We have gone through many theories but not the following
combined theory which is most read at present time:
Although I am writing purely about external influence, I
must make an unforgivable mistake if I don’t mention these issues:
-The gap between Earth’s rotation axis and magnetic pole: This
issue will be re-compromised in the conclusion of this book. However, one of
hypothesises about the origin of Earth Magnetism presumes that the ‘’yolk’’ of
the Earth, which induces the Earth Magnetism, used to be together with Earth’s
rotation axis but shocked by a huge meteorite then turns North side South. The
‘’turn’’ has not been perfect and leaves the North Magnetic pole far from
geometric North pole (about 110-170). By that author, the
collision with the huge meteorite made a very serious disaster to the living in
Dinosause Era, when all the Dinosause dead.
-The deviation and magnetic-longitude of ‘’0’’ deviation.(Magnetic
susceptibility of material).
The relevant documents may build a huge pile; we can’t read
every one of them but the following magazine- The GEOMAGNETISM-Magnetic Model
and Navigation. The paper is to affirm that ‘’the study of geomagnetism is one
of oldest geophysical sciences. Geomagnetic fields have been observed and been used
from ancient time.’’ That paper also emphasizes that the magnetic compass
needle does not point toward the North Magnetic Pole, but in the direction of
the magnetic field line-horizontal composition-at the place where the compass
is located.
On the scope of International cooperation in research, the
paper introduces World Magnetic Model (WMM), a joint product of the United
States National Geospatial Intelligence Agency and United Kingdom Defence
Geographic Centre. This model is used by many giant and important bodies such
as U.S Department of Defence, NOAA, U.K ministry of defence, NATO,
International Hydrographic Organization (IHO).
The paper is interesting and to be one of viable information
sources for the author of this book.
''The Earth core is supposed to be filled with molten
Magnesium since Earth’s violent birth. The flow or move of the molten in Earth
core is to produce Earth Magnetism.''?
Anyhow, those scientists must satisfy themselves as how the magnesium
can be mixed together with iron, even if the molten magnesium is found in
there.
PART I
Some viable concepts and
The Sea vs Land contributions
to Earth Magnetism
Chapter I
VIABLE RELEVANT CONCEPTS
Nowadays, the quantum theory is the first and the most that
catch the attention of the people in the world. Nonetheless, we should
recognize that the physics can’t be just bracketed in quantum, and so we got to
look backward some centuries when we can find W. Coulomb, A.Ampere and the two others
J.B.Biot and F.Savart.
I-Static Electric Charge and Coulomb:
This is the first we inspire when discuss about Earth
Magnetism, the subject is attached to a scientist who discovered electric
charge: W. Coulomb.
His rule is simply expressed in a formula for the force (F)
between the two charges:
F=ke*q1*q2/r2
Or
=ke*q1*q2*r-2
Where q1 and q2 are values of charges, each can be either (-)
negative or (+) positive. The distance between the two is ‘’r’’ and the Coulomb
constant ‘’ke’’ is depending on the media between the two.
ke=8.99*109 N.m2.C-2:
Coulomb constant for the normal environment or vacuum between the two charges. The
force is found to be negative (-) when either q1 or q2 is negative; to be
positive (+) when both of them are positive or negative; this is quite a law in
math and it demonstrates the wise of force ‘’+ push’’ or ‘’- pull’’.
Portrait of
Charles-Augustin de Coulomb
Charles-Augustin de Coulomb was an eminent French physicist.
He formulated the Coulomb’s law, which deals with electrostatic interaction
between electrically charged particles. The coulomb, SI unit of electric
charge, was named after him.
We are considering ‘’ke’’ for the media of large scale
and complicated, therefore we should give out some assumptions before any
problem.
Some more about moon-earth relation and calculation are debated
in the ‘’Moon charge and E.M’’ of this book.
II-A. Ampere:
The second scientist we inspire is A. Ampere, he is a great
scientist but simply his rule should be taken as: total charge in Coulomb
transported through a point within a unit of time (second) is to make current
value one Ampere.
