WAVE MECHANICS Schrdinger 1926 The currently accepted version

  • Slides: 10
Download presentation
WAVE MECHANICS (Schrödinger, 1926) The currently accepted version of quantum mechanics which takes into

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 y, called the “wave function”. * y can be obtained by solving Schrödinger’s equation (a differential equation): Hy=Ey ^ This equation can be solved exactly only for the H atom

WAVE MECHANICS * This equation has multiple solutions (“orbitals”), each corresponding to a different

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

WAVE MECHANICS * The energy depends only on the principal quantum number, as in

WAVE MECHANICS * The energy depends only on the principal quantum number, as in the Bohr model: En = -2. 179 X 10 -18 J /n 2 * 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”.

HYDROGEN ORBITALS n 1 2 l 0 0 1 3 0 1 2 4

HYDROGEN ORBITALS n 1 2 l 0 0 1 3 0 1 2 4 0 1 2 3 and so on. . . subshell 1 s 2 s 2 p 3 s 3 p 3 d 4 s 4 p 4 d 4 f ml 0 0 -1, 0, +1 -2, -1, 0, +1, +2 -3, -2, -1, 0, +1, +2, +3

What is the physical meaning of the wave function? BORN POSTULATE The probability of

What is the physical meaning of the wave function? BORN POSTULATE The probability of finding an electron in a certain region of space is proportional to y 2, the square of the value of the wavefunction at that region. y can be positive or negative. y 2 is always positive y 2 is called the “electron density”

E. g. , the hydrogen ground state y 1 s = y 21 s

E. g. , the hydrogen ground state y 1 s = y 21 s = 1 1 3/2 ao p 1 3 ao e -r/ao e (ao: first Bohr radius=0. 529 Å) -2 r/ao y 21 s r

Higher s orbitals All s orbitals are spherically symmetric

Higher s orbitals All s orbitals are spherically symmetric

Balloon pictures of orbitals The shape of the orbital is determined by the l

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

Radial electron densities The probability of finding an electron at a distance r from

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 r 2 y 2 Dr Surface = 4 pr 2 Volume of shell = 4 pr 2 Dr

r 2 y 2 Radial electron densities Maximum here corresponds to the first Bohr

r 2 y 2 Radial electron densities Maximum here corresponds to the first Bohr radius