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PHOTONS IN CHEMISTRY OUT WHY BOTHER?. E = h ν λν = c [3 10 8 m/s]

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Presentation on theme: "PHOTONS IN CHEMISTRY OUT WHY BOTHER?. E = h ν λν = c [3 10 8 m/s]"— Presentation transcript:

1 PHOTONS IN CHEMISTRY OUT WHY BOTHER?

2 E = h ν

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4 λν = c [3 10 8 m/s]

5 ~ 450-750 nm Take 500 nm

6 Boltzman T [ o K]n 2 /n 1 3003 x 10 -42 4007 x 10 -32 10003.4 x 10 -13 2,0006 x 10 -7 5,0003 x 10 -3 6,4001 % 10,0005.7 % 20,00024 % 50,00056 %

7 Grotthuss-Draper law: Only the light absorbed in a molecule can produce photochemical Change in the molecule (1871 and 1841) Stark - Einstein: If a species absorbs radiation, then one particle is excited for each quantum of radiation absorbed

8 Stark - Einstein: If a species absorbs radiation, then one particle is excited for each quantum of radiation absorbed QUANTUM YIELD: Φ = The number of molecules of reactant consumed for each quantum of radiation absorbed Primary Φ ≤ 1 Sum of all primary Φ’s = 1

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10 Photochemical kinetics

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12 Transmittance Absorbance Beer’s Law

13 Molar extinction Coefficient ~250 L.mol -1 cm -1 Cross section ~10 -18 cm 2

14 NB 1: Beer fails when photochemistry happens NB 2: The photophysics Is hidden in σ (So we haven’t done much yet)

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16 Absorption of a mixture

17 Photochemical kinetics STEADY STATE HYPOTESIS

18 NB 2: The photophysics Is hidden in σ (So we haven’t done much yet)

19 EINSTEIN COEFFICIENT # of transitions / second: Amplitude of TRANSITION MOMENT # of molecules degeneracy Radiation density =# of photons/unit freq.

20 Stimulated emission Spontaneous emission

21 Stimulated emission Spontaneous emission

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24 Boltzman Planck

25 Oscillator strength

26 Lifetimes Einstein coefficients are rate constants

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28 Heisenberg may have been here

29 Contributions to excited state lifetime  Natural lifetime  Pressure broadening  Saturaiton broadening  Doppler broadening NB: f(v) in a gas is Gaussian  Doppler line shape is Gausian

30 (depends on coordinates of electrons and nuclei And on time) electrons Nuclei

31 NB: Resonant frequency NB 1: I = f  e 0 and µ becomes permanent dipole NB 2: ν if as beat frequency NB 3:compare to nuclear vibrations

32 Compare 10 15 s -1 to IR: Nuclear motion is 2 orders of Magnitude slower than Electronic motion Born-Oppenheimer approximation

33 Orthogonal (no overlap) tells if allowed or forbidden: must be symmetric  selection rules Franck-condon factors

34 M x is odd:

35 One more parameter………. SPIN αβ updown ↑↓ +½-½

36 If we can separate space and spin (no spin-orbit coupling):

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44 Conical Intersections R1 R2 E


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