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TRANSCRIPT
Investigation of Structure and Dynamics in
Polymeric Systems via Solid State NMR
Robert Graf
Max-Planck-Institut für PolymerforschungMainz
March 2nd, 2005
founded 1983, 450 co-workers, on campus of the University of Mainz,
interdisciplinary fundamental research of polymers
Max Planck Institute for Polymer Research
MPI-P OrganizationBoard of Directors
MaterialsScience
Knoll
Theory
Kremer
Synthesis
Müllen
Solid StateChemistry
Wegner
PolymerPhysics
Butt
ScientificScientificProject AreasProject Areas
PolymerSynthesis
SupramolecularArchitecture
Surfacesand Interfaces
Developmentof Methods
Structureand Dynamics
FunctionalMaterials
Mass Spectrometry
High Resolution NMR
Optical Spectroscopy
Thin Films
Microscopy
Polymer Analysis
Computer and Network Service
Clean Room
Mechanical and Dielectric Relaxation
X-Ray Structure Analysis
Max Planck Institute for Polymer Research
Spectros-copy
Spiess
Scientific Activities of the MPI-P Spectroscopy Group
Structure and DynamicsStructure and Dynamics Development of MethodsDevelopment of Methods
Functional MaterialsFunctional Materials Supramolecular ArchitecturesSupramolecular Architectures
Su
rface
s & In
terfa
ces
Su
rface
s & In
terfa
cesP
oly
mer
Syn
thesi
sP
oly
mer
Syn
thesi
s
2D Multiple Quantum MAS NMRImaging of Hyperpolarized GasesDFT CalculationsPulsed and CW EPR Fourier-Transform Rheology
Polymer Chain DynamicsLocal-Order Phenomena
Polyelectrolyte MultilayersSelf Assembled Monolayers
Surface Patterning
PhotoconductorsProtonconductors
Shape-Persistent Macromolecules
Columnar π-π StackingHydrogen-Bonded StructuresCoordination Polymers
Polymerization: Radical, Anionic, Emulsion, Atom-Transfer Radical Isotopic Labelling
SpectroscopyGroup
•••••
•••
•••
••
•••
•
•
Investigation of Structure and Dynamics in Polymeric Systems via Solid State NMR
Introduction •
Solid State NMR •
Polymer dynamics •
Conclusions •
interactions in solid state NMR
resolution enhancement in solid state NMR, magic angle spinning, recoupling methods, double quantum NMR spectroscopy
Polyelectrolyte layers, polybutadiene, PEMA
Pro and Contra of Solid State NMR investigations
Molecular Structures and Dynamics via NMR
i
i0iZ BH I∑γ−=
Important NMR interactions:
Zeemann Interaction :
i
i0iCS BH Iσ∑γ−=Electronic Shielding :
i
i
i)1I2(I2
eQQH IVI∑ −−= hQuadrupol Interaction :
[ ]∑≠
γγπ
μ ⋅−⋅⋅−=ji
jijir3
r4D )r)(r(H 23ji0 IIIIh
Dipol-Dipol Interaction :
∑≠
⋅−=ji
jijiJH IJIIndirect Spin-Spin Interaction :
H = HZ + HQ + HCS + HD + HJ
Interactions in Solid State NMR Spectroscopy
ij0,2ij
2
ji21
r4D )1cos3(H 3ij
ji0 T−θ= ∑≠
γγπ
μ h
PerturbationTheory Orientation dependence of local spin interaction on B0
HQ, HD, HCS, HJ
Isotropic ContributionsHCS: chemical shift
HJ: J-couplings
Liquid state NMR
Anisotropic Contributions
SymmetricHQ: quadrupol
HD: dipol-dipol
HCS: chemical shift
AsymmetricHQ: quadrupol
HCS: chemical shift
Zeemann interaction dominates all other NMR interactions
Distance Orientation
θ
B0B0 θ
1H NMR Spectra in Liquid and in Solid State
60 40 20 0 -20 -40 k-60 Hz
5 0 kHz
20 10 0 kHz
static
30 kHz MAS
Solution
isotropic moleculardynamics
3 kHz4HRMAS soft
matter
rigid solid
dipolarbroadening
Spectral Resolution Enhancement in Solid State NMR
dipol-dipol coupling:
i
j
θij
B0
RF irradiation:
$ ( cos ) ( $ $ $ $ ), ,Hr
I I I Iij
ij i j Z i Z j i j∝ − − ⋅1
3 1 3312
2 θ γ γ
$ $ $, ,H R T= ⋅2 0 2 0
$,T2 0
0
space spin
0 tC
-x y -y x
tτ ττ τ2τ τ ττ τ2τ τ ττ 2τ
-x y -y x -x y -y
tC
magic angle spinning:
$,R2 0 0 ωR
θ
θm
ωR
θm
ωR
B0 B0 B0 B0
0 tR
t
tR
(CRAMPS)
(Recoupling)HD,eff.
