Bohr's circles work for hydrogen, and they fail for every other atom. The better picture is a cloud of probability. In this course we meet the waves of matter, the uncertainty principle, the four quantum numbers and the shapes of orbitals. Then we use three rules to write the electron configuration of any atom, and we explain the odd cases, such as chromium and copper.
4 lessons, about 1 h 45 min4 simulations12 problems8 practice questionsPython in every lesson
Every moving particle has a wavelength, . We see it only for very small particles such as electrons. Heisenberg showed that the position and the momentum of such a particle cannot both be known exactly: is at least . So an electron has no fixed path, only a probability of being found.
In the quantum model, the electron is described by a wave function, and its square gives the probability. An orbital is such a wave function, where the electron is found with high probability. Each orbital has three quantum numbers: , and . The electron has a fourth, the spin .
An s orbital is a sphere, a p orbital has two lobes along an axis (three orientations), and a d orbital usually has four lobes (five orientations). In hydrogen the energy depends on n only. In an atom with more electrons it also depends on l: ns is below np, below nd, below nf, and the orbitals fill in the order of increasing n + l.
Electrons fill the orbitals by three rules. The Aufbau principle fills the lowest energy first. Pauli's exclusion principle allows at most two electrons in an orbital, with opposite spins. Hund's rule puts one electron in each orbital of a subshell before any pair. Chromium and copper are exceptions, because half-filled and full d subshells are extra stable.
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