Conventional wide-field (deconvolution) image stacks were generated from 3D-SIM raw data by average projection of five consecutive phase-shifted images from each plane (only of the first angle) and, in case, subjected it to an iterative 3D deconvolution using softWoRx 6.0.
Furthermore, the first arm is able to rotate from 0° to 90°, where the second angle varies between 0° and 180°, as Fig. 10 explains this matter of fact.
When the second blade angle is 26°, the static pressure also increases with the increase of the first blade angle from 40° to 43°.
Consistent with results from the first experiment, the angle of the peak displacement during probe trials varied with hammer orientation and was close to the direction predicted by the dynamics.
Figure 6, bottom, shows the evolution of the estimated mean sarcomere length, accompanied with two sarcomere length estimates from correcting the ROI orientation with two methods: 1) using the time-dependent optimal ROI angle and 2) using fixed optimal ROI angle from the first microscopy image.
With the increase of the second blade angle from 24° to 26° in Fig. 5b, the shaft power of the second motor also increases.
Finally, we obtain a new value of the estimated central angle from the first estimated central moment (widehat {M}_{1k}(widehat {bar {theta }}_{k})).
Draw a second, gentler curve from there and join it to the first with a second straight line on a small angle from the first.
Each membrane is composed of 6 layers with strand angles from the first layer to the last layer of 45, 135, 0, 90, 0 and 90°.
Three parameters were collected as illustrated in Figure 1 including twisting length and twisting angles from the first, second, third and fourth quarters.
It can be seen that when the first blade angle increases from 40° to 43° in Fig. 6a, the shaft power of the first motor increases.
