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Each electron in an atom is described by four different quantum numbers. ... Angular Momentum (Secondary, Azimunthal) Quantum Number (l): l = 0, ..., n-1.
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Quantum Numbers and Atomic Orbitals
By solving the Schrödinger equation (Hψ = Eψ ), we obtain a set of mathematical equations, called wave functions (ψ ), which describe the probability of finding electrons at certain energy levels within an atom.
A wave function for an electron in an atom is called an atomic orbital ; this atomic orbital describes a region of space in which there is a high probability of finding the electron. Energy changes within an atom are the result of an electron changing from a wave pattern with one energy to a wave pattern with a different energy (usually accompanied by the absorption or emission of a photon of light).
Each electron in an atom is described by four different quantum numbers. The first three ( n , l , ml ) specify the particular orbital of interest, and the fourth ( ms ) specifies how many electrons can occupy that orbital.
1. Principal Quantum Number ( n ): n = 1, 2, 3, …, 8. Specifies the energy of an electron and the size of the orbital (the distance from the nucleus of the peak in a radial probability distribution plot). All orbitals that have the same value of n are said to be in the same shell ( level ). For a hydrogen atom with n =1, the electron is in its ground state ; if the electron is in the n =2 orbital, it is in an excited state. The total number of orbitals for a given n value is n^2. 2. Angular Momentum (Secondary, Azimunthal) Quantum Number ( l ): l = 0, ..., n -1. Specifies the shape of an orbital with a particular principal quantum number. The secondary quantum number divides the shells into smaller groups of orbitals called subshells ( sublevels ). Usually, a letter code is used to identify l to avoid confusion with n : l 0 1 2 3 4 5... Letter s p d f g h... The subshell with n =2 and l =1 is the 2 p subshell; if n =3 and l =0, it is the 3 s subshell, and so on. The value of l also has a slight effect on the energy of the subshell; the energy of the subshell increases with l (s < p < d < f). 3. Magnetic Quantum Number ( ml ): ml = - l , ..., 0, ..., + l****. Specifies the orientation in space of an orbital of a given energy ( n ) and shape ( l ). This number divides the subshell into individual orbitals which hold the electrons; there are 2 l + orbitals in each subshell. Thus the s subshell has only one orbital, the p subshell has three orbitals, and so on.
4. Spin Quantum Number ( ms ): ms = +½ or -½. Specifies the orientation of the spin axis of an electron. An electron can spin in only one of two directions (sometimes called up and down ). The Pauli exclusion principle (Wolfgang Pauli, Nobel Prize 1945) states that no two electrons in the same atom can have identical values for all four of their quantum numbers. What this means is that no more than two electrons can occupy the same orbital, and that two electrons in the same orbital must have opposite spins. Because an electron spins, it creates a magnetic field, which can be oriented in one of two directions. For two electrons in the same orbital, the spins must be opposite to each other; the spins are said to be paired. These substances are not attracted to magnets and are said to be diamagnetic. Atoms with more electrons that spin in one direction than another contain unpaired electrons. These substances are weakly attracted to magnets and are said to be paramagnetic.
Table of Allowed Quantum Numbers Number of Orbital Number of n l ml orbitals Name electrons 1 0 0 1 1 s 2 2 0 0 1 2 s 2
1 -1, 0, +1 3 2 p 6
3 ____ ____________ ____ ____ ____
4 ____ ____________ ____ ____ ____
5 ____ ____________ ____ ____ ____
Properties of Monatomic Ions
The electrons in the outermost shell (the ones with the highest value of n ) are the most energetic, and are the ones which are exposed to other atoms. This shell is known as the valence shell. The inner, core electrons ( inner shell ) do not usually play a role in chemical bonding.
Elements with similar properties generally have similar outer shell configurations. For instance, we already know that the alkali metals (Group I) always form ions with a +1 charge; the “extra” s^1 electron is the one that’s lost: IA Li 1 s^22 s^1 Li+^1 s^2 IA Na 1 s^22 s^22 p^63 s^1 Na+^1 s^22 s^22 p^6 IA K 1 s^22 s^22 p^63 s^23 p^64 s^1 K+^1 s^22 s^22 p^63 s^23 p^6
The next shell down is now the outermost shell, which is now full — meaning there is very little tendency to gain or lose more electrons. The ion’s electron configuration is the same as the nearest noble gas — the ion is said to be isoelectronic with the nearest noble gas. Atoms “prefer” to have a filled outermost shell because this is more electronically stable.