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input terminals. High input impedance is desirable, since the device will then draw less current from the
                                 source. Oscilloscopes and data acquisition equipment frequently have input impedances of 1 MΩ  or
                                 more to minimize this current draw. Output impedance is a measure of a sensor’s (or signal conditioning
                                 circuit’s) ability to provide current for the next stage of the system. Output impedance is frequently
                                 modeled as a resistor in series with the sensor output. Low output impedance is desirable, but is often
                                 not available directly from a sensor. Piezoelectric sensors in particular have high output impedances and
                                 cannot source much current (typically micro-amps or less). Op-amp circuits are frequently used to buffer
                                 sensor outputs for this reason. Op-amp circuits (especially voltage followers) provide nearly ideal cir-
                                 cumstances for many sensors, since they have high input impedance but can substantially lower output
                                 impedance.

                                 18.8 Nonlinearities

                                 Linear systems have the property of superposition. If the response of the system to input A is output A,
                                 and the response to input B is output B, then the response to input C (= input A + input B) will be
                                 output C ( = output A + output B). Many real systems will exhibit linear or nearly linear behavior over
                                 some range of operation. Therefore, linear system analysis is correct, at least over these portions of a
                                 system’s operating envelope. Unfortunately, most real systems have nonlinearities that cause them to
                                 operate outside of this linear region, and many common assumptions about system behavior, such as
                                 superposition, no longer apply. Several nonlinearities commonly found in mechatronic systems include
                                 static and coulomb friction, eccentricity, backlash (or hysteresis), saturation, and deadband.

                                 18.9 Static and Coulomb Friction

                                 In classic linear system analysis, friction forces are assumed to be proportional to velocity, i.e., viscous
                                 friction. With an actuator velocity of zero, there should be no friction. In reality, a small amount of static
                                 (no velocity) or Coulomb friction is almost always present, even in roller or ball type anti-friction
                                 bearings. A typical plot of friction force vs. velocity is given in Fig. 18.6. Note that the static friction force
                                 can assume any value between some upper and lower limit at zero velocity. Static friction has two primary
                                 effects on mechatronic systems:

                                    1. Some of the actuator torque or force is wasted overcoming friction forces, which leads to ineffi-
                                       ciency from an energy viewpoint.
                                    2. As the actuator moves the system to its final location, the velocity approaches zero and the actuator
                                       force/torque will approach a value that exactly balances frictional and gravity loads. Since static
                                       friction can assume any value at zero velocity, the actuator will come to slightly different final
                                       resting positions each time—depending on the final value of static friction. This effect contributes
                                       to some loss of repeatability in mechatronic systems.















                                 FIGURE 18.6  Static and Coulomb friction.



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