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As debonding progresses the angle becomes smaller and thus has less effect.
Obviously, when the angle becomes 0° or 180°, limb force vectors are collinear, and the end effector loses the force output capacity along the direction perpendicular to limb force vectors.
When the angle becomes large, the stress shared by the middle and posterior columns of the spine increases, the interspinous distance may be reduced significantly, and pseudarthrosis formation may occur in some patients (which suggests increased stress in the spinous process).
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However, the lower angle peak became smaller and broader, and the angle became higher.
After the initial contact and a small degree of bending, the angle became ~84° and then ~79°, indicating the interlayer sliding rather than bending as a whole plate (Fig. 3a,b).
Plamondon and Roy presented step-to-step changes in trunk angle during the acceleration phase and found that the angle became stable from the 14th step (Plamondon and Roy, 1984), which is in line with the results of our study.
During the downstroke the angles are positive, while after mid-upstroke, the angles become negative for all speeds.
Before the reference value, the channel height has the greatest influence on the module bottom surface temperature, whereas after the reference value, the corner angle becomes the largest influence factor.
The amplitude minimum on the dip equator is also seen in Figure 6.Figure 7 shows that as the dip angle becomes smaller, the averaged period of the spectral peak becomes longer.
However, when the structure is tilted, the relationship between the detachment force and the pulling angle becomes asymmetric.
As the incidence angle becomes larger, the channel width become narrower, however the light tunneling channel number is unchanged.
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