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CSDC - Università di Firenze
The Florence EMBIO group:
people and scientific activity
Lapo Casetti
Dipartimento di Fisica and CSDC, Università di Firenze
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CSDC - Università di Firenze
CSDC
Center for the Study of Complex Dynamics
The CSDC is our “home”
It is an inter-departmental structure of our University which
hosts also researchers from the CNR (National Research
Council) and from other research structures
Graduate school on Nonlinear dynamics and complex systems:
one graduate student funded by EMBIO starting January, 2006
All EMBIO researchers in Florence are part of CSDC
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People
theory
experiment
Physics Department
Dr. Lorenzo Bongini
Dr. Lapo Casetti
Dr. Carlo Guardiani
Prof. Roberto Livi
Lorenzo Mazzoni
EMBIO researcher
Physics Department
Dr. Francesca Sbrana
EMBIO graduate student
EMBIO postdoc
Energetics Department
Dr. Franco Bagnoli
ISC - CNR
Dr. Bruno Tiribilli
Dr. Massimo Vassalli
ISC - CNR
Dr. Antonio Politi
Dr. Alessandro Torcini
INAF
Dr. Marco Pettini
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Call for applications!
The call for applications for the EMBIO research position in
the Florence group is being opened: look at www.unifi.it/bu
The position is a research-only, fixed-term one (2 ½ years)
starting April 1, 2006. Net salary is around 1500-1600 euros
per month
We are looking for a young but experienced researcher able to
contribute with original ideas and to take a leading role in the
theoretical side of the project
We welcome applications from EMBIO partners
The deadline is tight (August 20 or so) due to Italian
rules, so hurry up!
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Outline
theory
experiment
Simple models of proteins
BPN models
Dynamical simulations
Atomic Force Microscopy
How it works
Pulling proteins
Energy landscape
Geometric and topological
properties
Dynamics on the
“connectivity graph”
Modeling
Simple statistical models
Reconstructing the (free)
energy landscape
Dr. Lorenzo Bongini
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Atomic Force Microscopy
An Atomic Force Microscope acts
on the sample as a
dynamometer able to probe the
local interactions between tip
and sample.
If no specific interaction occurs
between tip and sample, the
system senses the geometry of
the potential barrier defining the
sample: the topography.
The probe is a micrometric
cantilever, made by photolitographic methods, with a
sharp tip on the bottom. In the
interaction potential with the
sample, the cantilever behaves
like an elastic spring with k
ranging from 0.01 to 100 N/m
By performing a scanning, the
system spans the XY plane and
the information collected can be
imaged as a 2D map of the
interaction.
With standard cantilevers one
obtains a topographic map of the
surface (Microscopy) wherever
using functionalised tips is
possible to obtain specific maps
such as magnetic, electric or
affinity ones (Spectroscopy)
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Protein stretching
x
F  d
Z  Z 0  vt
F  20 pN  20nN

v  10 nm s 100 m s
k  0.01 N m  100 N m
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
CSDC - Università di Firenze
Typical AFM stretching patterns
Force
Displacement Z
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Experimental protocol
Adsorption link
The system studied
behaves like a series of
three springs. We have
to choose the spring
elastic constants
accordingly to what we
are interested in
 C P
P
I29
T4 or T8 fragment
I28
 P S
Au
I30
I27
Cys-Cys amino acids create
a polar link with the gold
substrate
Cys Cys
 P   C  P ;  PS
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Sawtooth pattern
Oberhauser et al., PNAS 98, p.468-472 (2001)
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Modeling sawtooth patterns
Force
Displacement Z
The unfolding pattern is modeled like
a polymer extension between two
successive rupture events.
The speed typically used allows to
trait this region as in equilibrium. No
information about folding is found by
this approach; only mechanical
parameters can be computed
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Polymer extension
ERT
Exponential rising of
Tension
FJC
Freely-jointed chain
WLC
Worm-like chain
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200 pN
WLC model
50 nm
Worm Like Chain
Model
k T
F B
Lp

1
1 Z 
  

2
 41  Z LC  4 LC 
Lp persistence length, LC contour length
Z displacement, T temperature
L p  0.39  0.07nm
LC  28.4  0.3nm
L
  C  73
Lp
Li et al., Nature 418, p.998 (2002)
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A unified approach
Our aim is to find a simple model
allowing a complete statistical
description of the stretching experiment
(not only polymer extension)
Franco Bagnoli,
Carlo Guardiani
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The model: schematic view
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The model: basic features
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Energy: harmonic term
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Energy: interaction term
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A typical plot
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Beyond our toy model
• Development of a more realistic protein
model:
• Three-dimensional model
• Modelling of interactions between
monomers
• Study of the role of the mass of the
cantilever and protein
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Free energy reconstruction
z
wi z, r    F z ' , r dz '
0
N
f
r
i
0
Reaction coordinate
z
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z’
CSDC - Università di Firenze
Free energy reconstruction:
Jarzinski equality
e
 G
 e
 wi
N
JE allows to reconstruct the
free energy landscape by
averaging over a set of nonequilibrium measurements
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