Atomic Force Microscopy – More Than Microscopy
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Transcript of Atomic Force Microscopy – More Than Microscopy
School of Pharmacy
报告题目: Atomic force microscopy more than microscopy
( 原子力显微镜 – 不仅仅是显微镜 )
报 告 人:陈新镛 教授 University of Nottingham
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Atomic Force Microscopy– More Than Microscopy
Xinyong ChenLaboratory of Biophysics and Surface Analysis
School of PharmacyThe University of Nottingham
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ConstantForce.swf TappingMode.swf
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Outline
• Force measurement– Force/distance (f/d)– Two-dimensional Force measurement
• AC mode “force” measurement– Amplitude/distance (a/d)– Phase/distance (p/d)– Tapping mode imaging and a-p/d
• Other force-related afm techniques– Force-modulation imaging– Lateral-force (friction) imaging– Lateral resonance (AC mode lateral force)
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Force measurement
ForceCurves.swf
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Force/distance curves
Maximum adhesion
force
Contact region
ab
c
d
Scanner Displacement (nm)
Point of maximum
load
Deflect
ion/F
orc
e
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Experimental f/d curves
Approach Retract
School of PharmacySingle particle interaction between salbutamol, lactose and PTFE
Increase in
strength of
interaction with
salbutamol in air
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Avera
ge A
dhesi
on F
orc
e/n
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Lactose
Salbutamol
PTFE
International Journal of Pharmaceutics 238 (2002) 17-27
PTFE
Salbutamol
250 5000Distance (nm)
Forc
e
(nN
) LactoseAFM probe
Salbutamol
Measurement of
particle-particle
interaction
Lactose1µm
School of PharmacyAdhesion between a solid sphere and a solid plane (Hertz Model)
• JKR (Johnson, Kendall, Roberts – 1964-1971) model:
• DMI (Derjagin, Muller, Toropov – 1975) model:
• Maugis (1992):
Radhesion ofwork :Δγ ,
2
3RF
RF 2
F3
1
2
2
0
06.2
K
R
Stiff materials (DMT)
Compliant materials (JKR)
With complex and implicit parameter equations
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Specific interaction
Anti - Anti - Ferritin Ferritin AntibodyAntibody
FerritinFerritin
AFM Cantilever and ProbeAFM Cantilever and Probe
SubstrateSubstrate
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Antigen-antibody interaction
Biochemistry, 36, 7457 – 7463 (1997)
-0.6
-0.2
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-25 25 75 125 175
Distance moved by the Cantilever (nm)
For
ce (
nN)
ApproachRetract
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-25 25 75 125 175
Distance moved by the Cantilever (nm)
For
ce (
nN)
ApproachRetract
School of PharmacyMultiple link in tip/surface modification
Force versus probe-sample separation curves for a BBSA coated probe and (a) a streptavidin coated silicon surface, (b) a streptavidin functionalised surface after incubation in a solution of the bis-biotinylated peptide, and (c) the streptavidin/bis-biotinylated peptide/streptavidin multilayer.
The Analyst, 2000, 125(2), 245 - 250
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Force curve of chain-like molecules
School of PharmacyForce measurement of RNA molecules
Examples of the types of force curves observed between RNA functionalized AFM surfaces and tips; each curve has been corrected to show force against tip-sample displacement. In each example the approach trace is shown in gray and the retract trace in black. (A) No interaction has occurred between the tip and substrate. (B) A nonspecific interaction between the two surfaces, with no observable change in the gradient of the retraction slope. (C) A specific interaction between the two RNA functionalized surfaces, showing a stretch of ~10 nm before the rupture event.
Biophysical Journal 86:3811-3821 (2004)
School of PharmacyRepresentative force-extension traces for DNA molecules of three different lengths
Biochem. Soc. Trans. (2003) 31, (1052–1057)
School of PharmacyAntigen-antibody interaction
Anti - Anti - Ferritin Ferritin AntibodyAntibody
FerritinFerritin
AFM Cantilever and ProbeAFM Cantilever and Probe
SubstrateSubstrate
- Single antigen-antibody bond?
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0 0.25 0.5 0.75
Force (nN)
Antigen-antibody interaction- Single antigen-antibody bond?
