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Report - PEER - University of California, Berkeley

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measurements, to the modeling <strong>of</strong> the compressibility <strong>of</strong> fluid, to the nonlinearities <strong>of</strong>the servo control system (servo valves) and other stiffness. The authors developedtwo approaches for dynamic force control:The first approach is using the convolution method with a compensationtechnique that is based on identification <strong>of</strong> thefrequency response function (FRF) <strong>of</strong> the systemand modifying the force input by the inverse <strong>of</strong> theFRF. The operation is done in the time domain byevaluating the convolution integral. The forces arecalculated based on Equation 6 with α 1 (s) =1 andα 3 (s)=0. Without the compensation theimplementation is not feasible. The system wastested for free vibrations, and base motion–whitenoise and earthquakes. The performance for thewhite noise <strong>of</strong> the 2-d<strong>of</strong> and the 1-d<strong>of</strong> hybrid set-up is shown in Figure 5. The hybridsystem simulates the 2-d<strong>of</strong> over the entire frequency range except for the very lowfrequencies with errors <strong>of</strong> up to 5%.The second approach is based on control characteristics <strong>of</strong> hydraulic actuators. Ahydraulic actuator is a rate-type device or velocity source; however, hydraulicactuators are typically designed for good position control. In contrast for forcecontrol, a force source is required. Thus force control using hydraulic actuators is aninherently difficult problem. Actuators designed for position control have stiff oilcolumns, making force control very sensitive to control parameters and <strong>of</strong>ten leadingto instabilities. Moreover friction, stick-slip, breakaway forces on seals, backlash etc.cause force noise, making force a difficult variable to control.Motivated by these observations and by the fact that causality requires a flexiblecomponent in order to apply a force in the force control scheme described here, aspring is introduced between the actuator and the structure as shown in Figure 6.Notice that the scheme (1) intentionally introduced series spring, K LC , which assumesthe role <strong>of</strong> the oil spring and (2) there is no force feedback loop.TargetForce1 / KLCFigure 5. Pilot test forwhite noise.MeasuredForceCommandSignalActuator withDisplacement ControlLoadCellSeriesSpring, KLCStructureCompensatorFigure 6. Proposed force control scheme.The actuator behaves as a displacement device. Hence the actuator in the controlscheme <strong>of</strong> Figure 6 is operated in closed-loop displacement control with a PIDF265

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