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Chapter 5 • Heat in Hydraulic Systems                                                         297

             lowing the system to cool. Figure 5-10 shows both rising and cooling tempera-
             ture profiles obtained from HyPneu for the pump, lines, orifice and tank. The
             results indicate the average steady state temperature is around 190°F which
             agrees with the theoretical calculation.




                               Figure 5-10. Heating and Cooling Temperature Profiles of
                                            Pump, Orifice, Lines, and Tank.




5.7          Thermal Duty Cycle Analysis

             M      any times, a hydraulic machine is expected to carry out a series of loading
                    applications over a prescribed distance or period of time in a recurring
             manner. In other words, the machine is commanded to follow a specific work
             cycle that defines the intended job function to a given application task. The ma-
             chine and its components will naturally response to the imposed work cycle and
             reflect a corresponding duty cycle. Speaking differently, a work cycle represents
             the stressing severity while a duty cycle is the resultant strain pattern. In thermal
             analysis, the stressing parameters are heat generation or removing sources,
             whereas the temperature is the strain parameter. A knowledge of the thermal duty
             cycle is essential in heat control for any hydraulic system.
                    To illustrate the thermal duty cycle analysis procedures, let’s first consider
             the lumped model approach previously described in the Thermal Steady State
             Analysis section. Assume that the work cycle is divided into n operating intervals
             as shown in Fig. 5-11. Each operating interval has a time elapse of ritp with a heat
             load of hi. Parameter ri is the time ratio of the time elapse at the ith operating in-
             terval to the work cycle period, tp. This is a typical periodic step function. The
             profile functions that define the maximum (upper) and minimum (lower) steady
             state boundary of a first order differential system responses to a periodic step
             input can be analytically derived. The detail of the derivation can be found in the
             companion Hydraulic System Control and Optimization book in the Computer-
             ized Fluid Power Series.




           Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.
298                                                  Hydraulic System Design for Service Assurance




                          Figure 5-11. Periodic Step Function Work Cycle.


              However, without getting involved with cumbersome analytical proce-
       dures, we can obtain a duty cycle (output) from a given work cycle (input) as
       depicted in Fig. 5-12 by the following reasoning. Consider a first order system
       with a time constant τ and assume that at time t = 0 both input and output are
       null. Right after this point, namely at t = 0+,the input jumps to a new amplitude
       U1. Dynamically the output follows an exponential decay curve with the time
       constant τ to “catch” the input. At t = t2, the input jumps to the other new ampli-
       tude U2. At this moment, the output will immediately change its direction toward
       the new equilibrium value even the output has not reach the first equilibrium
       value. Note that, at time t2, the output takes the last value before input changed as
       the initial point and continues to chase the new equilibrium value exponentially.
       This “jump-and-chase” occurs whenever the input changes. Accordingly, the
       duty cycle travels between the upper and lower boundaries.




                          Figure 5-12. Response to a Step-Input Function.




      Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.
Chapter 5 • Heat in Hydraulic Systems                                                             299

                   It is much easier to investigate the duty cycle using computer approach.
             Figure 5-13 shows a hydraulic circuit has a 10 gpm pump driving a variable load.
             The load is 70% on the low value (around 278 psi), and 30% on the high value
             (around 1100) during one work cycle. The equivalent heat loads to the system are
             4126 Btu⋅hr-1 for 70% time and 16330 Btu⋅hr-1 for 30%, respectively. Figure 5-14
             shows the corresponding oil temperature duty cycle at pump outlet from HyPneu
             simulation. It clearly shows that, as expected, the oil temperature travels between
             an envelope confined by the upper and lower boundaries.




                                 Figure 5-13. HyPneu Circuit for Thermal Duty Cycle Analysis.



                                             2 00


                                             1 80
                          Temperature (°F)




                                             1 60


                                             1 40


                                             1 20


                                             1 00


                                              80
                                                    0   5 00      1 00 0        1 50 0   2 00 0
                                                               T im e (s ec )



                    Figure 5-14. HyPneu Simulation Results for Thermal Duty Cycle Analysis.




           Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.

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hydraulics useful

  • 1. Chapter 5 • Heat in Hydraulic Systems 297 lowing the system to cool. Figure 5-10 shows both rising and cooling tempera- ture profiles obtained from HyPneu for the pump, lines, orifice and tank. The results indicate the average steady state temperature is around 190°F which agrees with the theoretical calculation. Figure 5-10. Heating and Cooling Temperature Profiles of Pump, Orifice, Lines, and Tank. 5.7 Thermal Duty Cycle Analysis M any times, a hydraulic machine is expected to carry out a series of loading applications over a prescribed distance or period of time in a recurring manner. In other words, the machine is commanded to follow a specific work cycle that defines the intended job function to a given application task. The ma- chine and its components will naturally response to the imposed work cycle and reflect a corresponding duty cycle. Speaking differently, a work cycle represents the stressing severity while a duty cycle is the resultant strain pattern. In thermal analysis, the stressing parameters are heat generation or removing sources, whereas the temperature is the strain parameter. A knowledge of the thermal duty cycle is essential in heat control for any hydraulic system. To illustrate the thermal duty cycle analysis procedures, let’s first consider the lumped model approach previously described in the Thermal Steady State Analysis section. Assume that the work cycle is divided into n operating intervals as shown in Fig. 5-11. Each operating interval has a time elapse of ritp with a heat load of hi. Parameter ri is the time ratio of the time elapse at the ith operating in- terval to the work cycle period, tp. This is a typical periodic step function. The profile functions that define the maximum (upper) and minimum (lower) steady state boundary of a first order differential system responses to a periodic step input can be analytically derived. The detail of the derivation can be found in the companion Hydraulic System Control and Optimization book in the Computer- ized Fluid Power Series. Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.
  • 2. 298 Hydraulic System Design for Service Assurance Figure 5-11. Periodic Step Function Work Cycle. However, without getting involved with cumbersome analytical proce- dures, we can obtain a duty cycle (output) from a given work cycle (input) as depicted in Fig. 5-12 by the following reasoning. Consider a first order system with a time constant τ and assume that at time t = 0 both input and output are null. Right after this point, namely at t = 0+,the input jumps to a new amplitude U1. Dynamically the output follows an exponential decay curve with the time constant τ to “catch” the input. At t = t2, the input jumps to the other new ampli- tude U2. At this moment, the output will immediately change its direction toward the new equilibrium value even the output has not reach the first equilibrium value. Note that, at time t2, the output takes the last value before input changed as the initial point and continues to chase the new equilibrium value exponentially. This “jump-and-chase” occurs whenever the input changes. Accordingly, the duty cycle travels between the upper and lower boundaries. Figure 5-12. Response to a Step-Input Function. Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.
  • 3. Chapter 5 • Heat in Hydraulic Systems 299 It is much easier to investigate the duty cycle using computer approach. Figure 5-13 shows a hydraulic circuit has a 10 gpm pump driving a variable load. The load is 70% on the low value (around 278 psi), and 30% on the high value (around 1100) during one work cycle. The equivalent heat loads to the system are 4126 Btu⋅hr-1 for 70% time and 16330 Btu⋅hr-1 for 30%, respectively. Figure 5-14 shows the corresponding oil temperature duty cycle at pump outlet from HyPneu simulation. It clearly shows that, as expected, the oil temperature travels between an envelope confined by the upper and lower boundaries. Figure 5-13. HyPneu Circuit for Thermal Duty Cycle Analysis. 2 00 1 80 Temperature (°F) 1 60 1 40 1 20 1 00 80 0 5 00 1 00 0 1 50 0 2 00 0 T im e (s ec ) Figure 5-14. HyPneu Simulation Results for Thermal Duty Cycle Analysis. Copyright © 1999 by BarDyne, Inc. of Stillwater, Okalhoma. All Rights Reserved.