Getaran Harmonik Paksa

1. Getaran Harmonik Paksa

2. Getaran Harmonik Paksa • Eksitasi harmonik terjadi biasanya akibat ketidakseimbangan pada mesin-mesin yg berputar. • Eksitasi harmonik dapat berbentuk gaya atau simpangan beberapa titik dalam sistem.

3. c k m Sistem 1 dof mengalami redaman c dan dieksitasi gaya harmonik Fo cos ωt

4. The solution to this equation consists of two • parts, the complementary function, which is • the solution of the homogeneous equation, and • the particular integral. • The complementary function. in this case, is a • damped free vibration. • The particular solution is a steady-state • oscillation of the same frequency was that of • the excitation.

5. See Blackboard

6. Secara Grafis • We can assume the particular solution to be of the form : where X is the amplitude of oscillation ø is the phase of the displacement with respect to the exciting force.

7. Secara grafis

9. Expressing in non-dimensional term by dividing the numerator and denominator by k, we obtain :

10. Expressed in terms of the following quantities:

11. The non-dimensional expressions for the amplitude and phase then become • These equations indicate that the non dimensional amplitude , and the phase ø are functions only of the frequency ratio , and the damping factor ζ

14. See Blackboard

15. Three identical damped 1-DOF mass-spring oscillators.all with natural frequency f0=1, are initially at rest. A time harmonic force F=F0cos(2 pi f t) is applied to each of three damped 1-DOF mass-spring oscillators starting at time t=0. The driving frequencies ω of the applied forces are f0=0.4, f0=1.01, f0=1.6

17. Open Matlab

18. Rotating Unbalance

19. Rotating Unbalance • Unbalance in rotating machines is a common source of vibration excitation. • We consider here a spring-mass system constrained to move in the vertical direction and excited by a rotating machine that is unbalanced.

20. Rotating Unbalance • The unbalance is represented by an eccentric mass m with eccentricity e that is rotating with angular velocity w. • By letting x be the displacement of the non rotating mass (M - m) from the static equilibrium position, the displacement of m is :

21. Rotating Unbalance • The equation of motion is then : • which can be rearranged to : • It is evident that this equation is identical to previous equation, where is replaced by

22. Rotating Unbalance • Hence the steady-state solution of the previous section can be replaced by :

23. Rotating Unbalance • These can be further reduced to non dimensional form :