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8.3   Properties of ER Fluid in Flow Mode                       137

               14
                     +   2 lin/min
                         4 lit/min
              12     #   12 lit/min
                         16 lit/min
                                                                       +
              10                                          +
             "ER Pressure (bar)"  8 6  +       +






               4             +


               2

               0
                 0      2       4      6       8      10     12      14     16
                                          Current (mamp)
            Fig. 8.11   Steady state pressure drops at different supplied current



            in the electronics. For fast response requirement applications, the power supply
            must be able to generate large voltage with little time delay.
              Another important property of ER fluid in flow mode is the steady state pressure
            drop across the valve at various current. This is shown in Fig. 8.11.
              The above diagram shows that there is approximately a linear relationship be-
            tween the current and the pressure drop across the valve at steady state. The flow
            rate has little influence on these phenomena. It would be interesting to investigate
            the transient behavior when a current is applied across the valve. This is shown in
            Fig. 8.12.
              It can be seen that there are two distinct phenomena in the transient response.
            One is a first order lag type which increases exponentially and the other one is the
            response of a second order transfer function. When the transfer functions cascaded
            together produces this kind of response.
              The above analysis shows that there is a transfer function between the current
            and input voltage and there is another transfer function between the pressure drop
            and the current. The transfer function between pressure drop and current can be
            obtained with assumption that the current response is much faster than the pressure.
            This approximation can be made because the current response is very fast and in
            Fig. 8.12, it can be assumed that it is pressure response to the applied current.
              From Fig. 8.8, the transfer function between current and voltage can be obtained
            as
                                          ( RCs +1 )
                                       I :=       v                       (8.1)
                                             R
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