\subfloat[][]{\asyinclude{figures/expt-sawtooth/expt-sawtooth}%
\label{fig:expt-sawtooth}}
% Possibly use carrion-vazquez00 figure 2 to show scale of afm tip
- \caption{(a) Schematic of the experimental setup for mechanical
- unfolding of proteins using an AFM (not to scale). An experiment
- starts with the tip in contact with the substrate surface, which
- is then moved away from the tip at a constant speed. $x_t$ is the
- distance traveled by the substrate, $x_c$ is the cantilever
- deflection, $x_u$ is the extension of the unfolded polymer, and
- $x_f=x_{f1}+x_{f2}$ is the extension of the folded polymer. (b)
- An experimental force curve from stretching a ubiquitin polymer
- with the rising parts of the peaks fitted to the WLC\index{WLC}
- model (\cref{sec:tension:wlc})\citep{chyan04}. The pulling speed
+ \caption{\subref{fig:unfolding-schematic} Schematic of the
+ experimental setup for mechanical unfolding of proteins using an
+ AFM (not to scale). An experiment starts with the tip in contact
+ with the substrate surface, which is then moved away from the tip
+ at a constant speed. $x_t$ is the distance traveled by the
+ substrate, $x_c$ is the cantilever deflection, $x_u$ is the
+ extension of the unfolded polymer, and $x_f=x_{f1}+x_{f2}$ is the
+ extension of the folded polymer. \subref{fig:expt-sawtooth} An
+ experimental force curve from stretching a ubiquitin polymer with
+ the rising parts of the peaks fitted to the WLC\index{WLC} model
+ (\cref{sec:sawsim:tension:wlc})\citep{chyan04}. The pulling speed
used was $1\U{$\mu$m/s}$. The irregular features at the beginning
of the curve are due to nonspecific interactions between the tip
and the substrate surface, and the last high force peak is caused