ACTIVE PANTOGRAPH CONTROL ACTIVE CONTROL OF HIGH-SPEED RAILWAY VEHICLE PANTOGRAPH CONSIDERING VERTICAL BODY VIBRATION.

International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 268

IV. ACTIVE PANTOGRAPH CONTROL

With the intension to minimize the vibration, the vibration cancellation control is applied. Based on transfer function TF, the controller is designed to produce displacement which is equal but opposite to the one that is produced by the pantograph due to the vertical vibration. The torque occurs at the lower frame caused by main spring k 3 and damper c 3 installed in the framework which produces the upward force. The damper in the actual design pulls the brake for the framework when the pantograph descends to a certain point. The control force f C is applied to the lower frame, 2 f c l f = τ 3 Where l f 2 is the length of the lower pantograph frame, which is equal to 1 m. The pantograph is controlled using vibration cancellation VC Fig. 4. In this control scheme, the controller uses the vibration as the input and feeds to the actuator. The actuator then produces the same magnitude of vibration at different direction to cancel the vibration itself. Fig. 5 shows the transfer function block diagram of the controller design with controller Ks, the pantograph G 1 s and actuator G 2 s. The vibration cancellation control force is denoted as f cVC . FIGURE 4: Block diagram for vibration cancellation control FIGURE 5: Block diagram of VC with transfer function The equations of motion for the pantograph system are shown in Eqn. 4, 5 and 6. 1 2 1 1 2 1 1 1 1 f p y p y T k p y p y T c p y T m = − + − + 4 2 1 1 2 1 1 3 2 2 3 2 2 2 2 p p T p p T p p p p p y y k y y c y y k y y c y m − + − = − + − + 5 International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 269 c p p p p p f y y k y k y c y m + − = + + 3 2 2 3 3 3 3 3 3 6 The above equations can be simplified using transfer function for block analysis and controller design. By neglecting the f 1 and assuming f c = 0, the transfer function for input y B and output y p 1 is, s Y s Y s G B p 1 1 = 7 The detail transfer function of G 1 s is, 8 And, assuming y B = 0, the transfer function for input f c and output y p 1 is, s F s Y s G C p 1 2 = 9 The detail transfer function of G 2 s is, 10 The numerator and denominator constants of G 1 s and G 2 s are summarized in Table 3. With the intention of zeroing the total displacement y p 1 , the controller Ks is derived by, - 11 s G s G s K 2 1 = 12 The detail TF of Ks is, 13 The numerator and denominator constants of controller Ks are summarized in Table 4. International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 270 TABLE 3: Numerators and denominators for G 1 s and G 2 s Constant Value Constant Value N 4G1 5.76 x10 8 N 3G2 2.88 x10 6 N 3G1 4.61 x10 11 N 2G2 1.87 x10 9 N 2G1 1.35 x10 14 N 1G2 2.96 x10 11 N 1G1 1.73 x10 16 N 0G2 2.70 x10 13 N 0G1 8.10 x10 17 D 7G2 7.34x10 4 D 7G1 7.34x10 4 D 6G2 2.52 x10 7 D 6G1 2.52 x10 7 D 5G2 3.12 x10 9 D 5G1 3.12 x10 9 D 4G2 4.10 x10 11 D 4G1 4.10 x10 11 D 3G2 2.01 x10 13 D 3G1 2.01 x10 13 D 2G2 1.44 x10 15 D 2G1 1.44 x10 15 D 1G2 1.73 x10 16 D 1G1 1.73 x10 16 D 0G2 8.10 x10 17 D 0G1 8.10 x10 17 TABLE 4: Numerators and denominators for Ks Constant Value Constant Value N 11K -4.23 x10 13 D 12K 2.12 x10 11 N 10K -4.83 x10 16 D 11K 6.33 x10 14 N 9K -2.34 x10 19 D 10K 7.17 x10 10 N 8K -6.35 x10 21 D 9K 4.00 x10 20 N 7K -1.12 x10 24 D 8K 1.26 x10 23 N 6K -1.40 x10 26 D 7K 2.48 x10 25 N 5K -1.30 x10 28 D 6K 3.34 x10 27 N 4K -8.83 x10 29 D 5K 3.33 x10 29 N 3K -4.39 x10 31 D 4K 2.41 x10 31 N 2K -1.58 x10 2 D 3K 1.24 x10 33 N 1K -2.80 x10 34 D 2K 4.89 x10 34 N 0K -6.56 x10 35 D 1K 8.31 x10 35 D 0K 2.19 x10 37 V. RESULTS AND DISCUSSIONS Table 5 summarizes the force abbreviations. Fig. 6 to 8 show the graphical results of the dynamic analysis at speed of 300, 350 and 400 kmh. In the VC control approach, the control force is applied in order to minimize the effect of vertical vibration. The VC control system has consistently reduced the CF and CL for all speeds Fig. 9 and 10. International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 271 TABLE 5: Contact forces abbreviations Abbreviations Description f 1V Contact force of system with vibration but without control f 1VC Contact force of system with vibration and vibration cancellation control f 1N Nominal contact force of 54 N FIGURE 6: Contact forces at v = 300kmh FIGURE 7: Contact forces at v = 350kmh 20 40 60 80 100 20 40 60 80 100 F o rc e N Contact force Distance m f 1V f 1VC f 1N 20 40 60 80 100 20 40 60 80 100 120 140 160 180 F o rc e N Contact force Distance m f 1V f 1VC f 1N International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 272 FIGURE 8: Contact forces at v = 400kmh FIGURE 9: Contact force controls evaluation FIGURE 10: Contact loss ratio 20 40 60 80 100 -20 20 40 60 80 100 120 140 F o rc e N Contact force Distance m f 1V f 1VC f 1N 100 150 200 250 300 350 400 500 1000 1500 2000 2500 C o s t fu n c ti o n N Running velocity kmh Without control With VC 100 150 200 250 300 350 400 1 2 3 4 5 6 7 8 C o n ta c t lo s s Running velocity kmh Without control With VC International Journal of Mechanical Engineering and Technology IJMET, ISSN 0976 – 6340Print, ISSN 0976 – 6359Online Volume 4, Issue 6, November - December 2013 © IAEME 273

VI. CONLCUSION