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The east and north tilt components can then be substituted into Eqs. 6.77 and 6.76 to obtain the equation for position error due to tilts. Schuler oscillations (Sections 2.2.2.3 and 6.5.2.1) are excited when these position errors, in turn, cause tilts. 6.5.3.3 Carouseling and Gimbal Flipping These methods are commonly used for mitigating the effects of sensor compensation errors in gimbaled systems. The ability to rotate a gimbaled inertial platform was soon exploited as a means of averaging out the effects of many types of sensor errors on navigational accuracy. The simplest schemes rotate the platform containing the sensors about the local vertical with a rotation period signi cantly shorter than the Schuler period of 84 min (carouseling) or in discrete 90 or 180 steps (gimbal ipping). The effects of many platform- xed sensor errors (e.g., accelerometer and gyroscope biases and input axis misalignments) can be effectively cancelled by such rotations. Problems 6.1 In the one-dimensional Line Land world of Section 6.4.1.1, an INS requires no gyroscopes. How many gyroscopes would be required for two-dimensional navigation in Flat Land Derive the equivalent formulas in terms of Y (yaw angle), P (pitch angle), and R (roll angle) for unit vectors 1R ; 1P ; 1Y in NED coordinates and 1N ; 1E ; 1D in RPY coordinates, corresponding to Eqs. C.86 C.91 of Appendix C. Explain why accelerometers cannot sense gravitational accelerations. Calculate the numbers of computer multiplies and adds required for (a) gyroscope scale factor=misalignment compensation (Eq. 6.23), (b) accelerometer scale factor=misalignment compensation (Eq. 6.28), and (c) transformation of accelerations to navigation coordinates (Fig. 6.13) using quaternion rotations (Eq. C.243) requiring two quaternion products (Eq. C.234). If the INS performs these 100 times per second, how many operations per second will be required crystal reports pdf 417 7 Adding PDF417 Symbols to Crystal Reports - PDF417 Fontware ...
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