(Portrait of André-Marie
Ampère)
André-Marie Ampère (1775-1836) is a French Physicist and
Mathematician; He worked at the beginning of the 1800s in Paris, France. He
used his mathematical and statistical skills to observe and measure natural
occurrences that had been discovered by other European scientists. He went on
to produce complete proof of the relationship between electricity and
magnetism. He also developed a new way of classifying chemical elements. Amp (Ampere)
or his name is given to basic unit of electricity.
With the above concept of electric current, an instant of the
5 different charges moving through a point in 5 seconds can make an average
current in that interim as following:
2 Coulombs in 1st second;
3 Coulombs in 2nd second;
1 Coulomb in 3rd second;
2 Coulombs in 4th second;
4 Coulombs in 5th second, can make a current of:
I = (2+3+1+2+4)/5=12/5=2.4 A
Figure 1/I-Electric
current & magnetism around
As soon as an electric current is created, a magnetic field
is established around it.
III-Biot-Sawart laws:
In physics, the momentum as well as the ‘’particle spin’’ is
considered as the most interesting subject. Let’s leave the modern physics and
work with these two scientists.
Jean Baptiste Biot – a
French scientist (1774-1862)
Felix Savart-a French
physicist (1791 -1841)
Those two French physicians are known as inventers to the
law that named after the both, the Biot-Savart about electromagnetism.
1-Biot - Savart law: The kernel of the law is to say
that a charge motion is to make magnetic field. A point ‘’P’’, at a distance ‘’r’’
from a conducting wire where the charge moves in, is in a magnetic field which
can be calculated as following:
Where dB is additional magnetic field contribution induced
by the current ‘’I’’, which is created by the directional move of a charge
‘’q’’.
Figure 2/I-A charge
move and its magnetism contribution to point P.
And ‘’ds’’ is a small segment of wire, both ‘’ds’’ and ‘’ȓ’’
are respective vector units of wire length and distance from the wire to ‘’P’’;
and product of those is dB -an outward vector or the vector that comes toward
reader as following figure.
µ0 – permeability coefficient of environment, is
4π
* 10-7 in normal air or vacuum.
2-Biot-Savart problem of many moving charged points:
Our discussion is not the first but is the most interesting application
of Biot-Savart law, which will be applied to almost every issue in this book. Instead
of momentum and spinning, we work with charge and orbiting. The following is an
excerpt from a manual on web.mit.edu.com (Mit. University web).
Quote:
The magnetic field due to 30 charges moving in a circle at a
given observation point. The position of the observation point can be varied to
see how the magnetic field of individual charges adds up to give the total
field.
In the above figure (9.1.11), we show an interactive Shock
Wave display that is similar to that in figure 9.1.10, but now we can interact
with the display to move the position of observer about in space. To get a feel
for total magnetic field, we also show a ‘’iron filings’’ representation of the
magnetic field due to these charges. We can move the observation point about in
space to see how the total field at various points arises from the individual
contributions of the magnetic field of to each moving charge.
Note, however, that since a point charge does not constitute
a steady current, the above equation strictly speaking only holds in the
non-relativistic limit where v<<C, the speed of light, so that the effect
of ‘’retardation’’ can be ignored.
The result may be readily extended to a collection of N
point charges, each moving with a different velocity. Let the ith charge qi be located at
(x,y,z) and moving with velocity v, using the superposition principle, the
magnetic field at P can be obtained as:
Unquote.
IV-Major historic notes:
This book is not written about industrial magnetism but the
subject is vital to the contemporary life, therefore the following note must
benefit the readers in general. On the other hand, some reader can’t get
through this book without reference back these notes.
The above figure illustrates how a direct current induces the magnetism
during flows through a coil.
1-Magnetic field
intensity: This is defined as the ratio between the max magnetic flux
density of a circuit to the permeability of free space.
H=B0/µ0
The magnetic intensity depends on the geometry of the
circuit and the conduction current, not on the medium.
The total magnetic field in a magnetic material is due to
the conduction current in the external circuit and the microscopic current
developed in the material.
