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Atomic theory through time

The Dalton model of the atom = hard sphere model

The Thompson model of the atom = plum-pudding model

The Bohr model of the atom = planetary model

The modern model of the atom = wave-mechanical model

 

Millikan’s oil drop experiment 

Millikan determined the mass and charge of electrons.

 

Louis de Broglie Postulate

Particles such as electrons must have both wave-like and particle-like properties.

 

The Heisenberg uncertainty principle

The position and the momentum (mass times velocity) of a particle cannot be accurately measured.

 

The Schrodinger Wave Mechanics Theory

An electron can only have certain states or orbital (a mathematical expression which represents the behavior of electrons in curved paths)

 

Electron Configuration

An electron has four quantum numbers corresponding to its location within an atom.

 

The Quantum Numbers are

The principal quantum number (n) or shell, or level

The azimuthal quantum number (l) or subshell, or sublevel 

The magnetic quantum number (ml) or orbital

The magnetic direction (ms) or spin

 

The principal quantum number (n) represents the distance from the nucleus, shell 1 is the closest. The potential energy of e- increases as the distance from the nucleus increases therefore electrons are most stable when close to the nucleus.

 

n

---7---

---6---

---5---

---4---

---3---

---2---

---1---

NUCLEUS

  

The azimuthal quantum number (l) or angular momentum quantum number represents the shape of an orbital.

There are 4 sublevels (s, p, d, and f)

 

n

l

---7---

 

---6---

 

---5---

 

 

---4---

 

---3---(f)

---2---(d)

---1---(p)

---0---(s)

 

---3---

 

---2---(d)

---1---(p)

---0---(s)

---2---

---1---(p)

---0---(s)

---1---

---0---(s)

NUCLEUS

 

The magnetic quantum numbers (ml) represents the orientation of a sublevel in space along the x, y, and z axis of a coordinate system.

 

---n--- 

---l---

 ---ml---

---4---

 

 

 

 

 

 

 ---3---

 

 

 

 

 ---2--- (d)

--- (+2) ---

--- (+1) ---

---  (0)  ---

--- (-1) ---

--- (-2) ---

---1--- (p)

--- (+1) ---

---  (0)  ---

--- (-1) ---

---0--- (s)

---  (0)  ---

 

  ---2---

 

---1--- (p)

--- (+1) ---

---  (0)  ---

--- (-1) ---

---0--- (s)

---  (0)  ---

 ---1---

---0--- (s)

---  (0)  ---

NUCLEUS

 

The magnetic direction (ms) represents the spin of electrons. Values can be -½ or +½.

 

---n--- 

---l---

 ---ml---

---ms-- -

---4---

 

 

 

 

 

 

 

 ---3---

 

 

 

 

---2--- (d)

--- +2 ---

+ or - ½

--- +1 ---

+ or - ½

---  0  ---

+ or - ½

--- -1 ---

+ or - ½

--- -2 ---

+ or - ½

 ---1--- (p)

--- +1 ---

+ or - ½

---  0  ---

+ or - ½

--- -1 ---

+ or - ½

---0--- (s)

---  0  ---

+ or - ½

 

  ---2---

 

 ---1--- (p)

--- +1 ---

+ or - ½

---  0  ---

+ or - ½

--- -1 ---

+ or - ½

---0--- (s)

---  0  ---

+ or - ½

 ---1---

---0--- (s)

---  0  ---

+ or - ½

NUCLEUS

 

 

Summary of Electron Configuration

 

Principle Quantum Numbers

Sublevels

Orbitals

Spin numbers

Total Number of sublevels

Total Number of Orbitals

Total Number of Electrons

n

l

ml

ms

n

n2

2n2

1

0 (s)

0

+ or - ½

per

electron

1

1

2

2

0 (s)

0

2

4

8

1 (p)

-1,0,+1

3

0 (s)

0

3

9

18

1 (p)

-1,0,+1

2 (d)

-2,-1,0,+1,+2

4

0 (s)

0

4

16

32

1 (p)

-1,0,+1

2 (d)

-2,-1,0,+1,+2

3 (f)

-3,-2,-1,0,+1,+2,+3

 

 

The Pauli Exclusion Principle

Only two electrons can occupy any one orbital, and they must have opposite spins. Therefore no two electrons can have the same values for all four quantum numbers.

 

The Hund’s rule

Electrons occupy the orbitals of a subshell singly and with parallel spins until each orbital has one electron, this way electrons are farther away from each other.

 

The Aufbau or energy order

Electrons fill the orbital that have the lowest energy first.

Example

 

1s

2s

2p

 

H

1

 

 

 

 

1s1

He

2

 

 

 

 

1s2

Li

2

1

 

 

 

1s2 2s1

Be

2

2

 

 

 

1s2 2s2

B

2

2

1

 

 

1s2 2s2 2p1

C

2

2

1

1

 

1s2 2s2 2p2

N

2

2

1

1

1

1s2 2s2 2p3

O

2

2

2

1

1

1s2 2s2 2p4

F

2

2

2

2

1

1s2 2s2 2p5

Ne

2

2

2

2

2

1s2 2s2 2p6

 

 

 

 

 

 

 

 

 

 

 

 

Since some energy levels have lower potential energy than others follow the table below to write electron configurations.

 

1s

 

 

 

2s

2p

 

 

3s

3p

3d

 

4s

4p

4d

4f

5s

5p

5d

5f

6s

6p

 6d

6f 

7s

7p 

7d 

 

 

 

 

 

 

 

 

 

Example

In the electron configuration of K, 4s is filled before the 3d.

1s2 2s2 2p6 3s2 3p6 4s1

 

Electron configurations can be abbreviated by replacing the inner electrons by the electron configuration of the corresponding noble gas.

Example:

 F is [He] 2s2 2p5

 K is [Ar] 4s1

 

Transition and Inner Transition Elements

In addition when a sublevel is half or fully filled it gives the atom more stability therefore next level or sublevel is filled once a half or full sublevel occurs.

Example:

Cr is [Ar] 3d5 4s1 and not [Ar] 3d4 4s2

Cu is [Ar] 3d10 4s1and not [Ar] 3d9 4s2

 


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