tusenfem
Illuminator
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- May 27, 2008
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Perhaps you could help me? Aren't you a plasma physicist?
whatevah! look at post 1638, there is your answer.
Perhaps you could help me? Aren't you a plasma physicist?
OK, I'm sorry Tusenfem, It's no use gettn narkie at each other, does nuthn for the thread, so truce ay!
Perhaps you could help me? Aren't you a plasma physicist?
that won't achive anything, so I sorry I'm sure you get as frustrated as I do but lets keep it focused.Zeuzzz or "Sol", can you enlighten us? Where did you first hear about EU/PC, and why did you become so obsessed with it? Are you interested in learning "mainstream" physics too? Or is it just that you draw some enjoyment from feeling like an iconoclast?
Originally Posted by Sol88 View Post
What happens when you pass en electric current thru a plasma? At this stage forget about field lines. Be it lightning or a plasma globe filament.
Nuthing!?!?!
Some or all of the following may happen, depending on the situation:
- plasma heating (basically always happens because of the resistivity of the plasma)
- instabilities (depending on the flow velocity of the electrons or ions carrying the current, instabilities may or may not arise)
- double layers (although this partly fits into the instabilities category, depending on the local plasma density or on the flow velocity of the particle carrying the current, see instabilities, double layers may or may not be created)
- filamentation (depending on the strength of the current and on the properties of the plasma filamentation may or may not occur)
That is basically all that can happen in a plasma. Unless you mean an only partially ionized plasma, then you can get ionization too.
OK, so let's try it once again, a little bit slower this time.No I do not, your post wrt this subject is very limited!DeiRenDopa said:We need to be clear about this, so let's put it to bed before moving on, shall we?
Do you accept that my post was limited to illustrating a logical inconsistency?
If you don't accept that, then we need to work out why ... because that's what I intended.
Clear on what exactly?logical inconsistencies?
![]()
I hope the above clarifies what I am pointing out; if it doesn't, please say so and I'll try again to make it clear.That I gave a link to Arp's work after I said he was denied telescope time?
To be clear: I am trying to establish an agreed basis for having a discussion on this topic; I have not even begun to look at "EU/PC", whatever that might be.This is your beef against the merits of the EU/PC?![]()
For avoidance of doubt here are all three papers I could dig up in chronological order on H.Arp after he was denied Telescope time
[...]
Say whaaa? Tripper!
Do you know what's being discussed here?
Space is a PLASMA.
99% of Space is plasma.
Plasma contains + (positive) & - (Negative) charges.
Charge separation occurs in lab plasma’s
Plasma is an excellent conductor.
Plasma has known, though difficult mathematical properties.
Plasma is self organizing.
Plasma can be “cellular”.
Plasma can be “filamentary”.
Plasma we can observe in a lab/space
Plasma we can measure in a lab/space.
Dust can become a Plasma.
Magnetic fields require an electric current.
A flow of like charged particles constitutes an electric current.
We observe magnetic fields everywhere.
Charged particles are accelerated in an electric field.
Charged particles Follow magnetic field lines.
Lots of charges particle = PLASMA.
Plasma/Electricity/Magnetic effects comprise the electromagnetic spectrum.
N
where am I going wrong?
- Lots of charges particle = PLASMA.
- Plasma/Electricity/Magnetic effects comprise the electromagnetic spectrum.
Ok lets add field lines, perhaps I have some confusion in that department? Same deal except the current has to follow a field line.
Do you acknowledge that this is a logical inconsistency?
Quote:
That I gave a link to Arp's work after I said he was denied telescope time?
I hope the above clarifies what I am pointing out; if it doesn't, please say so and I'll try again to make it clear.
Sol88, we need to come to agreement on this, because it is the only mutually agreed basis we have, so far, for any discussion here.

Now suppose we find that "Sol88" presents these two statements:
A) Arp was (and continues to be) systematically denied publication of his results.
B) "The Discovery of a High-Redshift X-Ray-Emitting QSO Very Close to the Nucleus of NGC 7319" is a paper, by Arp, that was published in ApJ in 2005.
tusenfem
Originally Posted by Sol88 View Post
Ok lets add field lines, perhaps I have some confusion in that department? Same deal except the current has to follow a field line.
Add field lines (what kind of field lines? I assume magnetic).
The current follows a field line, which means that the electrons at least are magnetized.
