After substitution of (1, and using the notation with parameter we obtain dç, Ç1 —f—+ v — dp p p=1

9.2 Thin Lens Elastically Bent by Uniform Load and, from (9.39c), the integration constant is

E p + 3n nn ß + (m + 3)(m - 1) + n=2 n + 1 ü, m2 5

Finally from (9.22c), we determine the flexure z = aj 2dp. Setting the integration constant equal to zero, i.e. choosing the origin of the flexure at the center of the lens, the flexure is represented by (Lemaitre [10])

0 0

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