Waveform control device for electrical discharge machining apparatus

Abstract: A waveform control device for an electrical discharge machine apparatus which supplies current pulses to the gap between an electrode and a workpiece for machining of the workpiece. A first D.C. source (B₁₀), which supplies at least a part of a voltage that is applied across the gap, is connected in parallel with first and second circuits (10, 12) comprising a series connection of a switch (TR₁, TR₂) and a diode (D₁₀, D₂₀). Connected between a first and second series circuit (10, 12) is a switched conductive circuit which, together with an auxiliary D.C. source (B₂₀), maintains the current flow at a base current level. Control of operation of the switches (TR₁, TR₂) in the first and second circuits permit a controlled discharge of current across the gap while permitting the output voltage to be clamped at a safe level. A plurality of inductive circuits may be used to provide selectivity, where the inductances are different and to provide further control of the discharge current shape. A variable inductance, whose value is proportional to the output peak current, may be used to control current ripple.

Description: The present invention relates to a waveform control device for an electrical discharge machining apparatus as defined in the preamble of claim 1, claim 4 and claim 6, respectively. Such a waveform control device is for example disclosed in the Japanese Patent Application No. JP-A-49-43297, the French Patent Application FR-A-2 189 936 and in the Japanese Utility Model Publication No. 57-33950. A waveform control device for an electrical discharge machining apparatus supplies a pulsating current waveform, controlled to have a desired peak current value I p , between an electrode and a workpiece to generate an electrical discharge in accordance with a set ON-OFF time so that the workpiece can be machined to a desired form. It is desirable that the pulsating current waveform closely approximates a square wave pulse such that the machining operation can be made accurate, thereby requiring fast rise times and fast discharge times. Fig. 24 shows such a circuit diagram of a waveform control device for an electrical discharge machining apparatus as is disclosed in the afore-mentioned publications. In Fig. 24 an electrode 1 is positioned adjacent to a workpiece 2 to be machined. These two elements are connected in a circuit with a first circuit means including a first DC power source B₁ having a first voltage E₁ (V). A second circuit means is connected to said first circuit means and said wirings of said electrode 1 and said workpiece 2, respectively, including an auxiliary power source B₂ having a voltage E₂ (V) and a reactor means constituted by a choke induction coil L₁ serving as a magnetic energy reservoir. A first switching means constituted by a switch S₁ is connected in series between the auxiliary source B₂ and the coil L₁ for controlling the electric current flowing through the coil L₁ to assume a desired value. A second switching means constituted by a switch S₂ which is ON-OFF controlled by a pulse generator (not-shown) is connected in series between the first circuit means with the power source B₁ and the workpiece 2. Furthermore, the circuit comprises first and second diode means constituted by diodes D₁ and D₂, respectively, which are placed in the circuit to direct the current flow. The ON-OFF timing of the switches S₁ and S₂ and the waveform of the electric current i L1 flowing through the coil L₁ of the aforementioned circuit are illustrated in Figs. 25 and 26. Figure 25 shows the operation when the machining apparatus is performing a finishing step on a workpiece whereas Figure 26 shows the operation when a rough machining step is performed. In each of these figures, the switches S₁ and S₂ assume states 1 and O, which are conductive at 1 and non-conductive at O. With this circuit structure, the coil L₁ is connected in series between the electrode 1 and switch S₁ so that the coil acts as an energy reservoir. Accordingly, when the coil L₁ is changed from its saturated to its unsaturated states or vice versa by operation of switches S₁ and S₂, the discharge current from the coil is abruptly changed. For example, if the switch S₁ is ON, the current through the coil L₁ substantially increases so long as the switch S₂ is ON. If the switch S₂ is OFF, while switch S₁ is ON, the current of the coil L₁ is maintained at a substantially constant level because a closed circuit through diode D₂ is formed. If the switch S₁ is turned OFF, any stored energy in the coil is released and the current of the coil L₁ will decrease regardless of whether the switch S₂ might be ON or OFF. When both switches S₁ and S₂ are OFF, the current flows in a circuit comprising power supply B₁, diode D₁, coil L₁ and diode D₂ and settles at a steady state level. When a discharge occurs across the gap