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Etudes sur le mécanisme de remodelage des nucléosomes par ...

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tel-00413908, version 1 - 7 Sep 2009<br />

However, the final reaction volumes in this experiment were adjusted to 10 μl to be<br />

convenient for loading the samp<strong>le</strong>s on gel. After stopping the reaction with apyrase, reaction<br />

products were resolved on 5% native polyacrylami<strong>de</strong> gel. To ascertain the migration of<br />

unmobilized and mobilized species, a replicate of the experimental set containing 32 P- labe<strong>le</strong>d<br />

601-255 bp nuc<strong>le</strong>osomes was done and run on the same gel. Nuc<strong>le</strong>somes were eluted from<br />

excised bands, corresponding to control, remo<strong>de</strong><strong>le</strong>d and sli<strong>de</strong>d species, as <strong>de</strong>scribed before.<br />

Eluted nuc<strong>le</strong>osomes were filtered through glass fibre filter, prior to samp<strong>le</strong> pre<strong>par</strong>ation for<br />

AFM analysis.<br />

II.5.8 Atomic Force Microscopy, Image Analysis and construction of the 2D maps Lc/�L<br />

For the AFM imaging, the nuc<strong>le</strong>osomes were immobilized onto APTES-mica <strong>sur</strong>faces as<br />

<strong>de</strong>scribed previously (Montel et al., 2007). To automatically analyze AFM images, we have<br />

written a Matlab © (The Mathworks, Natick, MA) script based on morphological tools. Using<br />

this script we are ab<strong>le</strong> to isolate sing<strong>le</strong> mono-nuc<strong>le</strong>osomes from other objects present on the<br />

image (<strong>sur</strong>face roughness, naked DNA, two connected nuc<strong>le</strong>osomes).<br />

In or<strong>de</strong>r to remove the piezoe<strong>le</strong>ctric scanner thermal drift, flatten of the image is performed.<br />

The use of a height criteria (h>0.5nm where h is the height of the object) allows to avoid the<br />

shadow artifact induced by high objects on the image. Then we se<strong>le</strong>ct nuc<strong>le</strong>osomes based on<br />

area criteria and height thresholding. Using a hysteresis height thresholding, we verify the<br />

presence of an NCP on each se<strong>le</strong>cted objects. For each mono-nuc<strong>le</strong>osome, the NCP center of<br />

mass is localized and an Euclidian distance map can be calculated from this origin. After<br />

exclusion of the NCP <strong>par</strong>t, the ske<strong>le</strong>tons of the free arm regions are obtained by thinning. By<br />

applying the previous distance map, the <strong>le</strong>ngth of each arm is mea<strong>sur</strong>ed from the NCP<br />

centroid. The longest arm is named L + and the shortest L -. DNA comp<strong>le</strong>xed <strong>le</strong>ngth is <strong>de</strong>duced<br />

by Lc = Ltot - L- - L+ where L tot is 255 bp in this case. The position of the nuc<strong>le</strong>osome<br />

relatively to the DNA template center is calculated as ∆L = (L+ - L-)/2. It is important to<br />

notice that the position <strong>de</strong>fined in this way corresponds to the location of the most <strong>de</strong>eply<br />

buried base pair, which might differ from dyad axis position (strictly <strong>de</strong>fined for symmetric<br />

nuc<strong>le</strong>osomes).<br />

110

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