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1
Negative Differential Resistanceof Extended Viologen.
Oscillations with Odd HarmonicFrequencies.
Stochastic Resonance.
J. Heyrovský Institute of Physical Chemistry, AS CR, Prague
Institute of Organic Chemistry & Biochemistry, AS CR, Prague
Lubomír Pospíšil, Magdaléna Hromadová
2
Redox reactions of organic radicalsExample of negative impedance causing oscillations
-1.5 -2.0 -2.5 -3.00.0
0.2
0.4
FA-i
/
A
E / V vs Fc
-10k -5k 0 5k
0
5k
10k
D
-6k -4k -2k 0 2k
0
2k
4k
6k
8k
F
-3k -2k -1k 0
-1k
0
1k E
0 2k 4k 6k
0
2k
4k B
0 2k 4k 6k
0
2k
4k A
-2k 0 2k
0
2k
C
-Z
''/o
hm
.cm
2
Z' / ohm.cm2
aromatic nitro-compounds
This presentation: extended viologenNegative differential resistance near E0
3
4
Why to deal with electrochemicaloscillators?
Good models for system dynamics
Many controlling parameters
Electrical current or potential directly monitorsthe rate of kinetics
5
Why to model oscillations andchaos?
Climate & geophysics(7 years polar motion, El Nino, sea temperature)
Economic & Social(business cycle, generation gaps, news cycle)
Astronomy(helioseismology, cosmological cyclic model, neutron stars)
6
Common chemical reactions:reactants → products
The first electrochemical oscillator:1828 Fechner
Periodic release of gas bubblesfrom iron in HNO3
G. Th. Fechner: Schweiger’s J. Chem. Phys. 53 (1828) 129
7
Important oscillating processes:
Circadian clock, or circadian oscillatorbiochemical mechanismoscillates with a period of 24 hours
8
Important oscillating processes:
Alpha waves: neural oscillations in brainfrequency 8 – 12 Hz1931 Berger inventor of electro-encephaloraphy
9
Belousov–Zhabotinsky reaction
1950 Boris Belousov1961 Anatol Zhabotinsky1968 congress in Prague and dissemination to the West
Classical example of non-linear thermodynamicsmix of potassium bromate, Ce(IV) sulfate, propanedionic acid and citric acidin dilute H2SO4
concentration of the cerium(IV) and cerium(III) ions oscillatescolor oscillates: yellow ↔ colorless
reduction Ce(IV) → Ce(III) by propanedionic acid oxidation back to Ce(IV) → Ce(III) ions by bromate(V) ions.
10
Two driving forces of opposite sense
Mass on a string & gravity
Charging a capacitor in parallel with inductance
Energy dissipation as heat, friction,… damping
External energy source: driven oscillator
Damped & driven oscillators
11
Oscillating reactions
Corrosion of metals in acids
Oxidation of organic compounds on Cuelectrodes
Electrocatalysis by adsorbed ions
Oxidation of gaseous CO on Pt
Bio-processes
12
Outline of our recent results
Molecular conductors –
viologen oligomers
Driven oscillations yield only odd harmonics
Stochastic resonance of a driven system
13
Molecular conductorsocto- and deca-cations of “extended viologens”
N NAcHN NHAcN N N N N N N N
Two electrons for each viologen unit
n = 2, 3, 4, 5, 6
14
DC polarograms (low current damping)Reversible 3-electron reductionCurrent instability near potential E0
0.7 mM 0.07 mMConcentration
of extended viologen
15
Mechanism & models
Positive feed-back loop:
disproportionation re-generates reducible parent form
1)-(n1)-(n2)-(nn
2)-(n1)-(nn
WWWW
...WWW ee
Negative feed-back loop:change of concentration gradient & mass transport
16
e-
e-
e-
18+18+
17+17+
16+16+
15+15+
+e-
-e--
-e--
+e-
electrode solution of 18+
masstransport
heterogeneouselectron transfer
homogeneousbimolecular
electron transfer
Coupling of heterogeneous and homogeneouselectron transfers & mass transport
Oscillations caused by periodic changesof rates of heterogeneous electron transfer,
homogeneous electron transferand mass transport rate
Extended viologen:Negative differential resistance near E0
17
18
Extended viologen:AC polarograms with admittance < 0
Low frequency AC polarogram
0.32 Hz
Im
Re
19
Extended viologen:Currenttime series & FFT
Fourier transform
Odd harmonics: 3rd, 5th, 7th, 9th, 11th…
20
Extended viologen:Odd harmonics due to stochastic resonance
Stochastic resonance (SR)cooperative action of fluctuation andperiodic driving in bi- & multi-stable systems
SR can trigger the transfer of powerto the periodic signal and enhance it.
Driving by pickup of ~1 mV & 50 Hz
21
• 1980’s: Bartussek and co-workers: theory of higherharmonics for non-linear systems
• cases with potential-symmetric, potential-asymmetric,and additive or multiplicative fluctuations
• potential-symmetric systems suppress 2nd harmonicsand retain the odd harmonics
• Fast and reversible viologens are potentialsymmetric systems.