between electrode 1 and workpiece 2, a current will flow and the voltage across the elements will drop. As a result, a waveform control circuit using a coil as a discharge current limiting element has advantages over a waveform control circuit using a resistor as the current limiting element since there is no resistor to consume energy. In the circuit constructed in accordance with Figure 24, however, there is a wiring inductance L₃ that exists in connection with the electrode 1 and the workpiece 2. Typically, the wires are several meters long and the resulting inductance is significant, since it will tend to make the current across the gap constant and, thereby extend the period of current flow. As a result of this wiring inductance, a high voltage is generated which can break down switching element S₂ if it is a MOSFET (Metal Oxide Semiconductor Field Effect Transistor) or other transistor, thereby adversely affecting the circuit reliability. Fig. 27 is a circuit diagram showing an example of the prior art using transistors TR₁ and TR₂ as the switches S₁, S₂ of the foregoing circuit. The switching element TR₂ is ON-OFF controlled by an oscillation control circuit 3. The wiring inductance L₃ is not shown but remains effective in this circuit. Fig. 28 is a timing chart showing in waveform (a) the inter-electrode voltage, in waveform (b) the discharge current, in waveforms (c) and (d) the ON-OFF timing of the switching elements TR₂ and TR₁, and in waveform (e) the current flowing through the coil L₁. The discharge current waveform (b) may be controlled by a waveform control method called "slope control". This method is particularly effective for low consumption of the electrodes. According to this method, the discharge current seen in waveform (b) is steeply raised to a base current level having a value I B and is then increased at a predetermined rate to, and maintained at the peak value I p , from which it then should drop rapidly. Specifically, with reference to the coil current in waveform (e), initially during period t₁, switching element TR₁ is switched between ON-OFF states (waveform d) to set the current of the coil L₁ at I B . The current is set in a step-wise fashion, as seen in waveform (e). For a period t₂, when TR₁ is ON, the current flows at an increasing rate via a path including the auxiliary power source B₂, the switching element TR₁, the coil L₁ and the diode D₁. The increasing rate is expressed by the following Equation if the coil L₁ has an inductance L (µH): di/dt = E₂/L (A/µs) Then, for a period t₃, while both TR₂ and TR₁ are OFF, the current flows at a decreasing rate via a path including the DC power source B₁, the diode D₂, the coil L₁ and the diode D₁. The decreasing rate is expressed by the following Equation: di/dt = E₁/L (A/µs) At time t₄, the switching element TR₂ is turned ON, while switching element TR₁ continues to turn ON and OFF, to impress the so called "unloading voltage" voltage E₁ between the electrode 1 and workpiece 2. Then, if a discharge takes place in the gap between the electrode and workpiece at time t₅, the current flows at a generally increasing rate during a period between times t₅ and t₈ through a path including the DC power source B₁, the auxiliary power source B₂, the switching element TR₁, the coil L₁, the electrode 1, the workpiece 2 and the switching element TR₂. On discharge the voltage across the gap will decrease from E₁ to V arc , the arc voltage at which the arc discharge is extinguished. This increasing rate is expressed by the following Equation: di/dt = (E₁ + E₂ - V arc )/L (A/µs) If during the period between times t₅ - t₈, when TR₂ is ON, the switching element TR₁ is turned ON for a period t₆, the current flows at an increasing rate through a path including power supplies B₁ and B₂, switching elements TR₁ and TR₂, coil L₁, electrode 1 and workpiece 2. This increasing rate is expressed by: di/dt = (E₁ + E₂ - V arc )/L (A/µs) However, when TR₁ is turned OFF for a period t₇, the current flows at a decreasing rate through a path including the diode D₂, the coil L₁, the electrode 1, the workpiece 2 and the switching element TR₂. This decreasing rate is expressed by: di/dt = V arc /L (A/µs) If both the switching elements TR₁ and TR₂ are turned OFF at time t₈, the discharge current is blocked, as seen in waveform (b). As a result, the current I L through the coil L₁ (the "breaking current") will flow at a decreasing rate for a period t₉, until it reaches level I B , as seen in waveform (e). During period t₉, the breaking current I L flows along a path including the DC power source B₁, the diode D₂, the coil L₁ and the diode D₁. The decreasing rate is expressed by: di/dt = E₁/L (A/µs) Hence, the time period for the current I L to decrease from I P to I B , i.e. the dropping period of the breaking current, is calculated by: T = L(I P - I B )/E₁ (µs) In the case of waveform control by the slope control method