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                                                            ELECTROHYDRAULIC MOTION CONTROL SYSTEMS  479
                             Even though the commands to each valve do not change, the flow rate to each circuit, and
                             hence the speed of each cylinder, will vary due to the variation in the load in each circuit.
                                  If it is desired to modify circuit design so that the flow rate distribution between
                             circuits is independent of the load, the pressure drop across each valve must be same even
                             if the load pressures are different,
                                                          p − p = p − p l2                     (7.214)
                                                                   s
                                                           s
                                                               l1
                             Under this condition, flow rate distribution to each circuit is independent of the load
                             difference between the circuits and would be controlled by specific spool displacement of
                             each valve (x , x ). When both valves are same size and have the same displacement, flow
                                        v1
                                           v2
                             rate distribution would be equal, 50% each of total flow, or Q v1  = Q , Q = Q v1  + Q .
                                                                                         s
                                                                                     v2
                                                                                                   v2
                             When load pressures are different (p ≠ p ), the equal pressure drop across the valve for
                                                               l2
                                                           l1
                             each circuit can be accomplished by:
                                1. Adding restriction to the circuit which has the lower load so that the total hydraulic
                                  load seen by the valve is the same as the load on the other circuit. This means adding
                                  “positive hydraulic resistance” to the circuit with lower load.
                                2. Removing restriction from the circuit which has the higher load so that the total
                                  hydraulic load seen by the valve is same as the load on the other circuit. This means
                                  adding “negative hydraulic resistance” to the circuit with higher load.
                             The second option is not physically possible. Negative hydraulic resistance cannot be added
                             to a hydraulic circuit. Therefore, in order to equalize the effective hydraulic resistance
                             (making the total pressure drop equal in each circuit), we need to add hydraulic resistance
                             into the circuit which has lower load.
                                  The electrical analogy of this concept is shown in Figure 7.59a. Consider that we
                             have a constant voltage supply (analogy of pump), and two parallel resistors (analogy of
                             valve-cylinder of each circuit). The current (analogy of flow rate) is divided between the
                             two circuits as follows,
                                                              i = i + i 2                      (7.215)
                                                                 1
                                                                  V
                                                             i =                               (7.216)
                                                             1
                                                                 R v1
                                                                  V
                                                             i =                               (7.217)
                                                             2
                                                                 R
                                                                  v2
                                                 R
                                                  v1
                                               i 1
                                                 R
                                       i          v2
                             v                 i 2


                                                (a)

                                                R    R
                                                 v1   c1
                                             i 1
                                                R     R c2
                                      i          v2
                                                                    FIGURE 7.59: (a) Electrical analogy for a
                              v              i 2                    two function hydraulic circuit. (b) Same
                                                                    analogy with adjustable resistors in each
                                                                    path to control the current (flow rate)
                                                (b)                 distribution between the two parallel paths.
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