the spin angular momentum of the electron is not a  
"magical
quantum" property at all, and can in fact be less than h_stripe /  
2. Each

successive sub_ground state orbital has less angular momentum, and the
difference between that and the angular momentum of higher orbitals  
(up to the
"ground state") is always less than h_stripe, making photon  
emission impossible,
and neatly explaining the stability of the ground state to normal  
radiation.


You are of course assuming radiation can only come from spin flipping.





thus guaranteeing Larmor radiation.  In fact, some molecular orbitals
exist in a figure 8 configuration, where the center of the 8 is the
nucleus, thus guaranteeing constant nuclear traverses.  I think
ordinary Newtonian point particle models just can't explain the lack
of radiation.


I think that if you calculate the angular momentum of an electron  
in/near the

nucleus, you may get a surprise. The "r" part of "mvr" is very small.


Yes, but as r->0 we have energy->inf and the energy available to  
Larmor radiation goes to infinity.  Stable orbital conditions no  
longer apply.  If a spin zero electron enters a nucleus then all bets  
are off regarding angular momentum and the Coulomb force interaction  
of the components.  Once within the nucleus the "spin zero" means  
nothing.  It is not a "direct hit" on any specific charged particle  
because the nucleus has multiple charged particles, including quarks.  
Any collision "off center" has an inherent angular momentum, and the  
initial "spin zero" is irrelevant.  It is not possible to be "on  
center" to multiple targets.


I suspect that Larmor radiation is only possible when the electron  
comes from

outside the atom.


That then is an assumption outside the boundaries of my statement  
which explicitly assumed "ordinary Newtonian point particle  
models" (i.e. implying your model appears to assume this), and thus  
proves my point.


Best regards,

Horace Heffner
http://www.mtaonline.net/~hheffner/






Re: [Vo]:ref QED

2009-03-25 Thread thomas malloy

Jones Beene wrote:


-Original Message-
From: Horace Heffner 

 


In fact, some molecular orbitals exist in a figure 8 configuration, where
   


the center of the 8 is the nucleus, thus guaranteeing constant nuclear
traverses.  


[JB:] Understanding the figure 8 configuration is perhaps the most important
basic challenge in QM and it can also be said that most theorists are simply
not "up to the task".
 

I've seen a model of the atom which has the nucleus as a torroid and the 
electrons going through the center of it.



--- Get FREE High Speed Internet from USFamily.Net! -- 
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Re: RE: [Vo]:ref QED

2009-03-25 Thread Harry Veeder

- Original Message - From: Jones Beene  Date: Wednesday, March 25, 2009 4:50 pm Subject: RE: [Vo]:ref QED > -Original Message- > From: Horace Heffner > > > In fact, some molecular orbitals exist in a figure 8 > configuration, where > the center of the 8 is the nucleus, thus guaranteeing constant nuclear > traverses. > > [JB:] Understanding the figure 8 configuration is perhaps the most > importantbasic challenge in QM and it can also be said that most > theorists are simply > not "up to the task". 
speaking of figure eights... 
http://www.facebook.com/photo.php?pid=1277715&l=6e4f24e6e2&id=676517267
Harry
> However, I would add that "guaranteeing constant nuclear > traverses" is a bit > of a reach in this regard  > > The following observation may or may not help with that > understanding of 2p > orbitals- but - if you think about a capacitor as being able to > "pass" AC > current, and current consists of, well it consists at least partly of > electrons - then the nuclear-cap can be a decent analogy (i.e with the > nucleus as a kind of capacitor)... but of course there is the > argument that > it is "not the same electron"... > > However, in Dirac's universe - is not the electron the epitome of > "fungibility"? > > http://en.wikipedia.org/wiki/Fungibility > > When I wrote that word "fungibility" I was almost certain that it > would not > be in Wiki, but heck, it is getting pretty damn hard to come up with > anything 
 that is not in Wiki these daze... > > Jones > > BTW here is some interesting commentary on 2p orbitals that adds some > credence to the idea that indeed it is "not the same electron" > that crosses > the nucleus ... > > http://winter.group.shef.ac.uk/orbitron/AOs/2p/index.html > > > 



Re: [Vo]:ref QED

2009-03-25 Thread mixent
In reply to  Horace Heffner's message of Wed, 25 Mar 2009 11:46:46 -0800:
Hi,
[snip]
>
>On Mar 23, 2009, at 1:05 PM, mix...@bigpond.com wrote:
>>
>> I think the electron doesn't spiral into the nucleus because it  
>> doesn't have
>> enough angular momentum to create a photon, hence it can't radiate,  
>> which means
>> it can't lose energy.
>
>
>This argument must not be true.  There is a finite probability of  
>finding the electron near or within the nucleus. 
>If viewed as a point  
>particle and not a wave function, the acceleration can thus become  
>arbitrarily high, as can the kinetic energy and angular momentum,  

In standard QM the angular momentum of any given orbital is a constant. For the
1S orbital there is no orbital angular momentum, only spin angular momentum. 
In theory therefore, the electron could radiate by flipping it's spin back and
forth, and dropping into ...what? This apparently doesn't happen.