B=B0+ µ0*M
2-Field strength (H):
Definition: It is the force experienced by a unit north pole
at a point in a magnetic field
H=F/m
Where F is the force, m is pole strength.
-If the field lines are more, then H is high and vice versa.
-Thus, the closer to the pole, the higher strength of
field.
Nowadays, magnet is applied in almost every equipment or even
toy. The power of U-shaped magnet is known to everyone who is experienced with
machinery work.
3-Magnetization:
a-Magnetic domains in an
un-magnetised bar point to random directions.
b-A bar magnet is brought near
the un-magnetised bar.
c-The magnetic domains point in the same direction,
producing magnetism. N or S poles of adjacent domains cancel each other out.
d-The atomic magnets at both ends are free. This produces N
and S poles at the ends.
e-The atomic magnets at the ends tend to fan out due to
repulsion between the like poles.
The magnet and its force applied in industry are not magic;
they are available in every material and everything, their force is null
because every elementary magnet in there points to different directions or even
one eliminates the other. The external magnetic force helps a certain bar in
its adjacent area to re-direct every elementary direction and make a force of
their total.
4-Magnetic Equivalent
Circuit:
Magnetic Field
Intensity (H): the amount of field force (mmf) distributed over the length
of the electromagnet. Sometimes referred to as Magnetizing Force.
Magnetic Flux Density (B)-The amount of magnetic
field flux concentrated in a given area.
Where N-numbers of turns of coil; i-current in the coil;
H-magnetic field intensity; l-mean length of the core.
Relation between B and H:
The magnetic field intensity, H produces a magnetic flux
density, B everywhere it exists.
B=µH (weber/m2) or Tesla
B=(µr/µ0)H(w/m2) or T
µ: Permeability of the medium.
µ0: Permeability of free space=4π.10-7
wbA.t.m
µr=µ/µ0 relative permeability of
medium.
Magnetic Flux Φ
-Unit
for flux is ‘’weber’’
-The
definition of 1 weber is the amount of flux that can produce and induced
voltage of 1 volt on a one-turn coil if the flux reduced to zero with uniform
rate.
This
concept is also defined as following: It is a measure of magnetic field in a
certain medium. In simple term if the magnetic field has to pass through a
certain medium, it will always travel as ‘’flux’’ lines (flux lines are
imaginary, but continuous lines travelling from North pole to South pole of a
magnet. Its units are Weber.
Magnetic Flux Density B
-Unit
for magnetic flux density is Tesla.
-The
definition of 1 tesla is the flux density that can produce a force of 1 Newton
per meter acting a conductor carrying 1 ampere of current.
Magnetic Field Strength H
-Unit
for magnetic field strength is Ampere/meter.
-A
line of force that produce the flux.
Earth’s Magnetic intensity in history and now (an
excerpt):
The above note is cited as some information about the
Earth’s magnetism in history and now. Definitely Humphreys does not fabricate the
graph, and he draws it with facts that found in researching. The question is
‘’steady decay’’ now and then?
V-Major Features & compositions:
1-E.M polarity: at present, south magnetic pole is
nearly coinciding with earth north geographic pole, that’s why magnetic compass
north hand always points toward North.
Figure-3/I-Earth
Magnet with zero-deviation.
The above image is set with assumption that magnetic
deviation is ‘’nil’’, and South magnetic pole is on North geographic pole.
2-Earth Magnetic field in different coordinates:
The following is an excerpt from manual of Bremen University:
3-Earth Magnetic field compositions:
Earth Magnetism or E.M is contributed by several magnetic
inducers, we are going to discuss about someone and not the whole. Unlike
traditional way, our way is to start from inducers such as charge on continent,
sea surface charge and Moon charge. Therefore we got to denote each magnetic composition
with a number attached to a symbol ‘’Δ’’ such as Δ(1) or Δ(2), except B(e)
which is induced by inner rotor of the Earth as well as local man-made source.
B(e) is also denoted as Δ(7), the only one composition which has undefined
direction and left as non-directional quantity, while all the rest are
directional.
