kinetics of photochemical reaction
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23.7 Kinetics of photochemical reactions
Primary photochemical process:products are formed directly from theexcited state of a reactant.
Secondary photochem ical process:intermediates are formed directly from theexcited state of a reactant.
Photophysical processes compete with theformation of photochemical products via
deactivating the excited state
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Times scales of photophysical processes
Within 10-16~ 10-15s for electronic transitions induced byradiation and thus the upper limit for the rate constant of afirst order photochemical reaction is about 1016s-1.
10-12~ 10-6s for fluorescence
10-12~ 10-4s for intersystem crossing (ISC)
10-6~ 10-1s for phosphorescence (large organic molecules)
A slowly decaying excited species can undergo a very largenumber of collisions with other reactants before deactivation.
The interplay between reaction rates and excited statelifetimes is a very important factor in the determination ofthe kinetic feasibility of a photochemical process.
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The primary quantum yield, , the number ofphotophysical or photochemical events that lead
to primary products divided by the number ofphotons absorbed by the molecules in the sameinterval, or the radiation-induced primary eventsdivided by the rate of photo absorption.
The sum of primary quantum yields for allphotophysical abd photochemical events mustbe equal to 1
)(
)(
absorbedlightofintensityI
processtheofratev
absorbedphotonsofnumber
eventsofnumber
abs
1i
i
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From the above relationship, the primary
quantum yield may be determined directly fromthe experimental rates of ALL photophysical
and photochemical processes that deactivate
the excited state.
i absi
i
iI
v
i
ii
v
v
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Decay mechanism of excited singlet state
Absorption: S +hv
i S*v
abs=Iabs
Fluorescence: S* S + hvi vf= kf[S*]
Internal conversion: S* S vIC= kIC[S*]
Intersystem crossing: S* T* vISC= kISC[S*]
S* is an excited singlet state, and T* is an excited triplet state.
The rate of decay = - kf[S*] -kIC[S*] - kISC[S*]
When the incident light is turn off, the excited state decays exponentially:
with
dt
Sd *][
0
0
/*][*][
tt eSS
I SCICf kkk
1
0
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If the incident light intensity is high and the absorbance
of the sample is low, we may invoke the steady-state
approximation for [S*]:Iabs - kf[S*] -kIC[S*] - kISC[S*] = 0
Consequently,
Iabs = kf[S*] -kIC[S*] - kISC[S*]
The expression for the quantum yield of fluorescence
becomes:
The above equation can be applied to calculate the
fluorescence rate constant.
I SCICf
f
abs
ff
kkk
k
I
v
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Quenching The presence of a quencher, Q, opens an additional channel for
deactivation of S*
S* + Q S + Q
vQ= kQ[Q][S*]
Now the steady-state approximation for [S*] gives:
Iabs
- kf
[S*] -kIC
[S*] - kISC
[S*] -kQ
[Q][S*] = 0
The fluorescence quantum yield in the presence of quencherbecomes
The ratio of / fis then given by
Therefore a plot of the left-hand side of the above equation against[Q] should produce a straight line with the slope
0k
Q. Such a plot is
calledStern-Volmerplot. (fluorescence intensity and life time)
][Qkkkk
k
QISCICf
f
][QkQof
1
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The fluorescence intensity and lifetime are both
proportional to the fluorescence quantum yield, plot of
If,0/I0and t0/t against [Q] should also be linear with thesame slope and intercept as
Self-test 23.4 The quenching of tryptophan
fluorescence by dissolved O2gas was monitored by
measuring emission lifetimes at 348 nm in aqueous
solutions. Determine the quenching rate constant for
this process[O2]/(10
-2M) 0 2.3 5.5 8 10.8
Tau/(10-9s) 2.6 1.5 0.92 0.71 0.57
][QkQof
1
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Three common mechanisms for
bimolecular quenching
Collisional deactivation:
S* + Q S + Q
is particularly efficient when Q is aheavy species such as iodide ion.
Resonance energy transfer:
S* + Q S + Q*
Electron transfer: S* + Q S+ + Q- or
S* + Q S- + Q+
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Energy Transfer Processes
(Forster theory,1952) Energy transfer is moreefficient when
1. The energy donor and acceptor are separatedby a short distance, in the nanometer scale
2. Photons emitted by the excited state of the
donor can be absorbed directly by the acceptor
The efficiency of energy transfer, ET, equals
Where R is the distance between the donorand the acceptor. R0is a parameter that ischaracteristic of each donor-acceptor pair.
Fluorescence resonance energy transfer (FRET)
66
0
6
0
0,
1
RR
REE T
f
f
T
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Electron transfer reactions
(Marcus theory) The distance between the donor and acceptor, with
electron transfer becoming more efficient as the distancebetween donor and acceptor decrease.
The reaction Gibbs energy, rG, with electron transferbecoming more efficient as the reaction becomes moreexergonic.
The reorganization energy, the energy cost incurred by
molecular rearrangements of donor, acceptor, andmedium during electron transfer.
The electron transfer rate is predicted to increaseas this reorganization energy is matched closely by thereaction Gibbs energy.
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23.8 Complex photochemical
processes
The overall quantum yield of a photochemical
reaction. (can be larger than 1)
Rate laws of complex photochemical reactions.
Photosensitization (no direct absorption).
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Quantum yield of a complex
photochemical reaction
Overall quantum yield: the number of reactant
molecules consumed per photon absorbed:
For example: HI + hv H. + I.
HI + H. H2 + I.
I. + I. + M I2 + M*
Here the overall quantum yield is two, because the
absorption of one photon destroys two reactant
molecules HI. Therefore, in a chain reaction the overall
quantum yield can be very large.
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Example:When a sample of 4-heptane was irradiatedfor 100s with 313 nm radiation with a power output of
50W under conditions of total absorption, it was foundthat 2.8 mmol C2H4was formed. What is the quantumyield for the formation of ethylene?
Solution: First calculate the number of photons generated in theinterval 100s.
Then divide the amount of ethylene molecules formed bythe amount of photons absorbed.
N(photons) = Pt/(hc/)
= n(C2H4)*NA/N
= 0.21