The **electron configuration** of an atomic types (neutral or ionic) allows us to know the shape and also energy that its electrons. Numerous general rules room taken into factor to consider when assigning the "location" of the electron to its prospective energy state, but these assignments space arbitrary and it is constantly uncertain regarding which electron is being described. Learning the electron configuration of a types gives united state a far better understanding of its bonding ability, magnetism and other altoalsimce.orgical properties.

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## Introduction

The **electron configuration** is the standard notation provided to explain the digital structure of an atom. Under the orbital approximation, us let every electron occupy an orbital, which deserve to be addressed by a single wavefunction. In law so, we acquire three quantum number (n,*l*,ml), which room the very same as the ones obtained from solving the Schrodinger"s equation for Bohr"s hydrogen atom. Hence, countless of the rules that we use to describe the electron"s attend to in the hydrogen atom can additionally be offered in systems involving multiple electrons. As soon as assigning electrons to orbitals, we need to follow a set of 3 rules: the Aufbau Principle, the Pauli-Exclusion Principle, and also Hund"s Rule.

The wavefunction is the systems to the Schrödinger equation. By addressing the Schrödinger equation because that the hydrogen atom, we attain three quantum numbers, specific the principal quantum number (n), the orbital angular inert quantum number (*l*), and also the magnetic quantum number (ml). Over there is a fourth quantum number, referred to as the rotate magnetic quantum number (ms), which is not acquired from solving the Schrödinger equation. Together, these 4 quantum numbers deserve to be provided to explain the location of an electron in Bohr"s hydrogen atom. These numbers can be thought of together an electron"s "address" in the atom.

## Notation

To help describe the ideal notation because that electron configuration, it is finest to do so with example. For this example, we will usage the iodine atom. There are two means in which electron configuration can be written:

I: 1s22s22p63s23p64s23d104p65s24d105p5

or

I:

In both the these species of notations, the order of the energy levels should be composed by raised energy, mirroring the variety of electrons in each subshell as an exponent. In the short notation, you place brackets roughly the *preceding* noble gas facet followed by the valence covering electron configuration. The routine table reflects that kyrpton (Kr) is the ahead noble gas listed before iodine. The noble gas configuration encompases the power states lower than the valence shell electrons. Therefore, in this instance

### Principal Quantum Number (n)

The major quantum number *n* suggests the shell or energy level in i beg your pardon the electron is found. The value of *n* can be set between 1 to *n*, wherein *n* is the value of the outermost shell containing one electron. This quantum number deserve to only be positive, non-zero, and integer values. That is, *n*=1,2,3,4,..

For example, one Iodine atom has its outmost electron in the 5p orbital. Therefore, the principle quantum number for Iodine is 5.

### Orbital Angular momentum Quantum Number (*l*)

The orbital angular inert quantum number, *l*, shows the subshell the the electron. You can also tell the form of the atom orbital v this quantum number. An *s* subshell synchronizes to *l*=0, a *p* subshell = 1, a *d* subshell = 2, a *f* subshell = 3, and also so forth. This quantum number have the right to only it is in positive and also integer values, back it deserve to take ~ above a zero value. In general, because that every worth of n, there room n values of *l*. Furthermore, the worth of *l* arrays from 0 come n-1. Because that example, if n=3, *l*=0,1,2.

So in regards come the example used above, the *l *values of Iodine for n = 5 are* l* = 0, 1, 2, 3, 4.

### Magnetic Quantum Number (ml)

The magnetic quantum number, ml, represents the orbitals the a given subshell. For a provided *l*, ml can variety from *-l* come *+l*. A p subshell (*l*=1), because that instance, have the right to have three orbitals corresponding to ml = -1, 0, +1. In other words, it specifies the px, py and pzorbitals the the p subshell. (However, the ml numbers don"t necessarily correspond to a given orbital. The fact that there are three orbitals just is indicative the the 3 orbitals that a p subshell.) In general, for a given *l*, there room 2*l*+1 possible values for ml; and in a *n* major shell, there are *n*2 orbitals found in that energy level.