Analysis of the distribution of adhesive forces (n = 140) obtained with three functionalized AFM probes. Each data point represents an individual force measurement performed at any position on the sample surface. The force distribution data is plotted, using data bin sizes from 15 to 35 pN, as a stacked area graph (smallest bin size plotted lowermost). In this way, common features of the distributions are reinforced by the stacking process. A quantization in the forces, with a period of 49 ± 10 pN, is suggested by this analysis.
Biochemistry, 36, 7457 – 7463 (1997)
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“Spacers” – a way to measure single molecular interaction
PEG attached Antibody
Mono-functional Spacer PEG molecules
Silicon Substrate
Covalently attached hCG
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Force measurements between PEG-antibody coated probes and hCG coated surfaces
-2
0
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0 100 200 300
Distance Moved by the Cantilever (nm)
ApproachRetractF
orce
(n
N)
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ce (
nN)
ApproachRetract
Distance Moved by the Cantilever (nm)
ApproachRetract
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Distance Moved by the Cantilever (nm)
For
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Distance moved by the Cantilever (nm)
ApproachRetract
For
ce (
nN)
(a) (b)
(c) (d)
Low probability in detectingsingle molecular pair interaction!
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Antibody-antigen interaction using polymeric linkers
Polymeric linker e.g. agarose, PEG
Antigen
Biotinylatedantibody
Streptavidin
PLA-PEG-Biotin
AFM probe
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Exploring surface hardness
Z
F
Z: Indentation on soft surfaces
Deflection onhard surfaces(no indentation)
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0.30 1.06 1.82 2.58 3.34 4.09 4.85 5.61 6.37 M ore
You ng 's M o dul u s (G pa )
Fre
qu
en
cy
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0.32 0.56 0.80 1.04 1.2 8 1.5 2 1.7 6 2.0 0 2.24 M or e
You n g's Mo du lus (Gpa )
Fre
qu
en
cy
Hertz Model:
2
1
2
3
2
4
)1(3
RZ
FE
crystalline budesonide Lactose
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Searching for specific interaction sites: Two dimensional force measurement
Functionalized probe
Array of Potential Interaction Sites
Specific Molecular Interaction
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Force-Volume (FV) mode
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School of PharmacyFV measurement of salbutamol particles on lactose-coated surfaces
AFM probe
Salbutamol
Scan probe whilst
recording adhesion events
Lactose1µm
A
B
A
B
A BForce distance curves extracted from the marked locations on the force volume image. The Salbutamol particle has greater adhesion to the lactose carrier at position B.
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FV measurement on BSA partially coated surfaces with a BSA-coated tip
Si
PS
BSA
Buffer
500 nm
Topography Adhesion
Langmuir 13, 4106 (1997)
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FV measurement on BSA partially coated surfaces with a BSA-coated tip:Time evolution
Langmuir 13, 4106 (1997)
Dynamic observation of BSA adsorption onto apolystyrene surface. Retract f-d curves were measured on apolystyrene spin-cast surface with a BSA-coated probe afterthe surface was exposed to a BSA solution (0.01 mg/mL, pH 7,100 mM phosphate buffer) for 0 min (I), 4 min (II), 5 min (III),7 min (IV), 10 min (V), and 60 min (VI) without movement ofthe sampling location.
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Pulsed-Force AFM
Topography
AdhesionDrive
Maximum force(Topography)
Adhesion
Stiffness
Sample: a silicon surface AFM tip: silicon, 4 N/m PF frequency: 905Hz
Tip oscillation
School of PharmacyPF-AFM images of PLMA/PmMl6 blend in water
PLMA: poly (lauryl methacrylate)PmMl6: 2-methacryloyloxyethyl phosphorylcholine-co-lauryl methacrylate (1:6)
1 m
Height Adhesion Stiffness
School of PharmacyPF-AFM images of a polystyrene surface partially coated with albumin
Height Adhesion5 m
0102030
0 4 8 12
Hei
gh
t (n
m)
0.0
0.3
0.6
0 4 8 12
Ah
esio
n (
V)
Albumin
Albumin
Polystyrene Buffer
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Si
PS
PF-AFM images of a polystyrene surface partially coated with fibrinogen
Fibrinogen
Height Adhesion1 m
0
2
4
0.0 1.0 2.0
Heigh
t (nm
)
0.00.51.01.5
0.0 1.0 2.0
Ahes
ion (V
)
Polystyrene
Fibrinogen
pH7 Phosphate Buffer
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-5
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-100 0 100 200 300 400 500
