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Reflecting cantilever beam optical modulator

The electrostatic deflection of a cantilever beam has been derived by Petersen [2] and Kovacs [3]. The deflection of a cantilever beam of width w and length I due to a point load F acting on the end of a beam was found to be [Pg.74]

If we consider a normalized point force q x) = F(x)IA acting on a small segment of the cantilever beam wdx at the position x. [Pg.75]

For an electrostatic force on the cantilever with an initial gap d(, the force would be [Pg.75]

The total tip deflection can be found from integrating the incremental deflection along the length of the cantilever beam  [Pg.76]

To solve this equation in closed form, Kovacs made a parabolic approximation for the gap d x) as a function of the tip deflection y t)  [Pg.76]


See other pages where Reflecting cantilever beam optical modulator is mentioned: [Pg.74]    [Pg.75]    [Pg.74]    [Pg.75]    [Pg.317]    [Pg.58]    [Pg.693]   


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Optical beams

Optical modulation

Optical modulator

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Optics reflective

Reflected beam

Reflection optics

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