When an atom loses electrons we would expect it to lose its outermost electrons first. But which are outermost? Remember the "last added" electrons in the transition elements are in the d orbitals of the next outermost shell. The the d orbital electrons should not be the outermost electrons in an atom. Thus we will lose the s & p electrons first then the d electrons if any are present. If additional electrons are lost then we can go into the d shell. Examples: look at Periodic Chart and figure out configurations for Na ion, Ni 2+ ion and Fe 2+ ion,
| IA | IIA | IIIA | IVA | VA | VIA | VIIA | VIIIA | |||||||||||
| H | He | |||||||||||||||||
| 2 | Li | Be | B | C | N | O | F | Ne | ||||||||||
| 3 | Na | Mg | IIIB | IVB | VB | VI | VIIB | VIIIB | IB | IIB | Al | Si | P | S | Cl | Ar | ||
| 4 | K | Ca | Sc | Ti | V | Cr | Mn | Fe | Co | Ni | Cu | Zn | Ga | Ge | As | Se | Br | Kr |
| 5 | Rb | Sr | Y | Zr | Nb | Mo | Tc | Ru | Rh | Pd | Ag | Cd | In | Sn | Sb | Te | I | Xe |
| 6 | Cs | Ba | Lu | Hf | Ta | W | Re | Os | Ir | Pt | Au | Hg | Tl | Pb | Bi | Po | At | Rn |
| s1 | s2 | d1 | d2 | d3 | d4 | d5 | d6 | d7 | d8 | d9 | d10 | p1 | p2 | p3 | p4 | p5 | p6 | |
It turns out that symmetry is a strong driving force in nature and symmetry considerations are a powerful tool for predicting how nature operates. This is important in predicting electronic configurations because when two electronic energy levels are close to each other, as in the 3d orbitals (highest energy in the 3 shell) and the 4s orbitals (lowest energy in the 4 shell), symmetry considerations can result in an electron preferring to "fill" the 3d orbital set, making it symmetrical, instead of going to the already symmetrical 4s orbital. This can be done in two ways: we can put one electron in each of the five d orbitals giving a spherical half-filled d orbital set, or we can put 2 electrons in each orbital. Examples: look at Periodic Chart and figure out configurations for Cr, Cu, Cu +1 ion, Zn +2 ion and Fe +3 ion,
| IA | IIA | IIIA | IVA | VA | VIA | VIIA | VIIIA | |||||||||||
| H | He | |||||||||||||||||
| 2 | Li | Be | B | C | N | O | F | Ne | ||||||||||
| 3 | Na | Mg | IIIB | IVB | VB | VI | VIIB | VIIIB | IB | IIB | Al | Si | P | S | Cl | Ar | ||
| 4 | K | Ca | Sc | Ti | V | Cr | Mn | Fe | Co | Ni | Cu | Zn | Ga | Ge | As | Se | Br | Kr |
| 5 | Rb | Sr | Y | Zr | Nb | Mo | Tc | Ru | Rh | Pd | Ag | Cd | In | Sn | Sb | Te | I | Xe |
| 6 | Cs | Ba | Lu | Hf | Ta | W | Re | Os | Ir | Pt | Au | Hg | Tl | Pb | Bi | Po | At | Rn |
| s1 | s2 | d1 | d2 | d3 | d4 | d5 | d6 | d7 | d8 | d9 | d10 | p1 | p2 | p3 | p4 | p5 | p6 | |
Atoms and compounds are paramagnetic when they have unpaired electrons. Recall that electron spin can be thought of as electrons behaving as tiny magnets, and the arrows we use in orbital filling diagrams corresponding to the direction of the magnetic poles.
As a result, atoms such as oxygen and iron will be paramagnetic and be attracted to a magnetic field. For example, oxygen has two unpaired electrons as seen in the orbital filling diagram:
, so it is paramagnetic. Similarly, iron is paramagnetic due to its unpaired d electrons:
| Fe | |||||||
1s |
2s |
2p |
3s |
3p |
4s |
3d |
Whereas zinc, with the d shell filled, is not paramagentic since it has no unpaired electrons:
| Zn | |||||||
1s |
2s |
2p |
3s |
3p |
4s |
3d |
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© R A Paselk
Last modified 29 March 2013