Continuing on native out instance from above, the ml values of Iodine are ml = -4, -3, -2, -1, 0 1, 2, 3, 4. This arbitrarily exchange mail to the 5s, 5px, 5py, 5pz, 4dx2-y2, 4dz2, 4dxy, 4dxz, and also 4dyz orbitals.

### Spin Magnetic Quantum Number (ms)

The spin magnetic quantum number have the right to only have actually a value of either +1/2 or -1/2. The worth of 1/2 is the spin quantum number, s, which defines the electron"s spin. As result of the spinning of the electron, that generates a magnetic field. In general, one electron with a ms=+1/2 is dubbed an alpha electron, and one v a ms=-1/2 is referred to as a beta electron. No 2 paired electrons deserve to have the very same spin value.

Out that these four quantum numbers, however, Bohr postulated that just the principal quantum number, n, determines the energy of the electron. Therefore, the 3s orbital (*l*=0) has actually the same power as the 3p (*l*=1) and 3d (*l*=2) orbitals, nevertheless of a difference in *l* values. This postulate, however, holds true just for Bohr"s hydrogen atom or various other hydrogen-like atoms.

When taking care of multi-electron systems, us must take into consideration the electron-electron interactions. Hence, the previously defined postulate breaks under in the the power of the electron is now figured out by both the primary quantum number, n, and the orbit angular inert quantum number, *l*. Although the Schrodinger equation for many-electron atoms is extremely daunting to fix mathematically, we deserve to still describe their electronic structures via electron configurations.

## General rule of Electron Configuration

There are a collection of basic rules that are used to figure out the electron configuration of an atomic species: Aufbau Principle, Hund"s Rule and the Pauli-Exclusion Principle. Prior to continuing, it"s essential to know that each orbital deserve to be populated by *two* electron of opposite turn (which will certainly be further debated later). The complying with table reflects the *possible* number of electrons that can occupy every orbital in a given subshell.

subshell | number of orbitals | total number of possible electron in each orbital |

s | 1 | 2 |

p | 3 (px, py, pz) | 6 |

d | 5 (dx2-y2, dz2, dxy, dxz, dyz) | 10 |

f | 7 (fz3, fxz2, fxyz, fx(x2-3y2), fyz2, fz(x2-y2), fy(3x2-y2) | 14 |

Using our example, iodine, again, we watch on the periodic table the its atom number is 53 (meaning it includes 53 electron in that neutral state). Its complete electron configuration is 1s22s22p63s23p64s23d104p65s24d105p5. If you counting up all of these electrons, friend will view that that adds as much as 53 electrons. Notice that every subshell have the right to only contain the max quantity of electrons as indicated in the table above.

### Aufbau Principle

The indigenous "Aufbau" is German because that "building up". The Aufbau Principle, also called the building-up principle, states that electron"s accounting orbitals in stimulate of raising energy. The stimulate of occupation is as follows:

**1s**

**Hund"s dominion states that as soon as electrons accounting degenerate orbitals (i.e. Very same n and l quantum numbers), they must an initial occupy the north orbitals before dual occupying them. Furthermore, the most stable construction results as soon as the spins are parallel (i.e. Every alpha electrons or all beta electrons). Nitrogen, because that example, has 3 electron occupying the 2p orbital. Follow to Hund"s Rule, castle must an initial occupy each of the three degenerate ns orbitals, specific the 2px orbital, 2py orbital, and the 2pz orbital, and also with parallel spins (Figure 2). The configuration listed below is incorrect since the 3rd electron occupies does no occupy the empty 2pz orbital. Instead, it occupies the half-filled 2px orbital. This, therefore, is a violation of Hund"s rule (Figure 2).**

**Figure 2. A visual representation of the Aufbau Principle and Hund"s Rule. Keep in mind that the filling of electrons in every orbital(px, py and also pz) is arbitrary as lengthy as the electrons space singly filled prior to having two electrons occupy the same orbital.(a)This diagram represents the**

*correct*filling the electrons for the nitrogen atom. (b) This diagramrepresents the*incorrect*filling the the electrons for the nitrogen atom.## Electronic configuration of Cations and also Anions