In my model, the spin angular momentum of the electron is not a "magical
quantum" property at all, and can in fact be less than h_stripe / 2. Each
successive sub_ground state orbital has less angular momentum, and the
difference between that and the angular momentum of higher orbitals (up to the
"ground state") is always less than h_stripe, making photon emission impossible,
and neatly explaining the stability of the ground state to normal radiation.

>thus guaranteeing Larmor radiation.  In fact, some molecular orbitals  
>exist in a figure 8 configuration, where the center of the 8 is the  
>nucleus, thus guaranteeing constant nuclear traverses.  I think  
>ordinary Newtonian point particle models just can't explain the lack  
>of radiation.

I think that if you calculate the angular momentum of an electron in/near the
nucleus, you may get a surprise. The "r" part of "mvr" is very small.

I suspect that Larmor radiation is only possible when the electron comes from
outside the atom. 

Regards,

Robin van Spaandonk

http://rvanspaa.freehostia.com/Project.html



Re: [Vo]:ref QED

2009-03-25 Thread Harry Veeder




Instead of asking why the electron doesn't spiral into the nucleus,
perhaps one should question the law(s) that lead one to expect it should
spiral into nucleus.

The mathematical strategy of quantizing energy saves the law(s) and
avoids the latter question.

Harry 



RE: [Vo]:ref QED

2009-03-25 Thread Jones Beene
-Original Message-
From: Horace Heffner 

> In fact, some molecular orbitals exist in a figure 8 configuration, where
the center of the 8 is the nucleus, thus guaranteeing constant nuclear
traverses.  

[JB:] Understanding the figure 8 configuration is perhaps the most important
basic challenge in QM and it can also be said that most theorists are simply
not "up to the task".

However, I would add that "guaranteeing constant nuclear traverses" is a bit
of a reach in this regard 

The following observation may or may not help with that understanding of 2p
orbitals- but - if you think about a capacitor as being able to "pass" AC
current, and current consists of, well it consists at least partly of
electrons - then the nuclear-cap can be a decent analogy (i.e with the
nucleus as a kind of capacitor)... but of course there is the argument that
it is "not the same electron"...

However, in Dirac's universe - is not the electron the epitome of
"fungibility"?

http://en.wikipedia.org/wiki/Fungibility

When I wrote that word "fungibility" I was almost certain that it would not
be in Wiki, but heck, it is getting pretty damn hard to come up with
anything that is not in Wiki these daze...

Jones

BTW here is some interesting commentary on 2p orbitals that adds some
credence to the idea that indeed it is "not the same electron" that crosses
the nucleus ...

http://winter.group.shef.ac.uk/orbitron/AOs/2p/index.html




Re: [Vo]:ref QED

2009-03-25 Thread Horace Heffner


On Mar 23, 2009, at 1:05 PM, mix...@bigpond.com wrote:


I think the electron doesn't spiral into the nucleus because it  
doesn't have
enough angular momentum to create a photon, hence it can't radiate,  
which means

it can't lose energy.



This argument must not be true.  There is a finite probability of  
finding the electron near or within the nucleus. If viewed as a point  
particle and not a wave function, the acceleration can thus become  
arbitrarily high, as can the kinetic energy and angular momentum,  
thus guaranteeing Larmor radiation.  In fact, some molecular orbitals  
exist in a figure 8 configuration, where the center of the 8 is the  
nucleus, thus guaranteeing constant nuclear traverses.  I think  
ordinary Newtonian point particle models just can't explain the lack  
of radiation.


Best regards,

Horace Heffner
http://www.mtaonline.net/~hheffner/






Re: [Vo]:ref QED

2009-03-23 Thread mixent
In reply to  fznidar...@aol.com's message of Mon, 23 Mar 2009 08:43:37 -0400:
Hi Frank,
[snip]
>
>The reason that the electron does not spiral into the nucleus has been a 
>fundamental mystery. It is currently accepted that the angular momentum cannot 
>be lees that h/2pie.? This has been accepted because the result agrees with 
>experimental spectra.? Puthoff came up with some ideas about the emission and 
>absorption of zero point energy.? I believe that I have solved this problem.? 
>The orbits of the atoms exist as point of electromagnetic and gravitomagnetic 
>accessibility.? The ground state orbit is a point where the transitional 
>frequency ( 1.094 megahertz-meters ) equals the natural frequency of the 
>electron.
[snip]
I think the electron doesn't spiral into the nucleus because it doesn't have
enough angular momentum to create a photon, hence it can't radiate, which means
it can't lose energy.

Regards,

Robin van Spaandonk

http://rvanspaa.freehostia.com/Project.html



[Vo]:ref QED

2009-03-23 Thread fznidarsic

The reason that the electron does not spiral into the nucleus has been a 
fundamental mystery. It is currently accepted that the angular momentum cannot 
be lees that h/2pie.? This has been accepted because the result agrees with 
experimental spectra.? Puthoff came up with some ideas about the emission and 
absorption of zero point energy.? I believe that I have solved this problem.? 
The orbits of the atoms exist as point of electromagnetic and gravitomagnetic 
accessibility.? The ground state orbit is a point where the transitional 
frequency ( 1.094 megahertz-meters ) equals the natural frequency of the 
electron.

?

?

?

I have a paper coming out on this in Infinite Energy in Sept of 09.? I hope the 
paper proves to be epic.

?

Frank Znidarsic