The only thing that needs to be added than is that there will be effects of magnetic pressure in the possible instabilities
Ah, let's see, start at the end? Here you are wrong:
1. Just lots of charged particles is not a plasma
2. Effects are not an electromagnetic spectrum, a spectrum is a specific word used in physics
and then the greatest weirdness: Space is a PLASMA
Space is space and is not a plasma.

Could that be called a Birkeland current?
Say we have a "cloud" of charged particle a light year cubed? whats that called?
tusenfem said:There are three criteria that a plasma needs to obey, which will be stated here, but some of the defintions will first get clear in the following sections.
DeBye shielding
By looking at the Coulomb potential of a charge $q$, which is placed in a ``plasma'' and at the way the charge carriers behave because of this extra charges, it is found that the field of this extra charge gets shielded off by the original charge carriers. This happens over distance of the DeBye length $\lambda_{\rm D}$. In order for a plasma to be quasineutral, the physical dimension of the system, $L$, must be large compared to $\lambda_{\rm D}$:
\lambda_{\rm D} << L,
otherwise there is not enough space for the collective shielding effect to occur, and we have a simple ionized gas. This requirement is often called the first plasma criterion.
Plasma Parameter
This has to do with the density of the plasma and the DeBye length. Since the shielding effect is the result of the collective behaviour inside a DeBye sphere of radius $\lambda_{\rm D}$, it is necessary that this sphere contains enough particles. The number of particles inside a DeBye sphere is $(4/3)\pi n_{\rm e} \lambda_{\rm D}^3$. The term $n_{\rm e} \lambda_{\rm D}^3$ is often called the plasma parameter, $\Lambda$, and the second criterion for a plasma reads:
\Lambda = n_{\rm e} \lambda_{\rm D}^3 >> 1.
The mean potential energy of a particle due to its nearest neighbour, which is inversely proportional to the mean interparticle distance, and thus proportional to $n_{\rm e}^{1/3}$, must be much smaller than its mean energy,
$k_{\rm B} T_{\rm e}$.
\item Plasma Frequency \\
A typical oscillation of the plasma happens when both species (i.e.\ the positive and the negative) are moved wrt. eachother. The equations of motion for the distributions will show that the plasma starts oscillating {\it collectively} around the zero point at the so called plasma frequency:
\omega_{\rm p} = \sqrt{\frac{n_{\rm e} e^2}{m_{\rm e} \epsilon_0}}
Some plasmas, like the Earth's ionosphere, are not fully ionized. Here we have a substantial number of neutral particles and if the charged particles collide too often with neutrals, the electrons will be forced into equilibrium with the neutrals and the medium does not behave as a plasma anymore, but simply like a neutral gas. For the electrons to remain unaffected by collisions with neutrals, the average time between two electron-neutral collisions, tn, must be larger that the reciprocal of the plasma frequency:
\omega_{\rm p} \tau_{\rm n} >> 1
This is the third criterion for an ionized medium to behave as a plasma.
Sorry in effects I meant to say, when plasma/electricity and magnetic fields DO something we see the effects in the electromagnetic spectrum.
What would I see in the EM spectrum of a current following a magnetic field line thru a plasma?
How many charged particle per cubic cm would constitute a plasma?
I fail to see why the discharges in a plasma ball are equivalent to Birkeland currents.
These discharges are equivalent to lightning, they do not flow along the magnetic field, they just search the path of least resistance inside the ball and discharge.
It is a complete mystery to me that proponents of EU don't understand how a plasma ball works.
It's no mystery!
Though they may not be following a magnetic field line as per magnetosphere/steller/Cosmic/Galactic understanding, they do show a very distinct property of ELECTRICITY flowing in a plasma!
You're wrong.
A Birkeland current is a current that flows along magnetic field lines. The image you posted shows precisely the opposite (and at least the first image has nothing to do with plasma, by the way).
Now insert a field line going FROM somewhere TO somewhere and that is my understanding of a Birkeland current, on any scale!
.Yes that was it's purpose, as it does when any current flows. I do realize the Birkeland current also has one "down the guts" so to speak. That's the one the electron are spiraling around, no?The first image you posted shows magnetic field lines circling around a current. They are perpendicular to the current - the opposite of a Birkeland current - and the picture was probably intended to illustrate the B fields due to current flowing down a wire surrounded by vacuum
What happens when you pass en electric current thru a plasma? At this stage forget about field lines. Be it lightning or a plasma globe filament.