x y -y-x
τ τ
x y -y-x
τ τ
x y-x
τ
Double Quantum NMR Spectroscopy under MAS
ω ωDQ SQ ii
= ∑ ,
I f D tDQ ij ij, ( )= ⋅
d Mdt ≈ 0
preparation reconversionevolution t1 detection t2
6.0 5.0 4.0 3.0 2.0 ppm12
10
8
6
4ppm
CH CH2
-CH2
CH2-CH
CH=CH
doub
le q
uant
umdi
men
sion
(f 1)
single quantum dimension (f2)
properties of double quantum coherences :
Molekulare Stuktur von Silikat-Schichten
Analysis of layered silicates via next nearest neighbor relations
Single quantum dimension
Dou
ble
quan
tum
dim
ensi
on
29Si double quantum spectrum: DQ intensity ∝ r-6 => coordination shells
-150-100-50 ppm0
Q4
Q3
Molecular Structure of Layered Silicates
A
B C
DE
structure of layered silicates from analysis of spatial proximitiesN. Hedin et al., J. Am. Chem. Soc. 126, 9425 (2004).
single quantum dimension
doub
le q
uant
umdi
men
sion
29Si double-quantum spectrum: DQ-Intensities => coordination spheres
Polybenzoxazines
N
O
X
R
N
OH OH
R
n-1X X
Ring Opening
Useful Properties• High Tg
• Good mechanical properties
• Excellent UV and chemical resistance
Unusual Properties• Low water absorption
• Low volumetric expansion on curing
• High modulus
Hydrogen-bonded network
What is the nature of the network?
Benzoxazine Oligomers Studied by 1H DQ NMR
Dimer Trimer Tetramer
Changes in hydrogen bonding structure evident from changing 1H resonances and DQ contacts
Hydrogen Bonds Assigned via DFT-Based Chemical Shift Calculations
1H chemical shifts influenced by proximity to oxygen. Helical structure predicted for polymer.
G. R. Goward et al., J. Am. Chem. Soc. 125, 5792 (2003).
Isolated Dimer Pair - X-ray StructureIntra:Inter = 1:1
Trimer forms Planar Ring Intra:Inter = 2:1
Tetramer forms Overlapping Loop Intra:Inter = 3:1
Calculated and experimental 1H NMR spectra agree, particularly in hydrogen-bonding region.
Dimer Trimer Tetramer
Order Parameter in Liquid Crystalline Phases
2.54 Å
1.83 Å
2.49 Å
2.48 Å
1.83 Å
2.56 Å
A
B
C
CD
F
G
FE
D
chemical structur of nematic model
compound
order parameter Sij :
)1cos3(S 221
ij −θ=
stat,ij
eff,ijij D
DS =
c
A BC
D
E
F
G
G-GF-FE-E
D-E
D-D
C-D
B-CA-C
ppm
8 7 6 5 4 3 2 ppm16
14
12
10
8
6
4
2
doub
le q
uant
um d
imen
sion
single quantum dimension
Order Parameters in Liquid Crystalline Systems
0,0 0,1 0,2 0,3 0,4 0,5 0,60,0
0,1
0,2
0,3
0,4
0,5
BC DQ coherences
DQ
Inte
nsity
[a.
u.]
