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Oscillations, Waves, and Interactions - GWDG

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DPI60plus – a future with biophysics 443<br />

Figure 5. Height distribution of MTs. Undecorated MTs show an average diameter of<br />

25.9 nm at a loading force of < 0.1 nN. When MTs are preincubated with tau the height<br />

increased by 2.2 nm. Kinesin added 4.5 nm to the MT height. Note that the 2.2 nm are caused<br />

by tau binding all around MTs while kinesin is bound to MTs just on one side because<br />

in this case MTs were attached to the surface before addition of kinesin. The differences<br />

between the three distributions were tested for statistical significance by a Student’s t-test.<br />

The probability that any pair of the measured distributions belong to the same parent<br />

distribution was estimated to be smaller than 0.1 % by applying the Student’s t-test for<br />

samples with an unequal variance. (From Ref. [1]).<br />

Figure 6. Calculated dependence of F/E on CCMV-capsid deformation for R = 14.3 nm,<br />

h = 3.8 nm, <strong>and</strong> s = 0.4. The images above the curve show a one-quarter segment of the<br />

capsid at indentations d = 0, 5.6, <strong>and</strong> 14 nm, <strong>and</strong> the von Mises stress is indicated by the<br />

colour. The image below the curve shows the buckling of the capsid away from the tip that<br />

is mirrored by a decrease in the slope. (From Ref. [5]).

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