The means we designate digital configurations because that cations and anions is essentially similar to that for neutral atom in your ground state. That is, us follow the three crucial rules: Aufbau Principle, Pauli-exclusion Principle, and Hund"s Rule. The electronic configuration of cations is assigned by removing electrons first in the outermost p orbital, adhered to by the s orbital and finally the d orbitals (if any more electrons must be removed). Because that instance, the ground state electronic configuration of calcium (Z=20) is 1s22s22p63s23p64s2. The calcium ion (Ca2+), however, has actually two electron less. Hence, the electron configuration for Ca2+ is 1s22s22p63s23p6. Since we have to take away 2 electrons, we an initial remove electron from the outermost covering (n=4). In this case, every the 4p subshells room empty; hence, we start by removing indigenous the s orbital, i m sorry is the 4s orbital. The electron construction for Ca2+ is the very same as the for Argon, which has 18 electrons. Hence, we have the right to say that both space isoelectronic.

The electronic configuration the anions is assigned by adding electrons follow to Aufbau Principle. We add electrons to fill the outermost orbital that is occupied, and then add much more electrons come the next higher orbital. The neutral atom chlorine (Z=17), for instance has 17 electrons. Therefore, its ground state electronic configuration have the right to be written as 1s22s22p63s23p5. The chloride ion (Cl-), on the other hand, has secondary electron for a full of 18 electrons. Complying with Aufbau Principle, the electron occupies the partially filled 3p subshell first, make the 3p orbital fully filled. The digital configuration for Cl- can, therefore, be designated together 1s22s22p63s23p6. Again, the electron configuration for the chloride ion is the very same as the for Ca2+ and also Argon. Hence, they are all isoelectronic to each other.

## Problems

1. I m sorry of the princples explained over tells united state that electrons that are paired cannot have the same spin value?

2. Discover the worths of n, *l*, ml, and also ms because that the following:

a. Mg

b. Ga

c. Co

3. What is a possible mix for the quantum number of the 5d orbital? Give an instance of an aspect which has the 5d orbital together it"s most outer orbital.

4. I beg your pardon of the adhering to cannot exist (there may be much more than one answer):

a. N = 4; *l* = 4; ml = -2; ms = +1/2

b. N = 3;* l* = 2; ml = 1; multiple sclerosis = 1

c. N = 4; *l* = 3; ml = 0; multiple sclerosis = +1/2

d. N = 1; *l* = 0; ml = 0; ms = +1/2

e. N = 0; *l* = 0; ml = 0; ms = +1/2

5. Compose electron configurations because that the following:

a. P

b. S2-

c. Zn3+

## Answers

1. Pauli-exclusion Principle

2. A. N = 3; *l* = 0, 1, 2; ml = -2, -1, 0, 1, 2; ms have the right to be either +1/2 or -1/2

b. N = 4; *l* = 0, 1, 2, 3; ml = -3, -2, -1, 0, 1, 2, 3; ms can be either +1/2 or -1/2

c. N = 3; *l* = 0, 1, 2; ml = -2, -1, 0, 1, 2, 3; ms deserve to be one of two people +1/2 or -1/2

3. N = 5; *l* = 3; ml = 0; multiple sclerosis = +1/2. Osmium (Os) is one example.

4. A. The worth of *l* cannot be 4, because *l* varieties from (0 - n-1)

b. Ms can only it is in +1/2 or -1/2

c. Okay

d. Okay

e. The value of n can not be zero.

See more: Boku No Koto Suki Ni Natte

5. A. 1s22s22p63s23p3

b. 1s22s22p63s23p6

c. 1s22s22p63s23p64s23d7

## References

Atkins, P. W., & De Paula, J. (2006).*Physical altoalsimce.orgistry because that the Life Sciences.*brand-new York, NY: W. H. Freeman and Company. Petrucci, R. H., Harwood, W. S., & Herring, F. G. (2002).*General altoalsimce.orgistry: principles and modern Applications.*upper Saddle River, NJ: Prentice-Hall, Inc. Shagoury, Richard.*altoalsimce.orgistry 1A class Book.*4th Ed. Custom Publishing. 2006. Print