wave mechanics (schrödinger, 1926) the currently accepted version of quantum mechanics which takes...

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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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Page 1: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

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

^

Page 2: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

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 numbern=1,2,3,...

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

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

Page 3: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

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”.

Page 4: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

HYDROGEN ORBITALS

n l subshell ml

1 0 1s 02 0 2s 0

1 2p -1,0,+13 0 3s 0

1 3p -1,0,+12 3d -2,-1,0,+1,+2

4 0 4s 01 4p -1,0,+12 4d -2,-1,0,+1,+23 4f -3,-2,-

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

Page 5: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

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?

Page 6: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

E.g., the hydrogen ground state

1 1 3/2

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

ao

1 1 32

1s = e -2r/ao

ao

21s

r

Page 7: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

Higher s orbitals

All s orbitals are spherically symmetric

Page 8: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

Balloon pictures of orbitals

The shape of the orbital is determined by the l quantum number. Its orientation by ml.

Page 9: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

Radial electron densitiesThe probability of finding an electron at a distance r from the

nucleus, regardless of direction

The radial electron density is proportional to r22

Surface = 4r2

r

Volume of shell = 4r2 r

Page 10: WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into account the wave nature of matter and the uncertainty

Radial electron densities

Maximum here corresponds to the first Bohr radius

r2

2