DQ-Preparation Time [ms]
BC DQ coherence
-100100 0 kHz
orde
r par
amet
erS
0.0
0.1
0.2
0.3
0.4
0.5
0.6
A-C B-C D-D E-E F-F G-G
F
D
C
B
A
CD
E
F
G
orientation of nematic
directorDQ sidebands
DQ intensity
Introduction •
Solid State NMR •
Polymer Dynamics •
Conclusions •
Interaction in solid state NMR
MAS, recoupling, double-quantum NMR
Polyelectrolyte multi layers,reptations-model, scaling laws in polymer dynamics, influence of rigid confinements, conformational stability in PEMA melts.
Pro and Contra Solid State NMR investigations
Investigation of Structure and Dynamics in Polymeric Systems via Solid State NMR
Polyelectrolyte Multi-Layers
Structure of Polyelectrolyte Layers
DQ NMR Investigation of Structure: PEM vs. PEC
N+
SO O
O-
HH
HH
H
H
H
H
H3C CH3
Polyelectrolyte MultilayerPolycationSolution
PolyanionSolution
Anionic Substrate
Aqueous Rinse
After 3 cycles
Polyelectrolyte Complex
PolyanionSolution
Polyelectrolyte Complex Formation
9 8 7 6 5 4 3 2 1
2
4
6
8
10
12
14
16
18
Single Quantum Dimension [ppm]9 8 7 6 5 4 3 2 1
Single Quantum Dimension [ppm]
Double
Quantu
m D
imen
sion [
ppm
]
2
4
6
8
10
12
14
16
18
Double
Quantu
m D
imen
sion [
ppm
]
PolycationSolution
After Drying
Molecular Dynamics in Polyelectrolyte Multi Layers
N+
HH
HH
H 3C CH 3
SO O
O-
H
H
H
H
1 2 3 4 5 6 7 9 108 C
PSS 500 MHzPDADMAC 500MHzPSS 700 MHzPDADMAC 700MHz
200
400
600
800
1000
Number of Layers
T1
[mse
c]
Spin-LatticeRelaxation
10-12 10-11 10-10 10-9 10-8 10-7 10-6 10-5
0,01
0,1
1
10
500 MHz700 MHz
correlation time τ [s]
T 1[s
]
theoretical T1 relaxation behavior:
Localization of Water in Polyelectrolyte Multilayers
Layer 1
Layer 2
Layer 3
Layer 4
Layer 5
Layer 6
Layer 7
Layer 8
Layer 9
Layer 10
ppm12 10 8 6 4 2 0
5.0
4.8
4.6
4.4
4.2
4.0
3.8
3.6W
ate
r Che
mi c
al S
hift
[ppm
]
1 2 3 4 5 6 7 8 9 10Layer Number
bulkPDADMAC
bulk PE C
bulk PS S
SO O
O-
H
H
H
H
N+
HH
HH
H3C CH3
8 7 6 5 4 3 ppm
1H MAS NMR Spectra 1H Chemical Shift
M. McCormick et al., Macromolecules 36, 3616 (2003).S. Pawsey et al., J. Am Chem. Soc. 125, 4174 (2003).
Length- and Time Scales in Polymer Dynamics
t > τeslow, collective
Reptation dynamics
t < τe
fast, local dynamics
separation of time scales!
dynamic regimes of the Reptation model :
τR
log(t)
log
[Rn(
t)-R
n(0)
]2
∝ t1/2
∝ t
∝ t1/4
∝ t1/2
τdτe
I. II. III. IV.
DQ Measurements of Dynamics on Different Time Scales
θ(t1)
θ(t0) θm + α(t)
t = 0 t ≈ τe t > τe
I dt dt D d t d tDQt t
t tt
ij eff m m∝ ′ ′′ ⋅ ′ ′′+
+
−∫∫1
12
0
2
22
22
, ,( )
,( )( ) ( )
return-to-origin probability C (t)
corresponds tod t d tm exc m rec t22
22
,( )
. ,( )
.( ) ( )− ′ ⋅ ′′
S Ne≈ −35
1polymer network theory :
Polybutadien : S MMKuhn
e≈ ≈3
5 003.
