Appendix B | STT WAVE SHAPING PRINCIPLES | |
T2 – T3 | The pinch mode applies an increasing, |
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| shorted electrode. The dual slope ramp of current accelerates the transfer of |
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| molten metal by the electric pinch forces. The pinch force is directly proportional | |
| to the square of the pinch current. |
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T3 – T5 | dV/dt is the rate of |
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| dV/dt calculations are performed electronically during the pinch mode. Due to the | |
| high resistance of molten iron, the | |
| Near fuse separation at T4 raises the dV/dt value to a designated maximum. The | |
| power source immediately reduces the arc current to 50 Amps. The current drop | |
| occurs before the shorted electrode separates. The T4 event indicates that fuse | |
| separation has occurred, but at a very low current. |
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T5 – T6 | Immediately following separation of the electrode from the weld puddle, peak | |
| current occurs. Peak current is a period of high arc current. The electrode is |
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| quickly saturated by this current and melts back. The jet forces acting upon the | |
| weld puddle (cathode) depress the molten surface, increasing the arc length and | |
| thereby minimizing the possibility of the electrode shorting prematurely. Peak | |
| current is maintained for approximately 1 to 2 milliseconds. Excessive power |
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| would melt too much electrode and cause weld spatter. Even at low power, the | |
| shape of the melted electrode at this point is very irregular. |
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T6 – T7 | Plasma is the final period when the arc current is reduced exponentially from the | |
| peak current level to the background Ievel. The exponential current drop |
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mechanically dampens the weld pool agitation produced during peak current.
WAVE DESIGNER