The electrical shorts which occur often between the electrode and the work in the electrical discharge machining lower the machining speed. To improve the machining speed we have to release the electrode from contacting the work either by actuating the servo motor controlled by the voltage between the electrode and work or by imparting the displacement to the electrode by actuating the moving armature type servo magnet.
In this paper the displacement of armature have been discussed.
From the equation of motion of the armature we obtained the approximate solution and then calculated the steady displacement of the armature considering it's magnetizing characteristic.
By this study the following points were clarified.
1) The transient response of armature is shorter when the exciting current is put in to the coil than when the exciting current is broken in to the coil.
2) For reducing the response time of armature displacement, the decreasing the electrical current response time is more important than increasing the resonance frequencies of the armature.
3) When the time constant τ
E is several times larger than the value of 2π/ω
0, and at the same time when the steady displacement
xS is smaller than the initial air gap
x0, the displacement response can be given approximately by the following equation.
x=
K2/
k (1-ε
1/τEt)
2 (When the exciting current is put into the coil)
x=
K2/
kε
2/τE't (When the exciting current is broken in the coil)
Where ω
0 : angular velocity of armature [Rad/sec],
x : armature displacement [m],
K2 : constant of attractive force [N],
k : spring constant [N/m] and
τ
E : time constant of exciting current [sec].
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