US 2010/0122385 A1). Of particular interest is the adhesion data which measures the forces arising from the forced dissociation of the RC-His12-LH1-PufX-cyt c 2-His6 complex upon the separation (retraction) of the AFM probe from the surface. Both the topography and the adhesion data were recorded simultaneously, thus imaging the surface distribution of the selleck inhibitor molecules while monitoring the interactions between the two proteins. A topography
image (Fig. 3a) was recorded at modulation frequency of 1 kHz, in imaging buffer (45 mM KCl, 10 mM HEPES pH 7.4) and under white light illumination with a power density of approximately 11 W m−2 (measured at the sample surface) in order to ensure the photo-oxidation of the RC-His12-LH1-PufX special pair and to favour binding of the reduced cyt c 2-His6 electron donor attached to the functionalised AFM probe. I-BET-762 Individual RC-His12-LH1-PufX complexes can be clearly seen on the gold substrate with an average height of around 7 nm and a lateral size (FWHM) in the range 16–20 nm (inset in Fig. 3a), consistent with the expected size (~12 nm) of the monomeric RC-His12-LH1-PufX complex and taking into account increased lateral dimensions due to geometrical tip convolution effects. PU-H71 mw Notably, some larger aggregates (of 2 or 3 core complexes) are also visible on the surface, indicated by the red arrows in Fig. 3a. Simultaneously with the topography, an adhesion
image was recorded (Fig. 3c), where we can easily identify the high adhesion (or high unbinding force) events, highlighted in red, resulting from forced dissociation of the cyt c 2-RC-His12-LH1-PufX complexes while they are still in a transient bound state. The total number of molecules on the surface in Fig. 3a is 209 and the total number of high unbinding force events in the corresponding adhesion image is 137, giving a binding frequency, under these experimental conditions, of approximately
66 %. In order to estimate the magnitude of the interaction forces between the two molecules, we measured the forces corresponding to each of the unbinding events in Fig. 3c, and the histogram of the interaction force distribution (inset in Fig. 3c) gave a mean value of 483.3 ± 9.8 pN (mean ± SE). The good correlation between the unbinding events and the position of the RC-His12-LH1-PufX http://www.selleck.co.jp/products/ch5424802.html molecules on the surface is highlighted in Fig. 3e by combining the topography and adhesion images in a 3D composite image, where the profile represents the sample topography and the colour coding indicates the strength of the interaction forces. The slight offset of the high unbinding force events from the centres of the RC-His12-LH1-PufX molecules is most likely result from interaction with cyt c 2-His6 molecules attached with an offset (not directly at the apex) to the AFM tip, together with a scan direction artefact during the image acquisition. Fig. 3 Functional AFM imaging of the interaction between RC-LH1-PufX and cyt c 2.