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Testing on the simulated united bone produced much smaller deflections as shown in Figs. 3 and 4, with a mean maximal deflection of 0.05 mm at both pretensions.
The experimental tooth was tipped starting from the zero position in 0.05° steps to a maximal deflection of ± 0.42° of the incisal edge in vestibular and palatal direction, after positioning the RTA onto the model.
The design is first formulated as an optimization problem to minimize the peak acceleration of a load while keeping the maximal deflection of the isolator within a specified physical limit.
Then, on the basis of the design sensitivity analysis, a heuristic optimization algorithm, called the evolutionary shift method, is presented for support position optimization to minimize the maximal deflection of a structure with a fixed grid mesh scheme.
The I V curves were extracted from the maximal deflection of the membrane potential following hyperpolarizing current injection and from the stable membrane potential level reached at the end of the pulse.
Maximal deflection of the accelerometer following a unilateral phrenic nerve electrical pulse was measured on the 6 7 intercostal space area of the rib cage, where the diaphragmatic fibres are directly apposed to its inner surface, thereby minimizing the distance between the accelerometer and the muscle.
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Second, the maximal deflections of wire and fishing line compare well with each other and with the theoretical curve for a frictionless, cylindrical beam (the experimental values are somewhat larger than the theoretical curve, presumably due to friction between the pin and the whisker).
Latency and amplitude of diaphragm compound muscle activity potentials (CMAP) were measured during tPNS; maximal deflections of Paw (ΔPaw), esophageal (ΔPes), and transdiaphragm (ΔPdi) pressures were measured during repetitive tPNS (40 Hz, 100 stimuli) and eOM.
First, maximal deflections for the tapered whiskers of cat and rat differ from each other by less than ∼10°, and are clearly distinguished from the untapered model whiskers.
The theory of elastic beams predicts that a plot of maximal deflection angle, scaled as shown in Fig. 2, should be independent of the whisker length, diameter, and Young's modulus, and depend only on the whisker taper and the amount of friction at the contact point (see File S1).
A non-linear behavior of maximal deflection with the applied pressure is predicted by the ANSYS simulation.
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