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WAVE MECHANICS

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WAVE MECHANICS

(Schrödinger, 1926)

The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty principle.

* The state of an electron is described by a function , called the “wave function”.

*  can be obtained by solving Schrödinger’s equation (a differential equation):

H  = E 

This equation can be solved exactly only for the H atom^

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WAVE MECHANICS

* This equation has multiple solutions (“orbitals”), each corresponding to a different energy level.

* Each orbital is characterized by three quantum numbers:

n : principal quantum number n=1,2,3,...

l : azimuthal quantum number l= 0,1,…n-1

ml: magnetic quantum number ml= -l,…,+l

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WAVE MECHANICS

* The energy depends only on the principal quantum number, as in the Bohr model:

En = -2.179 X 10-18J /n2

* The orbitals are named by giving the n value followed by a letter symbol for l:

l= 0,1, 2, 3, 4, 5, ...

s p d f g h ...

* All orbitals with the same n are called a “shell”.

All orbitals with the same n and l are called a “subshell”.

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HYDROGEN ORBITALS

n l subshell ml

1 0 1s 0

2 0 2s 0

1 2p -1,0,+1

3 0 3s 0

1 3p -1,0,+1

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

4 0 4s 0

1 4p -1,0,+1

2 4d -2,-1,0,+1,+2

3 4f -3,-2,-

1,0,+1,+2,+3 and so on...

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BORN POSTULATE

The probability of finding an electron in a certain region of space is proportional to 2, the square of the value of the wavefunction at that region.

 can be positive or negative. 2 is always positive

2 is called the “electron density”

What is the physical meaning of the wave function?

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E.g., the hydrogen ground state

1 1 3/2

1s = e -r/ao (ao: first Bohr radius=0.529 Å)

 ao

1 1 3

21s = e -2r/ao  ao

21s

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Higher s orbitals

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Balloon pictures of orbitals

The shape of the orbital is determined by the l

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Radial electron densities

The probability of finding an electron at a distance r from the nucleus, regardless of direction

The radial electron density is proportional to r22

Surface = 4r2

r

Volume of shell = 4r2 r

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Radial electron densities

r22

Riferimenti

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