gang ma, xiangke chen and heather allen the ohio state university june 21 st 2007 interfacial water...
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Gang Ma, Gang Ma, Xiangke ChenXiangke Chen and Heather Allen and Heather Allen
The Ohio State UniversityThe Ohio State University
June 21June 21stst 2007 2007
Interfacial water structure of phospholipid Interfacial water structure of phospholipid Langmuir monolayers investigated by Langmuir monolayers investigated by vibrational sum frequency generation vibrational sum frequency generation
spectroscopyspectroscopy
SFG
Lung SurfactantLung SurfactantAn essential component for our An essential component for our breathingbreathing
FunctionFunction
1.1. Reach near-zero surface tensionReach near-zero surface tension
2.2. Prevent lung from collapsePrevent lung from collapse
3.3. Ease work of breathingEase work of breathing
DPPC: Dipalmitoyl-phosphatidyl-choline
DPPE: Dipalmitoyl-phosphatidyl-ethanolamine
Broad Bandwidth Sum Frequency Broad Bandwidth Sum Frequency Generation &Generation &
Langmuir troughLangmuir trough
sample
vis
IR
vis + IR= sum
~100fs
SFG is a powerful technique providing vibrational spectra of interfaces.
Simultaneous acquisition of thermodynamic and spectroscopic data when combined with Langmuir trough.
Trough
0
10
20
30
40
50
60
70
80
10 20 30 40 50 60 70 80 90 100 110
mean molecular area (Å2/molecule)
su
rfa
ce
pre
ss
ure
(m
N/m
)
DPPC-d62
DPPE-d62
PA-d31
IsothermsIsotherms
LE
Condensed
LC
Gas
Free OD of neat DFree OD of neat D22OO
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
2550 2600 2650 2700 2750 2800 2850 2900
wavenumber (cm-1)
SF
In
ten
sity
(a.
u.)
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
2550 2600 2650 2700 2750 2800 2850 2900
SF
In
ten
sity
(a.
u.)
2740 cm-1
free OD of d62-DPPC
0
0.2
0.4
0.6
0.8
1
1.2
2550 2600 2650 2700 2750 2800 2850 2900
wavenumber (cm -1)
SF
Inte
nsi
ty (
a.u
.)DPPC-d62 free OD DPPC-d62 free OD
evolution evolution
Neat D2O
Π=0mN/m (G)
Π=0.5mN/m
Π=1mN/m (LE)
Π=8mN/m (LE)
Π=42mN/m (LC)
2740 cm-1
~2720 cm-1
~2680 cm-1
• Upon compression, two new bands at ~2680 cm-1 and 2720 cm-1 appear
- Free OD peak gradually disappears
DPPE-d62 free OD DPPE-d62 free OD evolution evolution
free OD of d62-DPPE
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
2550 2600 2650 2700 2750 2800 2850 2900
wavenumber (cm-1)
SF
In
ten
sity
(a.
u.)
Neat D2O
Π=1mN/m
Π=2mN/m (LC)
Π=42mN/m (LC)
~2670 cm-1
2740 cm-1
Which part of the lipid is perturbing the free OD slightlyslightly?
A comprehensive view
• Tail Hydrocarbon Chain?
Hydrophobic perturbation
• Head Phosphate, Choline or -C=O group?
H-bond interaction
Devlin P. has demonstrated that CH4 causes ice free OD to red shift!
Rowland B., Fisher M., Devlin P. J. Chem. Phys. 95(2), 1991
free OD of d31-PA
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
2550 2600 2650 2700 2750 2800 2850 2900
wavenumber (cm-1)
SF
In
ten
sity
(a.
u.)
How about PA-d31 (chain How about PA-d31 (chain only)?only)?
~2720 cm-1
~2670 cm-1
Π=0mN/m
Π=1mN/m
Π=3mN/m (LC)
Π=25mN/m (LC)
2740 cm-1
free OD of d31-PA (25mN/m) @26 C & 11C
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
2550 2600 2650 2700 2750 2800 2850 2900
wavenumber (cm-1)
SF
In
ten
sity
(a.
u.)
26 C
11 C
~2670 cm-1
Lowering temperature can reduce tail influence
from hydrogen bonding region
Distance-dependent hydrophobic perturbation
I~2670 cm
I I~2720 cm
I I I2740 cm-1
I~2670 cm-1
I I~2720 cm -1
I I I2740 cm-1
Distance-dependent hydrophobic perturbation
D2O
PA monolayer
~2670 cm-1 2740 cm-1 ~2720 cm-1
Air
ConclusionConclusion
Free OD/OH still persists at the interface even Free OD/OH still persists at the interface even under full monolayer coverage.under full monolayer coverage.
Due to a distance dependent chain Due to a distance dependent chain perturbation, the vibrational frequency of free perturbation, the vibrational frequency of free OD/OH red-shifts as the Langmuir monolayers OD/OH red-shifts as the Langmuir monolayers are packed more and more tightly.are packed more and more tightly.
Acknowledgements
Prof. H. Allen
Dr. Gang Maand
All Allen group members!
Thanks for your attention!!!