Nuthing!?!?!
Some or all of the following may happen, depending on the situation:
* plasma heating (basically always happens because of the resistivity of the plasma)
* instabilities (depending on the flow velocity of the electrons or ions carrying the current, instabilities may or may not arise)
* double layers (although this partly fits into the instabilities category, depending on the local plasma density or on the flow velocity of the particle carrying the current, see instabilities, double layers may or may not be created)
* filamentation (depending on the strength of the current and on the properties of the plasma filamentation may or may not occur)
That is basically all that can happen in a plasma. Unless you mean an only partially ionized plasma, then you can get ionization too.
tusenfem
Originally Posted by Sol88 View Post
Ok lets add field lines, perhaps I have some confusion in that department? Same deal except the current has to follow a field line.
Add field lines (what kind of field lines? I assume magnetic).
The current follows a field line, which means that the electrons at least are magnetized.
The only thing that needs to be added than is that there will be effects of magnetic pressure in the possible instabilities.
tusenfem
Originally Posted by Sol88 View Post
Could that be called a Birkeland current?
Not in my definition. I am for the strict definition that Birkeland currents are a specific kind of field aligned currents in the Earth's magnetosphere. For all the rest of field aligned currents I use the term "field aligned currents." Only grudgingly I added the extended definition into the Wiki page.
That would just be cloud of ionized gas. There are special conditions for an ionized gas to be called a plasma. From Plasma physics for dummies (a BAUT thread):
Originally Posted by tusenfem
There are three criteria that a plasma needs to obey, which will be stated here, but some of the defintions will first get clear in the following sections.
DeBye shielding
By looking at the Coulomb potential of a charge $q$, which is placed in a ``plasma'' and at the way the charge carriers behave because of this extra charges, it is found that the field of this extra charge gets shielded off by the original charge carriers. This happens over distance of the DeBye length $\lambda_{\rm D}$. In order for a plasma to be quasineutral, the physical dimension of the system, $L$, must be large compared to $\lambda_{\rm D}$:
\lambda_{\rm D} << L,
otherwise there is not enough space for the collective shielding effect to occur, and we have a simple ionized gas. This requirement is often called the first plasma criterion.
Plasma Parameter
This has to do with the density of the plasma and the DeBye length. Since the shielding effect is the result of the collective behaviour inside a DeBye sphere of radius $\lambda_{\rm D}$, it is necessary that this sphere contains enough particles. The number of particles inside a DeBye sphere is $(4/3)\pi n_{\rm e} \lambda_{\rm D}^3$. The term $n_{\rm e} \lambda_{\rm D}^3$ is often called the plasma parameter, $\Lambda$, and the second criterion for a plasma reads:
\Lambda = n_{\rm e} \lambda_{\rm D}^3 >> 1.
The mean potential energy of a particle due to its nearest neighbour, which is inversely proportional to the mean interparticle distance, and thus proportional to $n_{\rm e}^{1/3}$, must be much smaller than its mean energy,
$k_{\rm B} T_{\rm e}$.
\item Plasma Frequency \\
A typical oscillation of the plasma happens when both species (i.e.\ the positive and the negative) are moved wrt. eachother. The equations of motion for the distributions will show that the plasma starts oscillating {\it collectively} around the zero point at the so called plasma frequency:
\omega_{\rm p} = \sqrt{\frac{n_{\rm e} e^2}{m_{\rm e} \epsilon_0}}
Some plasmas, like the Earth's ionosphere, are not fully ionized. Here we have a substantial number of neutral particles and if the charged particles collide too often with neutrals, the electrons will be forced into equilibrium with the neutrals and the medium does not behave as a plasma anymore, but simply like a neutral gas. For the electrons to remain unaffected by collisions with neutrals, the average time between two electron-neutral collisions, tn, must be larger that the reciprocal of the plasma frequency:
\omega_{\rm p} \tau_{\rm n} >> 1
This is the third criterion for an ionized medium to behave as a plasma.
Then, and only then, can you claim to talk about a plasma.
Read above, it does not just depend on how many particles or how big, three requirements are set for something to be called a plasma.How many charged particle per cubic cm would constitute a plasma?
yeah, but that is like saying if I turn the switch I see light. it does not mean anything.Originally Posted by Sol88 View Post
Sorry in effects I meant to say, when plasma/electricity and magnetic fields DO something we see the effects in the electromagnetic spectrum.