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-100 100 300 500 700 900
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Outline
• Force measurement– Force/distance (f/d)– Two-dimensional Force measurement
• AC mode “force” measurement– Amplitude/distance (a/d)– Phase/distance (p/d)– Tapping mode imaging and a-p/d
• Other force-related afm techniques– Force-modulation imaging– Lateral-force (friction) imaging– Lateral resonance (AC mode lateral force)
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Force measurement in AC mode
PhaseCurves.swf
AmplitudeCurves.swf
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40
45
50
-30 -20 -10 0 10
Relative scanner displacement (nm)
15
40
65
90
PS
PS30
35
40
45
50
-30 -20 -10 0 10
Relative scanner displacement (nm)
15
40
65
90
gel
gel
A-p/d curves measured on different material surfaces
30
35
40
45
50
-30 -20 -10 0 10
Relative scanner displacement (nm)
15
40
65
90
mica
mica
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
PS
PS3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
PS
PS
PS
PS3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
gel
gel
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
gel
gel
gel
gel
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
mica
mica
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
mica
mica
mica
mica
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Phase imaging
Phase Imaging
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Tapping mode images of gelatine on a mica surface
Height Phase
250 nm
Ultramicroscopy 75, 171 (1998)
Dark phase
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Tapping mode images of gelatine on a polystyrene surface
Height Phase
500 nm
Light phase
Ultramicroscopy 75, 171 (1998)
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3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
PS
PS3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
PS
PS
PS
PS3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
gel
gel
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
gel
gel
gel
gel
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
mica
mica
3 0
3 5
4 0
4 5
5 0
-3 0 -2 0 -1 0 0 1 0
Re la tive s ca nne r dis pla ce me nt (nm)
1 5
4 0
6 5
9 0
mica
mica
mica
mica
Phase imaging and a-p/d curves
Height Phase
Height Phase
Ultramicroscopy 75, 171 (1998)
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Physical meaning of phase contrast
= +
J.P. Cleveland et al., Appl. Phys. Lett. 72 (1998) 2613.
Energy dissipation model (J. Cleveland et al., 1998)
= –
Free of tip/sample interactions: = 90
School of PharmacyTM-AFM imaging of an EDMPC partially-coated mica surface
Height Phase
-5
0
5
10
15
20
25
13 15 17 19
RMS Amplitude (nm)
Dis
sip
atio
n P
ow
er
(pW
)
0
20
40
60
80
100
120
Pha
se L
ag
(D
eg
ree
s)
Mica, DissipationLiposome, DissipationMica, PhaseLiposome, Phase
Height Phase
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Physical meaning of phase contrast
Bistable status of tapping tips
0
5
10
15
20
25
0 3 6 9 12 15 18
Relative Z Scanner Displacement (nm)
RM
S A
mp
litud
e (
nm)
0
20
40
60
80
100
120P
hase
La
g (
de
gre
es)
Amplitude
Phase
ADRL
Setpoint
0
150
300
450
600
Co
unt
Mica
050
100150200250
0 4 8 12 16 20ADRL (nm)
Liposome
b
0
50
100
150
200
Liposome/Mica
c
a
Height Phase
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Outline
• Force measurement– Force/distance (f/d)– Two-dimensional Force measurement
• AC mode “force” measurement– Amplitude/distance (a/d)– Phase/distance (p/d)– Tapping mode imaging and a-p/d
• Other force-related afm techniques– Force-modulation imaging– Lateral-force (friction) imaging– Lateral resonance (AC mode lateral force)
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Force-modulation imaging
ForceModulation.swf
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FM-AFM images of a two-phase block copolymer
900nm scansHeight Force Modulation
Veeco Instrumentswww.veeco.com
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Lateral-Force AFM
LateralForce.swf
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Lateral-Force AFM
Height Lateral Force
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Lateral resonance (LR) AFM
HOPG surface imaged with interleaved TappingMode height (left) and TRmode phase (right). 3µm scan. (Supplied by Veeco.)
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Acknowledgements
Funding: BBSRC, EPSRC, RSPGB, GSK, Pfizer Global R&D, Nektar,
Molecular Profiles.
• Dr Ardeshir Danesh,• Dr Giles Sanders, Dr
Jianxin Zhang, Dr Wenke Zhang
• Prof Martyn Davies, Prof Saul Tendler, Prof Clive Roberts, Dr Phil Williams, Dr Steph Allen
• NT-MDT http://www.ntmdt.ru/
王宽诚教育基金会