-Positive charge on land contribution: Δ(1),
note that positive as well as negative charge is everywhere, but we do not
consider every one as it is but with massive quantity as representative of each.
Therefore a continent is positively charged in general. Direction of Δ(1)
will be defined in its problem, the land charge contribution in chapter II of
part I-‘’sea surface charge versus land charges’’.
-Negative sea surface contribution: Δ(2), unlike continental
surface which is positive, the sea surface is homogenous as only one electrode
and always negative. The direction of this composition is defined in its
problem, chapter II of part I.
-Van Allen belt contribution: Δ(3), Van Allen belt and its
companion, the plasma sphere, are not just making a shield to protect the
Earth, they are charged and to contribute to E.M. The direction of their
contribution is defined in the problem in chapter I of part II.
-Negative moon’s hemisphere contribution: Δ(4),
the Moon primarily is assumed as neutral with 2 hemispheres of 2 opposite
charges. Each hemisphere is inducing magnetism to Earth different to the other.
The direction of this quantity is defined in its problem in part II.
-Positive Moon’s hemisphere contribution: Δ(5),
the shined hemisphere of Moon is positive as losing electrons under solar wind.
It induces magnetism to Earth and its direction is defined in its problem in
part II.
-Contribution of total charge of Moon: Δ(6),
the above mentioned problems are considering Moon as neutral of 2 opposite
charges, but in reality the total of those charges Q(a)+Q(b) rarely is neutral,
besides a certain value different to Zero; therefore its contribution is
considered and it has potential to be a huge surprise.
V-Two important characteristics of material:
These are not just 2 important characteristic of material,
they are 2 subjects that attracts a lot of researchers in history and now.
Although we can go along with the researchers but we can’t keep going ahead
without some brief about them.
1-Permeability:
The magnetic permeability of a material is the degree of magnetization that it
receives when it responds linearly to a magnetic field. The symbol denoted for
permeability is a Greek letter ‘’µ’’, which is measured in units of H/m (Henry
per meter) or N/A2 (Newton per Ampere squared). Empty space itself
has an electromagnetic permeability value, also known as the magnetic constant,
µ0=4π*10-7 N/A2
For the purpose of demonstrating a mathematical relationship
between µ and some magnetic field B that is influencing a medium of some king,
let’s assume that there is an auxiliary magnetic field H that represents the
way this B field influences the organization of magnetic dipoles in our medium.
According to the way we have set up situation, the relationship between the
fields B, H and our permeability µ is mathematically defined by the following
equation:
B=µH
In the above case, our permeability will be scalar as long as our
medium is isotropic. Isotropy refers to a certain organization of medium that
means it is uniform in all directions. A good example of the use of isotropy is
in the cosmological principle that is a part of the Big Bang Theory. It is
assumed, in the Big Bang model, that space is isotropic, meaning there are no
localized anomalies in space that would stop the universe from expanding in the
way we observe. Anisotropy is opposite of isotropy. We are able to use a scalar
for permeability if we are working with a second rank tensor for anisotropy
linear medium.
2-Susceptibility: Magnetic susceptibility is the degree of
magnetism of a material in response to an applied magnetic field. If the
magnetic susceptibility is positive, the material can be paramagnetic,
ferromagnetic or antiferromagnetic. In these cases the magnetic field is
strengthened by the presence of the material. Alternatively, if the magnetic
susceptibility is negative, the material is diamagnetic and as a result, the
magnetic field is weakened by the presence of the material.
If the ratio between the induced magnetization and the
inducing field is expressed in unit volume, volume susceptibility (k) is
defined as
K=M/H
Where M is the volume magnetization induced in a material of
susceptibility k by the applied external field H. Volume susceptibility is a
dimensionless quantity. The value depends on the measurement system used:
K(SI)=4π*k(cgs)=4π*G*Oe-1,
Where G and Oe are abrreviations for Gause and Orstedt
respectively. The SI system should be used.
Mass, or specific, susceptibility is defined as
X=k/r
Where r is the density of material. The dimensions of mass
susceptibility are therefore cubic meters per kilogram.