Theory of stochastic resonancein non-linear systems
Examples of stochastic resonancefrom other fields
GeoscienceLaser opticsAcousticsEnzymatic reactions
M. Hromadová, M. Valášek, N. Fanelli, H. N. Randriamahazaka, L. PospíšilStochastic Resonance in Electron Transfer Oscillations of Extended Viologen.J. Phys. Chem. C, 2014, dx.doi.org/10.1021/jp501608b
23
Co-authors:
Magdaléna HROMADOVÁMichal VALÁŠEKNicolangelo FANELLIHyacinthe N. Randriamahazaka
Acknowledgement:
Grant Agency Czech Rep.,
Joint project C.N.R.-AS CR
Joint project C.N.R.S.-AS CR
24Thank you for your attention
25
Chaos is lifePeriodicity is boring
Stability is death
Thank you for your attention
26
Can we predict a change:
stability – periodicity – deterministic chaos
???
27
Deterministic chaos random fluctuations
Observation at time tn depends on values at tn-1, tn-2, …
Functional dependence exists - may not be known
Random events do not correlate with previous eventsNo functional law
The proof of a hidden functionaldependence:
Do the observation in timeform an attractor ?
28
29
Attractor
An attractor can be a point, a finite set ofpoints, a curve, a surface,
or even a complicated set with a fractalstructure known as a strange attractor.
Observed time series: i(t1), i(t2),…i(tn-1), i(tn)
Plotting i(t) vs i(t - 2) vs i(t - 4 )
30
Extended viologen:Time delay analysis of experimental series
31
Deterministic chaos random fluctuations
Diagnostic criteria
5 10
-0.5
0.0
0.5
i/A
t / s
Current-time series → Time-delayed plot →→ Phase space diagram → Attractor orbit →→ Exponential evolution → Ljapunov exponent λ
0 10 20 30 40 50
-8
-6
-4
-2
S(
n)
n
exponential divergence of nearbytrajectories for three embedded
space dimensions → λ=0.41 > 0 !!!Reconstructed attractor
32
Ljapunov exponent :quantifies the stregth of chaos
Adjacent trajectories diverge in time
Chaos: exponentially fast rate of separation
δo distance between two points
δΔt = δo e λ Δt
Ljapunov exponent : averaged exponent λ
Type of motion: λ<0 … fixed point
λ=0 … stable orbit periodicityλ>0 … deterministic chaosλ= … noise
33
Universal theoryof deterministic chaos
Mitchell Feigenbaum (*1944)
Properties of iterating equations
Feigenbaum universality constant
34
Stability depends on parameter a
Quadratic iterator: xn+1 = a xn(1-xn)(Peitgen, Juergens, Saupe: Chaos and Fractals)
a
lim xn
n
35
Feigenbaum constant
lim = k-1 / kk
k-1
k
36
Feigenbaum constant stability – oscillation – deterministic chaos
lim = k-1 / kk
Experiment: = 4.68Theory: = 4.6692…
Universal constant : similar to universality of π
Experimental verification of only in few casesFeigenbaum constant for prediction of chaos
37
Other examples ofelectrochemical oscillators:
Cationic electrocatalysisAnionic electrocatalysis
38
Reduction of aromatic radical anionRepulsion is size-dependent
-1.5 -2.0 -2.5
0.0
0.5
1.0
1.5
2e-
1e-
3e-
HexBuPrEt
Me
-i/
A
E / V (Fc/Fc+)
Different tetra-alkyl ammonium salts as electrolytesDC polarograms:
Ar-NO2−●
39
Acceleration effect :Cationic catalysis
Ar-NO2−● + K+ ↔ [ Ar-NO2
−●, K+ ]
Ion- pair formation eliminates electrostatic repulsion
[ Ar-NO2−●, K+ ] + 3e- → Ar-NHOH + K+ ≈ -1.6 to -1.9 V vs Fc
" cationic catalysis "
Ion pairs are reduced at less negative potentials by 800 mV:
40
Termination of cationic catalysis
Acceleration effect is terminated at potentials of K+ reduction
K+ + e- ↔ K(Hg) ≈ -2.3 V vs Fc
-1.5 -2.0 -2.5
0.0
0.1
0.2
0.3
10 M KPF6
20 M KPF6
2
-i
/
A
E / V vs Fc
DCBA
50 M nitrobenzene
0.5 mM THexA PF6
-1.5 -2.0 -2.5
0.0
0.1
0.2
20 M KPF6
Ar-NO2 /Ar-NO2−●
K + / K
41
Negative impedance & Impedance discontinuity
-1.5 -2.0 -2.5 -3.00.0
0.2
0.4
FA-i
/
A
E / V vs Fc
-10k -5k 0 5k
0
5k
10k
D
-6k -4k -2k 0 2k
0
2k
4k
6k
8k
F
-3k -2k -1k 0
-1k
0
1k E
0 2k 4k 6k
0
2k
4k B
0 2k 4k 6k
0
2k
4k A
-2k 0 2k
0
2k
C
-Z
''/o
hm
.cm
2
Z' / ohm.cm2
42
Bursting oscillations at Hg dropping electrode
5 10 150
10
20
30
-i/
A
time/ s10 15 20
0
10
20
30
-i/A
time / s
10 15 200
10
20
30
-i/A
time / s
43
Chrono-amperommetry(reduction current – time, E=const.)
octo-cation
44
Small changes of potential:large effect on current oscillations
0 50-10
0
10
i
-0.560 V
0 50-10
0
10
-0.565 V
0 50-10
0
10
-0.570 V
0 50-10
0
10
i
-0.575 V
0 50-10
0
10
i
-0.590 V
0 50-10
0
10
i
-0.580 V
0 50-10
0
10
i
-0.595 V
0 50-10
0
10
i
-0.585 V
0 50-10
0
10
i
-0.610 V
curr
ent
time (0 – 100 sec)
deca-cation