NOTHING! a current flowing though a plasma does not necessarily need to show a signature.What would I see in the EM spectrum of a current following a magnetic field line thru a plasma?
The least the current will do is heat the plasma, so I guess you will at least see a change in the emission of the plasma, in whatever way the plasma is emitting its thermal signature.
Then again, it can become wild and all kinds of plasma waves may be excited.

Thanks for that.DRD
All right I may have made a cock up, As far as I knew it was telescope time.DRD said:Do you acknowledge that this is a logical inconsistency?
I hope the above clarifies what I am pointing out; if it doesn't, please say so and I'll try again to make it clear.Sol88 said:That I gave a link to Arp's work after I said he was denied telescope time?
Sol88, we need to come to agreement on this, because it is the only mutually agreed basis we have, so far, for any discussion here.![]()
I have made no statement - in my posts on this kind of logical inconsistency - on the publication rights, or telescope time, of anyone.But are you saying he was denied puplication rights as well?
Now suppose we find that "Sol88" presents these two statements:
A) Arp was (and continues to be) systematically denied publication of his results.
B) "The Discovery of a High-Redshift X-Ray-Emitting QSO Very Close to the Nucleus of NGC 7319" is a paper, by Arp, that was published in ApJ in 2005.
Originally Posted by Sol88 View Post
Space is a PLASMA.
99% of Space is plasma.
I love it when people contradict themselves in two consecutive statements..
Quote:
.Magnetic fields require an electric current
False. Where's the current in your refrigerator magnets? Where's the current for the B fields in the radio waves broadcast in 2005 that are currently arriving at Alpha Centauri?
What bloody fridge magnet? Ever seen one is the cosmos?Quote:
False. Charged particles experience zero magnetic force if they follow B field lines. If they don't, they feel a force transverse to their motion that causes them to travel along a curved path.Charged particles Follow magnetic field lines.
Quote:
False. All matter contains charged particles - and at much higher density than most plasmas.Lots of charges particle = PLASMA.
The logical inconsistency comes in a pair of posts written by a "Sol88"; shall I quote them for you, and provide links?
I'm confused. Are you meaning to imply that plasma does not exert a gravitational pull?Ok ok the 1% is solid matter, gas, or liquid the substance of which gravity IS a property.
In post#1511, you quoted this (extract): "Arp was (and continues to be) systematically denied publication of his results"Sure why not I've been to busy seeing if I'm a total nutter or not, so far so good though!!DeiRenDopa said:The logical inconsistency comes in a pair of posts written by a "Sol88"; shall I quote them for you, and provide links?
Sure thing ... in a later post ...Perhaps you'd care to me here and run over some of the points I've listed in post 1642 maybe you think they may have some bearing on this thread.
We need an agreed basis for a discussion, as I proposed earlier.Am I in trouble for my illogical consistencies or something Miss?
Tusenfem wrote: I fail to see why the discharges in a plasma ball are equivalent to Birkeland currents.
Then I added:
Though they may not be following a magnetic field line as per magnetosphere/steller/Cosmic/Galactic understanding, they do show a very distinct property of ELECTRICITY flowing in a plasma!
Added few pics starting with the basics see POST 1616
Sol invictus jumped in and said this: A Birkeland current is a current that flows along magnetic field lines.
Maybe you did not see this:Now insert a field line going FROM somewhere TO somewhere and that is my understanding of a Birkeland current, on any scale!
Though you did later admit .Yes that was it's purpose, as it does when any current flows. I do realize the Birkeland current also has one "down the guts" so to speak. That's the one the electron are spiraling around, no?
Now insert a field line going FROM somewhere TO somewhere and that is my understanding of a Birkeland current, on any scale!
Which was clarified by Tusenfem in later posts
I did forget to mention the plasma ball gets hot when you put your full palm on it, uncomfortably so actually! And I in no way suggested the plasma ball was powerful enough to form double layers, though I spose you crank up the power and scale the plasma ball and it would? Fair call?
Then we added some MAGNETIC field lines on Tusenfem wrote:The only thing that needs to be added than is that there will be effects of magnetic pressure in the possible instabilities.
So then begrudgingly we call them Birkeland currents' or to give no credit were credits due "field aligned current" FAC's
So where did that argument take us?