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Differences in stress distributions due to an applied load moving along the long axis and the short axis of contact ellipse are discussed.
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Fig. 5 Percentage of time occupancy (y axis) of contacts at 3.5 Å between each asODN nucleotide (x axis) considering phosphate (PO), sugar, and base groups and a PAMAM-NH2 and b PAMAM-OH terminal groups (–NH2 and –OH, respectively).
One hundred percent represents the total number of frames of the last 10 ns of MD trajectory Fig. 6 a Summary of the percentage of time occupancy (y axis) of contacts at 3.5 Å between each type of nucleotide base (x axis) considering phosphate (PO), sugar, and base groups and PAMAM-NH2.
Due to this difference, the direction of the tangential force around the rotation axis of the contact plate is different, and the load applied to the ground at the time of executing the wiping motion is different.
Similarly, when local pressure was applied in a rod-shaped form (like the petri dish), a linear front is created that may stretch the cells in a direction perpendicular to the axis of the contact area.
On the selected cross-section, however, the half-space assumption does not hold since the smallest radius of rail curvature at the contact point is 13 mm, which is comparable to the largest semi-axis of the contact area.
It is generally believed that to guarantee acceptable accuracy in these half-space-based methods, the characteristic size (twice length of one semi-axis) of the contact patch should be much smaller than the significant dimensions (i.e. the height, width, length and the principal radii of curvature) of each body in contact.
With respect to the axis through the point of contact, the torque is equal to RFp, giving rise to an angular acceleration α given by Ipα = RFp, where Ip is the moment of inertia about the point-of-contact axis and can be determined by applying equation (80) relating moments of inertia about parallel axes (Ip = I + MR2).
Ten single-implant crowns were loaded with the use of a cyclic loading device with 100 N of force at 30° angles to the long-axis for 0.2 seconds of contact time with a frequency of 1 Hz.
The motion may be analyzed from the point of view of an axis passing through the point of contact between the rolling body and the plane.
Histone H1 is located at the dyad axis of the nucleosome, in contact with the entry and exit sites of the nucleosomal DNA, and is critical in organizing [3] and stabilizing maximal nucleosome compaction within the chromatin fibre [4], [5].
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