static systems : Sij(t)=1isotropic motion : Sij(t)=0
S D Dij ij eff ij= , /local order parameter :
Local Order Parameters in 1,4 Polybutadien Melts
SH-H = 0.13
S = 0.06-H2
S = 0.08H2-HT=Tg+50K
⇒ SC=C = 0.20 ± 0.05 6.0 5.0 4.0 3.0 2.0 ppm
12
10
8
6
4ppm
CH CH2
-CH2
CH2-CH
CH=CHdo
ubel
quan
tum
dim
ensi
on(f 1
)
single quantum dimension (f2)
1H double quantum NMR spectrum Dynamic order parameter
via residual dipolar couplings
S
Time Dependence of Local Order Parameter
10-1
100
101
102
103
t / te(T)
~ t -1/2
~ t -1/4
C (t
)tc( ) tc( )
1,0
0,1PB MW ≈ 76 Me
PB MW ≈ 11 Me
PB MW ≈ 4 Me
double-quantum filtered experiments on 1,4 poly-butadien
Reptation-model predicts two scaling laws:
S~t -1/4 and S~t -1/2
R. Graf et al., Phys. Rev. Lett. 80, 5738 (1998).
Molecular Weight Dependent Dynamics of PB Melts in PS-PB
Tethering a PB chain end to a rigid PS block stabilizes the t-1/4-regime
10
0.01
0.1
1
10
PS-b-PB 12k-10kPS-b-PB 22k-24kPS-b-PB 90k-120k
101010.01
0.1
1
10
D CH
=CH
/ kH
z
S(t/
t e)
102 103 104 10510010−1
t/ t e
~t −1/4
Influence of Rigid Confinements on Polymer Dynamics
PS-b-PB PS-b-PB-b-PSPB
0.01
0.1
1
~ t −1/4
t / te
PS-b-PB PB
0.01
0.1
1
10
PS-b-PB-b-PS
S (t/ t
e) CH
=CH
DC
H=C
H /
k Hz
102 103 104 10510010−1 101
~ t −1/2
T. Dollase et al., Macromolecules 34, 298 (2001).
PS-b-PBPB
PB inPS-b-PB
Polymer Dynamics in heterogeneous Polymer Melts
1010.01
0.1
1
10
0.01
0.1
1
10210010−1 103 104 105
t / τe
DC
H=C
H /
kHz
S(t/
τ e) C
H=C
H
PS-b-PB p6 (12k-10k)5 % PB p6 in PS-b-PB d6PB p6 (10k)
~t −1/2
~t −1/4
S(t/
t e)
t / te
Variation of Dynamic Order Along the Polymer Chain
10-2 10-1 100 101 102 10310-3
10-2
chain endchain centerwhole chain
PB(d6)-PB PB(d6)-PB-PB(d6) PB
~ t -1/4
~ t -1/2
t / te
S(t/
t e)
a-PEMA: Isotropisation of Chain Dynamics
180°
CO
13
ω33<10°
ω22
ω11
180°C
O13
0° - 180°
180°
CO
13 ω
50°ω
400 K
405 K
411 K
433 K
472 K
394 K
250 200 150 100
298 K
ω
ω
ω22
ω33
ω11
1D 13C NMR: experimentsimulation
Melt
Gla
ss
Tg
Melt
a-PEMA: Isotropisation of Chain Dynamics
200
150
100200 150 100250
250
[ppm
]ω
2
[ppm]ω1
T = 300 K
ω11
ω22 ω33
180°
CO
13
ω33<10°
ω22
ω11
200
150
100
200 150 100
T = 416 K
tc = 2,1.10-5 s
[ppm
]ω
2
[ppm]ω1
180°C
O13
0° - 180°
T = 394 K
tc = 3,3.10-4 s
200
150
100
200 150 100
[ppm
]ω
2
[ppm]ω1
ωω
180°
CO
13 ω
50°ω
Dynamic Models: Random Jump vs. Rotational Diffusion
rotational diffusion experimental results random jump
200
150
200 150 [ppm]
[ppm]
200
150
200 150 [ppm]
[ppm]
200
150
200 150
tc=3,3 .10-4s
[ppm]
[ppm]tc =3,3.10-4s T = 394 K
200
150
200 150
tc =8,3.10-5s
[ppm]
[ppm]
200
150
200 150 [ppm]
[ppm]
200
150
200 150
tc=8,3.10-5s
[ppm]
