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Validity was tested by "Principal Component Analysis", non-rotated method and "Varimax with Kaiser Normalization" with rotation (factor analysis) based on the subscales.
For FFT, h(l) is the rotation factor.
Approximate solutions for the root rotation factor, based on the engineers' theory of bending, are compared with finite element results to establish a reliable simple method of the estimation of the root rotation factor.
In this work, we consider a vertical translation factor, a horizontal translation factor, a rotation factor, and a scaling factor.
The researchers just need to add other rotation factor in Eq. 11 to describe the change of yaw angle.
A rotation factor rg of approximately 2 was obtained which is also independent of the specimen thickness.
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Depending on the relationship between (left{ R right}), {M} and (left{ C right}), we can know the two rotation factors.
In order to calculate C P from R P, we need a transition coordinate system ({ M}), and two rotation factors (_{M}^{C} R) and (_{R}^{M} R).
After the rotation, factors with an eigenvalue greater than 1 were retained.
In orthogonal rotation, factors do not correlate with each other: (5) G = L T T T L T + F = L L T + F, where T is an orthogonal transformation matrix.
Varimax rotation gave higher factor loading as compared to un-rotated factor method (factor loading ranged from 0.50 to 0.94).
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