Just hold your horses everyone.
With all this talk of dubious hidden dynamo models of planetary magnetic fields and convective fluid motion based ideas, there is a totally alterantive hypothesis for the origin of these magnetic fields (and even [though not really considered suffieciently yet] one that could explain the magnetic field of the sun and galaxies at large, based on similar ideas to that of Alfvens in them acting as large farday generators/unipolar inductors
*), all of which published in peer reviewed plasma cosmology journals (mostly, though by no means exclusively, the 2007 Special Issue on Cosmic Plasma). One day I wonder if anyones ever going to read all the peer reviewed materials in their journals, and Peratts book, And Alfvens, and other relenvent materials, so they actually know what they are talking about. The only two that I recall being discussed is Thronhills (largely crap and highly specualative [Though still interesting!]) paper on the Z-pinch morphology of electric stars, and Scotts still un-disproved, though admiteddly nitpicky, publication on the properties of magenetic fields and plasma in the cosmos.
Then maybe everyones heated arguments from ignorance can start to have some substance. No-ones claiming to have omnipotent knowledge. The material is all there in the IEEE journals for people to read, review and cite. Its just underappreciated and hard to acees for those that dont have the privelages.
http://ieeexplore.ieee.org/Xplore/l...l5/11181/36024/01707329.pdf&authDecision=-203
Van Allen has experimentally observed[1] that the magnetic moments of the planets and stars are proportional to their angular momentum over some 12 orders of magnitude. “This graph is purely empirical and is regarded with disdain by theorists of planetary magnetism.”—Van Allen. In this paper, I develop a model that both predicts the proportionality between magnetic moment and angular momentum and also fits the experimental results with no adjustable parameters. The model is based on the fact that each rotating planet and star is immersed in a nonrotating conducting plasma cloud, which constitutes a Faraday electrical generator. This Faraday generator is assumed to be the primary source of the magnetic field, in contrast to present models that assume that the flow of magma in the planets’ cores is responsible.
[1]
Image, Credit, IEEE Tranactions on Plasma Science, 2007
The following italisized test is Credit of:
"The Van Allen Hypothesis—The Origin of the Magnetic Fields of the, Planets and Stars", Alexeff, Igor, IEEE Transactions on Plasma Science, vol. 35, issue 4, pp. 748-750
http://adsabs.harvard.edu/abs/2007ITPS...35..748A
"We now develop a very simplified model of the mechanism of magnetic field generation, glossing over details in integration in order to present the basic details of the model. Consider Maxwell’s equations. The magnetic field is generated by a current
∇×B = μ0J. (1)
The magnetic field is operated on by a differential operator. The exact nature of the operator is not known at present, but the basic spatial distance in the differentiation process is obviously the celestial body’s radius R. Hence
B/R = μ0J. (2)
Next, the current must be generated by the rotation of the planet
J = σVB = σωRB. (3)
Equating the two expressions produces a result that is ambiguous in B
B/R = μ0σωRB (4)
However I note that the current flow from the equator of the celestial body is across the magnetic field in plasma, and Bohm conduction is appropriate. Bohm conduction will be discussed in more detail later [....]
J = σE = eneν = ene(E/B) = eneωR. (5)
The net result is as follows:
B = μ0eneωR2. (6)
Thus, the magnetic field of the planet is proportional to the permeability of space, the charge of the electron, the electron density of the surrounding medium, the angular velocity of rotation, and the square of the radius.
Now, the magnetic moment M is defined as the total flux multiplied by the distance between the magnetic poles. Using a simple cylindrical model, as shown in Fig. 2, We find,
[latex]M=\mu_0en_e{\omega}R^2(2{\pi}R^3)=2{{\pi}\mu_0}en_e{\omega}R^5[/latex] (7)
Next, consider the angular momentum L of a massM at radius R from the axis
L = MVR = MωR2. (8)
For a rotating cylindrical body, as shown in Fig. 2, I must integrate over the volume and assume a mass density m
[latex]L={\pi}m{\omega}R^5.[/latex] (9)
Thus, the ratio of magnetic moment M to angular momentum L does not depend on R or ω
M/L = (2μ0ene)/m (10)
The remarkable result is that these simple calculations reproduce the correct proportionality ratio between magnetic moment L and angular momentum M over 12 orders of magnitude.