[ppm]T = 405 K
M. Wind et al., Solid State NMR 27, 132-139 (2005).
Time Sclaes of Molecular Dynamics PEMA Melts
Arrhenius-diagram of dynamic processes in PEMA
corr
elat
ion
time
[s]
10-8
10-6
10-4
10-2
100
102
2.2 2.4 2.6 2.8 3.0 3.2 3.4
1000 / T [K-1]2.0
Tg = 338K
α-relaxation( tα)
β-relaxation( tβ)
αβ-relaxation( tαβ)
NMR
DielectricPCS
conformationalisotropisation (tR/I)
Length Scale of Isotropisation Process
**
*
*
**
*
*
T - Tg
95 K
55 K
410 K
449 K
395 K
434 K
387 K
426 K
322 K
346 K
379 K
403 K
300 K 300 K 300 K 221 K278 K
δ [ppm]100150200250
δ [ppm]100150200250
δ [ppm]100150200250
δ [ppm]100150200250
δ [ppm]100150200250
Mw = 600 kg mol -1 Mw = 15,9 kg mol -1 Mw = 7,6 kg mol -1 Mw = 1,4 kg mol -1 Mw = 0,46 kg mol -1
Mw/Mn = 1,53 Mw/Mn = 1,61 Mw/Mn = 1,48 Mw/Mn = 1,07 Mw/Mn = 1,14
from radicalic polymerisation from anionic polymerisation
M. Wind et al., Macromol. Chem. Phys. 206, 142 (2005).
Organisation in Poly(Methacrylats): WAXS(LVDW)
PMMA
PEMA
PBMA
PHMA
Inte
nsity
[a.u
.]
q [nm-1]0 10 20
II/I
WAXS-DataIII
(VDW)
III
?
0
0.4
0.8
1.2
1.6
0 2 4 6 8 10 12number of side chain C atoms
Bra
ggdi
stan
ce d
[nm
]
I
II
III
(VDW)
(LVDW)
Bragg distances
syndiotacticpoly(methacrylate)
main chain
side chains
dI
dIII
d0
dIII
dII
"Nano Layers"
isotacticPEMA
main chains
side chains
extrapolatedlokal structur:
M. Wind et al., J. Chem. Phys. 122, 14906 (2005).
Introduction •
Solid State NMR •
Polymer Dynamics •
Conclusions •
Interaction in solid state NMR
MAS, recoupling, double-quantum NMR
polyelectrolyte layers, polybutadiene, PEMA
solid state NMR investigations
Investigation of Structure and Dynamics in Polymeric Systems via Solid State NMR
+
Pro and Contra of Solid State NMR Investigation
T = 394 K
tc = 3,3.10-4 s
200
150
100
200 150 100
[ppm
]ω
2
[ppm]ω1
ωω
T = 394 K
tc = 3,3.10-4 s
200
150
100
200 150 100
[ppm
]ω
2
[ppm]ω1
ωω
θ(t1)
θ(t0) θm + α(t)
elucidation local structures in partially disordered systems
supra-molecular structures in hydrogen bonded systems
local molecular dynamics
needs expertise-expensive-
correlation of dynamic processes and chemical structure
single quantum dimension
doub
le q
uant
umdi
men
sion
single quantum dimension
doub
le q
uant
umdi
men
sion
- ...
+
+
+
Acknowledgements
Prof. Dr. H. W. Spiess ($, €, …)
Dr. I. Schnell, Dr. K. Saalwächter, Dr. M. Feike,Dr. S. Hafner, Prof. D. Demco. (NMR)
Prof. B. Chmelka, Dr. N. Hedin (layered silicates)
Prof. K. Ishida, Dr. D. Sebastiani (polybenzoxazines)
Prof. L. Reven, Dr. M. McCormick (polyelectrolytes)
Prof. A. Heuer (polymer theory, …)
Dr. T. Dollase, Dr. M. Neidhöfer (polybutadiene)
Dr. M. Wind, Dr. W. Steffen, Prof. Do Yoon (PEMA)