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BULETINUL INSTITUTULUI POLITEHNIC DIN IAŞI - Universitatea ...

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132 Mihăiță Horodincă<br />

behaviour of the driving belt from BT1. The belt generates a very strong<br />

variable component of AEP, with the fundamental frequency on 5.4 Hz (first<br />

peak on Fig. 7) and 6 harmonics (see the peaks 4, 6, 9, 11, 14 and 18). It is<br />

generated by the belt’s stiffness variation (the belt is a little bit damaged, it has a<br />

small tear). The fundamental’s frequency fFB is given by:<br />

π ⋅ D1<br />

π ⋅125mm<br />

(4)<br />

fFB<br />

= f EDM ⋅ = 24.<br />

84Hz<br />

⋅ = 5.<br />

38Hz<br />

.<br />

L<br />

1812mm<br />

c<br />

Fig. 8 – The BT1’s belt behaviour mirroring in PSD<br />

analysis of the IEP signal evolution.<br />

where: fEDM is the rotation frequency of the EDM’s rotor, D1- the diameter of<br />

the belt pulley of the EDM’s rotor, Lc- the belts’ length. A new experiment was<br />

done, with PSD analysis on IEP evolution during the steady-state regime, with<br />

all the clutches disengaged, see Fig. 8. The BT1’s belt behaviour is better<br />

indicated with the harmonic F and the harmonics H1,H2…H6. Because the<br />

mechanical loading of the EDM is smaller, the speed of rotation is bigger so the<br />

frequency in Fig. 8 increases. The first harmonic is bigger than the fundamental<br />

because of the EDM’s rotor elastic system resonance.<br />

5. Conclusions<br />

1. The paper proves that the computer-assisted monitoring of EP parameters<br />

on manufacturing systems (or any other electric actuated equipment) can be an<br />

available experimental research procedure.<br />

2. The computer assisted EP monitoring uses very simple procedures of data<br />

acquisition and processing. Using these research features, it is possible to detect<br />

and study a lot of new static and dynamic phenomena from kinematic chain.

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