The magnitude of the ratio M/L is evaluated as follows. The only variables are the electron density and the mass density. For the electron density, I choose the limiting density in interstellar space [4], 1 electron/cm3. This should produce a value of M/L at or below the experimental value. For the mass density, I choose the mass density of water, approximately 1 g/cm3. This should approximate the mass density of most celestial bodies. The net result is that not only are the magnetic moment M and the angular momentum L proportional to each other, but the agreement is reasonably correct with respect to the magnitude of the experimental data obtained by Van Allen. The previous equation yields a ratio of M/L of 5 exp−22 (about exp−21), while the value found by Van Allen from his graph is between exp−15 to exp−16. This appears to be a large discrepancy, but note that my calculation is in MKS units, while Van Allen’s are in CGS. (As a check, compute the angular momentum of the Earth.) Converting Van Allen’s results to MKS introduces a correction of exp−3, so his values become exp−18 to exp−19.
The final discrepancy is on the order of two to three orders of magnitude, but this is small compared to the agreement in slope over 12 orders of magnitude (Fig. 1). Also, the use of the limiting value of electron density in interstellar space yields the lowest possible limit for the value of M/L. In addition, the use of the density of hydrogen as a major component of some celestial bodies rather than that of water would also increase the agreement between the two values. Some values of the ratio of M/L are anomalously low. These include the values for Venus and the Moon. Discussions with one of my past students [5] reveal that the previously discussed ratio is the maximum possible value. The derivation is lacking the temporal behavior of M/L. The value can stay constant, decrease to zero, and even reverse. Note that no values of M/L are anomalously high, which further supports the model.
A. Detailed Discussion of “Bohm Conductivity”
This theory refers to “Bohm conduction.” Bohm conduction refers to electrical conduction [......]"
Again, Credit:
"The Van Allen Hypothesis—The Origin of the Magnetic Fields of the, Planets and Stars", Alexeff, Igor, IEEE Transactions on Plasma Science, vol. 35, issue 4, pp. 748-750
http://adsabs.harvard.edu/abs/2007ITPS...35..748A
Just thought I'd throw a but more data into the deabte, data that plasma cosmogology journals seem to be confronting, and traditional journals ignoring. So... just a brief spanner into the works
Not to discredit the work of any others that have contributed above, but this is certainly an extra alternative plasma characteristic based model worthy of consdieration.
...carry on.
* http://www.plasma-universe.com/index.php/Faraday_disk
A Unipolar inductor usually refers to a device in which a rotating metal disk rotating in a magnetic field, generates an electric current. The metal disk can be any conductor, including a rotating plasma. It is also known as a homopolar generator, unipolar generator, acyclic generator, disk dynamo, or Faraday disk.
Astrophysical unipolar inductors
Unipolar inductors occur in astrophysics where a conductor rotates through a magnetic field, for example, the movement of the highly conductive plasma in a cosmic body's ionosphere through its magnetic field. In their book, Cosmical Electrodynamics, Hannes Alfvén and Carl-Gunne Fälthammar write:
"Since cosmical clouds of ionized gas are generally magnetized, their motion produces induced electric fields [..] For example the motion of the magnetized interplanetary plasma produces electric fields that are essential for the production of aurora and magnetic storms" [..]
