A CLASSICAL LOOK AT THE MAGNETIC

 

PROPERTIES OF MATTER

 

 

 

Clarence L. Dulaney

2226 Fairgreen Drive

Missouri City, TX 77489

e-mail  cldtx1@sbcglobal.net

 

 

Abstract:  The magnetic properties of matter are due to the spins of its electrons.  There are three conditions, diamagnetic, paramagnetic and ferromagnetic.  This paper explains how these conditions can arise. 

 

 

TYPES OF MAGNETISM  

 

 

When any material (solid, liquid or gas) is placed in the poles of a powerful magnet, a force, usually quite small, is noted [1].  If the material is repelled by the magnet, it is said to be diamagnetic [2].

 

If it is attracted to the strongest part of the magnet, it is paramagnetic.  If the material is, or becomes a permanent magnet, it is said to be ferromagnetic.   

 

 

ELECTRON SPIN

 

 

All magnetism is caused by electron spin, which may be + or - (clockwise or counterclockwise).  See my paper on “Why Spin” [3] for a speculation on the magnitude of spin.  To comply with the principle of “Least Energy”, electrons usually pair off by spins, and the majority of substances have a net zero electron spin.  Such substances are diamagnetic, and the reaction to a strong magnet is virtually nil.

 

 

Some compounds such as NO and NO2 have odd numbers of electrons and hence are paramagnetic.  All “free radicals such as ·OH have a single, odd electron spin. All odd atomic numbered atoms such as 19K40  are also paramagnetic.  Oxygen and Sulfur both have 2 unpaired electron spins, although they have an even number of electrons.

 

 

All odd and even some even atomic numbered “Transition” Elements and “Rare Earth” elements have unpaired electron spins, and are paramagnetic.  The unpaired spins are “protected” by their positions in the Periodic Table [4].  The unpaired electrons have minimum energy configuration.  Gd, for example, a “rare earth”,  has 7 unpaired spins.  Most of the “rare earths” are strongly paramagnetic, and Gd is ferromagnetic below 20°C.

 

 

FERROMAGNETIC MATERIALS  

 

 

The other ferromagnetic materials are the “Transition” elements Fe, Co, and Ni (Iron, Cobalt and Nickel).  See reference [4] to visualize their “protected” position.  Note particularly that of Gd.  Some compounds and alloys of these elements are also ferromagnetic, for example, magnetite, Fe3O4.  This compound has 5+ unpaired electrons.

 

There are a number of alloys of these elements that are very strong permanent magnets.  Most of the alloys were developed by empirical methods.  Most contain iron.

 

 

FERROMAGNETISM OF IRON DOMAINS

 

 

 

.Very pure iron is only paramagnetic.  It is used in electromagnets, losing its magnetism when the current is turned off.  Steel contains 0.5% or more Carbon, and can be permanently magnetized, the more strongly the more C is present (up to a point).  Steel has been found to contain “domains” consisting of roughly 1015 atoms.  Assuming a spherical particle, it would have a diameter of about 2 x 10-3 cm.  These “domains” are randomly distributed in direction of their magnetic axes until the steel is put into a strong magnet.  Then, they align with the magnet.  The process of alignment can be observed with a microscope [2].  When they are all aligned, the magnetism is maximum.  They will basically stay aligned until the temperature of the magnet is raised to 770° C, at which point the domain order is broken, and the steel again becomes paramagnetic.  The whole process can be repeated when the steel is cooled.  The temperature of the transition is called the “Curie Temperature”.  (It is also the transition temperature from the a to the b crystalline form of iron).

 

Adding more Carbon to the steel increases both the ferromagnetism and the mechanical strength of the steel.  The point is eventually reached when the domains can no longer be turned by exposure to a strong magnet.

 

It is here proposed that the domains consist of some compound of Fe and C, possibly Fe4C3.  This compound would have 5+ unpaired electrons on the Fe[5.6].

 

Cobalt and Nickel have not been investigated to the same extent that Iron has, but they are reduced from their ores by Carbon, as is the case with Iron.  They probably contain compounds such as Co4C3 and Ni2C [6]. 

 

In the case of Gd below 20°C, the atoms with their 7 unpaired electron spins line up with the magnetic field.  Above the Curie Point, the atoms have enough energy that the magnetic order is destroyed.  It is here proposed that a phase modification must take place at 20°C,since the Curie Point is a definite transition,  Some sort of physical transition must take place as in the case of Iron.

 

 

SUMMARY

 

 

Paramagnetism is caused by unpaired electron spins on atoms or compounds.  Ferromagnetism occurs only in the case of Fe, Co, Ni and Gd and their compounds or alloys.  In the case of Fe, there are “domains” which probably consist of Fe4C3 that has 5+ unpaired electron spins. These domains may be aligned by exposure to a strong magnet.  This causes the steel to become a permanent magnet.

 

 

 

 

 

REFERENCES

 

 

1.     W. Hume-Rothery, “Atomic Theory for Students of Metallurgy”, The institute of Metals, London, 1947, p273ff.

2.     D. Vitogran, “Elements of Electric and Magnetic Circuits”, Rinehart, San Francisco, 1971, p194ff

3.     C. Dulaney, “Why Spin?’

4.     C. Dulaney, "nuclear Structure-Radioactivity"

5.     R. Weast, Ed., “Handbook of Chemistry and Physics, 63rd Edition. CRC press, Cleveland, 1982, pB1, F97

6.     F. Cotton and G Wilkinson, “Advanced Inorganic Chemistry”. John Wiley, 1980, p628

 

NOTE: All my papers may be found on my website,

http://nywebpage.netscape.com/clarencedulaney 

 

© Clarence Dulaney 10/5/2006