TMHP51 Servomechanisms (HT2012) Lecture 10 Signal Analysis Hydraulic System Evaluation Magnus Sethson [email protected] 1 1 “Real World” “Math & Physics” Analysis f 8 pL Ap Bp ẋp FL = Mt ẍp > > > < q = Ap ẋp + 41 Vet ṗL > q > > : q = Cq wxv 1 (Ps pL ) ⇢ Transformation t Synthesis “A Better World” [email protected] 2 2 f Frequency Domain Transformation f t f End-Value Theorem t f Loop Gain t f Fourier Transform t f Digital Filtering t f [email protected] Laplace Transform t Time Domain Inverse Fourier Transform t 3 3 Signal Analysis A Short Repetition [email protected] 4 4 Useful Transforms The Fourier Transform F (!) = Z 1 f (t) e i!t dt 1 The Laplace Transform F (s) = lim ✏!0+ [email protected] Z 1 f (t) e st dt ✏ 5 5 Sampling Theorem Source: Signaler och System, Anders Svärdström [email protected] 6 6 Nyquist Frequency & Filtering Source: Signaler och System, Anders Svärdström [email protected] 7 7 Ideal Signal vs. Sampled Signal [email protected] 8 8 Sampling Part of a Signal [email protected] 9 9 A Window Frame of a Signal [email protected] 10 10 Windows My Favorites Hanning Blackman Square [email protected] 11 11 Example [email protected] 12 12 Simulation model t f [email protected] 13 13 Model Disturbance Response −3 −8.2 x 10 −8.4 −8.6 −8.8 −9 −9.2 −9.4 −9.6 6 [email protected] 8 10 12 14 16 18 20 14 14 The “Real” Signal Response [email protected] 1 15 15 Windowed Signal and Removed Mean-Value −4 x 10 Output 5 0 −5 6 8 10 12 14 16 18 20 14 16 18 20 Time −4 Windowed Output x 10 2 1 0 −1 6 8 10 12 Time [email protected] 16 16 Result, Resonance vs. Stick Length 5 Resonance frequency [Hz] 4.5 4 3.5 3 2.5 2 [email protected] 0 2 4 6 r2 8 10 12 17 17 Result Damping 0.08 Relative damping [−] 0.07 0.06 0.05 0.04 0.03 0.02 [email protected] 0 2 4 6 r2 8 10 12 18 18 Result Comparison 5 10 0 10 −5 10 0 10 1 2 10 10 2 10 0 10 −2 10 0 10 [email protected] 1 2 10 10 19 19 Some Synthesis Issues [email protected] 20 20 “Worst case” !h = h s Kce = Ap 2 e Ap Mt s ✓ 2 2 + (Vt + Ap x) (Vt Ap x) e Mt ✓ ◆ 2 2 + (Vt + Ap x) (Vt Ap x) Lc Lc x 2 2 ◆ 10 9 Frequency and damping versus displacement xp of a symmetric cylinder 8 7 *+ 6 ;+ *+ ,( 20 +0 +1 21 ./ 345'"67%84 5 9: - 4 h/ !"#$#%&'"() 2 p eA 3 h Mt 1 V1 h0 1 V2 2 h 1 0 −0.5 −0.4 −0.3 −0.2 −0.1 0 0.1 Symetric Cylinder Position 0.2 0.3 0.4 K ce Ap e Mt 1 V1 1 V2 h 0.5 Karl-Erik Rydberg, Linköping University, Sweden [email protected] 15 21 21 Minimize Jerk F =ma Ap p L Bp ẋ ks (x x0 ) + Fexternal = mẍ A sudden change in forces is similar to a “hit”. Minimizing sudden changes is the same thing as limiting the acceleration or minimizing jerk. It is a good strategy for increasing the life time and endurance of machinery ... dF x / dt ... min x ! ramping ẍ [email protected] 22 22 Magnus Sethson [email protected] 23 23
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