![]() ![]() (when z =1 and n = 1, this Rb becomes "Bohr radius.") (This means that we can use the equations of the hydrogen-like atom in 2S electron approximately.)Īccording to the Bohr hydrogen-like model, the radius (Rb) of the n × de Broglie's wavelength orbit is, So approximately, we can suppose the 2S electron is moving around the 4e+ nucleus ( +6e - 2e = +4e ) on the circular orbit of the two de Broglie's wavelength. The two electrons of 1S state are attracted to the 6e+ nucleus strongly, so they are much closer to the nucleus than the 2S electron. Here we try the three-electron Carbon ion (C3+).Ĭarbon ion (C3+) has two electrons in 1S orbital, and one electron in 2S orbital. Visualization of four valence electrons in Carbon atom (C).Surprisingly, this new atomic structure of the Bohr's helium can be applied to other two-electron atoms (ions ), Lithium ion (Li+), Beryllium (Be2+), Boron (B3+) and Carbon (C4+) ions, too.įurthermore, the ionization (ground state) energy of the three-electron atom lithium (Li) can be calculated correctly using the approximate "2S" Bohr orbit. This model can explain the phenomena of Pauli exclusion principle correctly, because there is no space for the third electron to enter this new two-electron Bohr atom. In this new successful Bohr model, the two electrons of the helium atom (He) are moving on the orbits of just one de Broglie's wavelength which are perpendicular to each other. Our new Bohr model has succeeded in calculating the Helium ionization energy more correctly than the quantum mechanical variational methods as shown in the Top page. Top page (correct Bohr model including the two-electron atoms). Bohr's Carbon (ion) New Bohr model Carbon (C) ![]()
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