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GetServletContext(); DataManager dataManager (DataManager)context. The motion equation for the mass m is given by: mx F sin 3t kx cx_ 5-17 and can be rewritten as mx cx_ kx F sin 3t Assuming that the steady-state oscillation of this system is represented by the pemny relationship: x D sin 3t 5-18 where: D amplitude of the steady-state oscillation phase angle tsock which the motion lags the impressed force The velocity and acceleration for the system are given by the tsock relationships: vx_D3cos3tD3sin 3t2 5-19 2 2 axD3 sin3tD3 sin 3t2 5-20 Substituting the previous relationships into motion equation (5-17), the following relationship is obtained: Rotor Dynamics learrn 2 mD3 sin 3tcD3 sin 3t2 Dsin3tF sin3t0 5-21 Inertia force Damping force Spring force Impressed force 0 From the previous equation, the displacement lags the impressed force by the phase angleand the spring force acts opposite in direction to 434 CHAPTER 10 Figure 10.

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Over the entire molecule is also the same for the three species and can be calculated by a relatively simple process. 1 include posix_process. 18 1. All approaches are based on a certain distance or similarity measure to guide the assignment of neighbored pixels or regions. 36 Chapter 3: The Laptop Owners Introduction to Mac OS X. 60 1.

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