".. the rotation of a conductor in a magnetic field produces an electric field in the system at rest. This phenomenon is well known from laboratory experiments and is usually called 'homopolar ' or 'unipolar' induction. [3]
Unipolar inductors have been associated with the aurorae on Uranus,[[4]] binary stars,[5] [6] black holes,[7] [8] pulsars (neutron stars),[2] galaxies,[9] the Jupiter Io system,[10] [11] the Moon,[12] [13] the Solar Wind,[14] sunspots,[15] [16] in the Venusian magnetic tail.[17], the Earth,[18], and comets.[19] [20]
1. ^ Hannes Alfvén, "Keynote Address (1987) Double Layers in Astrophysics, Proceedings of a Workshop held in Huntsville, Ala., 17-19 Mar. 1986. Edited by Alton C. Williams and Tauna W. Moorehead. NASA Conference Publication, #2469" (Record | Full text) FULL TEXT
2. ^ a b Ruderman, M. A. & Sutherland, P. G., "Theory of pulsars - Polar caps, sparks, and coherent microwave radiation" FULL TEXT (1975) Astrophysical Journal, vol. 196, Feb. 15, 1975, pt. 1, p. 51-72. PEER REVIEWED
3. ^ Hannes Alfvén and Carl-Gunne Fälthammar, Cosmical Electrodynamics (1963) 2nd Edition, Oxford University Press. See sec. 1.3.1. Induced electric field in uniformly moving matter. ACADEMIC BOOK
4. ^ Hill, T. W.; Dessler, A. J.; Rassbach, M. E., "Aurora on Uranus - A Faraday disc dynamo mechanism" (1983) Planetary and Space Science (ISSN 0032-0633), vol. 31, Oct. 1983, p. 1187-1198 PEER REVIEWED
5. ^ Hannes Alfvén, "Sur l'origine de la radiation cosmique" {[full}} (On the origin of cosmic radiation)" Comptes Rendus, 204, pp.1180-1181 (1937) PEER REVIEWED
6. ^ Hakala, Pasi et al, "Spin up in RX J0806+15: the shortest period binary" FULL TEXT (2003) Monthly Notice of the Royal Astronomical Society, Volume 343, Issue 1, pp. L10-L14
7. ^ Burns, M. L.; Lovelace, R. V. E., "Theory of electron-positron showers in double radio sources" FULL TEXT (1982) Astrophysical Journal, Part 1, vol. 262, Nov. 1, 1982, p. 87-99 PEER REVIEWED
8. ^ Shatskii, A. A., "Unipolar Induction of a Magnetized Accretion Disk around a Black Hole"FULL TEXT, (2003) Astronomy Letters, vol. 29, p. 153-157
9. ^ Per Carlqvist, "Cosmic electric currents and the generalized Bennett relation"FULL TEXT (1988) Astrophysics and Space Science (ISSN 0004-640X), vol. 144, no. 1-2, May 1988, p. 73-84. PEER REVIEWED
10. ^ Goldreich, P.; Lynden-Bell, D., "Io, a jovian unipolar inductor"FULL TEXT (1969) Astrophys. J., vol. 156, p. 59-78 (1969) PEER REVIEWED
11. ^ Strobel, Darrell F.; et al, "Hubble Space Telescope Space Telescope Imaging Spectrograph Search for an Atmosphere on Callisto: A Jovian Unipolar Inductor" (2002) The Astrophysical Journal, Volume 581, Issue 1, pp. L51-L54 PEER REVIEWED
12. ^ "Sonett, C. P.; Colburn, D. S., "Establishment of a Lunar Unipolar Generator and Associated Shock and Wake by the Solar Wind" (1967) Nature, vol. 216, 340-343 PEER REVIEWED
13. ^ Schwartz, K.; Sonett, C. P.; Colburn, D. S., "Unipolar Induction in the Moon and a Lunar Limb Shock Mechanism"FULL TEXT in The Moon, Vol. 1, p.7 PEER REVIEWED
14. ^ Srnka, L. J., "Sheath-limited unipolar induction in the solar wind"FULL TEXT (1975) Astrophysics and Space Science, vol. 36, Aug. 1975, p. 177-204 PEER REVIEWED
15. ^ Yang, Hai-Shou, "A force - free field theory of solar flares I. Unipolar sunspots" Chinese Astronomy and Astrophysics, Volume 5, Issue 1, p. 77-83 PEER REVIEWED
16. ^ Osherovich, V. A.; Garcia, H. A., "Electric current in a unipolar sunspot with an untwisted field" (1990) Geophysical Research Letters (ISSN 0094-8276), vol. 17, Nov. 1990, p. 2273-2276 PEER REVIEWED
17. ^ Eroshenko, E. G., "Unipolar induction effects in the Venusian magnetic tail" (1979) Kosmicheskie Issledovaniia, vol. 17, Jan.-Feb. 1979, p. 93-10
18. ^ F J Lowes "The Earth as a unipolar generator" (1978) J. Phys. D: Appl. Phys. 11 765-768 PEER REVIEWED
19. ^ Minami, S.; White, R. S. "An acceleration mechanism for cometary plasma tails" (1986) Geophysical Research Letters (ISSN 0094-8276), vol. 13, Aug. 1986, p. 849-852. PEER REVIEWED
20. ^ Podgornyi, I. M.; Dubinin, E. M.; Israilevich, P. L.; Skolnikova, S. I. "Plasma dynamics in type-1 comet tails" (1984) Komety i Meteory (ISSN 0568-6199), no. 35, 1984, p. 30-34. In Russian PEER REVIEWED