in which the current is increased at an increasing rate from the value I B , defined by I B ≦ I P (I B ≧ 0) as illustrated in Fig. 28, it is necessary to allow I L to drop to reach the condition of I L = I B between cycles. As a result, the circuit of Fig. 27 is troubled by a problem that the cuiescent period of the breaking current cannot be made shorter than the time period T of the foregoing Equation (7). In order to shorten the time period T, it is sufficient to insert a resistance into the path curing the time period t₉ to thereby change the energy to heat. However, this modification is contrary to the aforementioned goal of energy economy. The object of the present invention is to provide a waveform control device for an electrical discharge machining apparatus having a structure as defined in the preamble of claims 1, 4 and 6, and preventing a high voltage generation at the second switching means, whose discharge current waveform possesses a fast rise and fall time, is energy economic and can be produced at a low cost. This object is solved by a waveform control device for an electrical discharge machining apparatus as defined in claim 1, 4 and 6, respectively. In the present invention damaging high voltage is prevented from developing at the second switching means, since the high voltage that may be established by the wiring inductances at the electrode and the workpiece is released through a second series circuit to the first DC-power source, so that it can be prevented from being built up. The waveform control device of the present invention permits the base current IB to rise quickly and allows to shorten the dropping period of the breaking current. In the present invention the voltage of the second DC-power source or the first DC-power source is applied to the reactor means L₂ by the first switching means TR₃ so that the reactor means L₂ is fed with a constant current. As a result, the base current can rise promptly to establish the discharge current waveform. The present invention possesses a further advantage in that it provides a waveform control device which may achieve the desired energy economy by minimizing the restrictions upon the quiescent period and the current ripple ratio. The current that flows through the second DC-power source is either the difference of the base current, i.e. the feedback current from the breaking current or the breaking current itself, and it may be one third or less of the peak current. Thus, a power source of low current capacity can be used for the auxiliary power source B₂ to provide a waveform control device for an electrical discharge machining apparatus at a low and reasonable cost. The waveform control device of the present invention is also highly reliable and accurate. Plural circuits having an equal inductance value may be selectively operated one by one. In such a case, the change of the inductance need not be accomplished to produce current pulses which have a small current ripple ratio and which are stable and reproducable with a short minimum quiescent time, i.e. the waveform control device of the present invention has an optimized performance by providing an output current with a minimum range of ripple and an optimal minimum breaking time. Also the effect of wiring inductance on the circuit switch reliability is compensated, such making it possible to realize a waveform control device having high reliabilty and accuracy. Finally, a reactor of variable capacity type can be used in an advantageous manner as a discharge current limiting element and, in that case, the quiescent time and the current ripple ratio can be minimized over a wide region of peak current values to achieve further energy economy. Thus, the single reactor of the waveform control devices of the present invention can be of the variable capacity type, which may have its inductance valued changed and controlled in accordance with the peak current value of the electrical discharge. In case a plurality of reactors are used, their inductance values may be equalized for cyclic operation. Further advantageous embodiments of the present invention can be taken from the dependent claims. Furthermore, other objects of the present invention will become apparent from the following description, in connection with the embodiments thereof with reference to the accompanying drawings. In the drawings: Fig. 1 is a circuit diagram showing a first embodiment of the waveform control apparatus of the present invention. Figs. 2(a) to 2(g) are timing charts explaining the current waveforms of the circuit of Fig. 1 and the timing of the switching elements. Figs. 3 to 5 are circuit diagrams showing modifications of the first embodiment. Fig. 6 is a circuit diagram showing a second embodiment of the present invention. Figs. 7(a) to (7g) are timing charts explaining the current waveforms of the circuit of Fig. 6 and the timing of the switching elements. Figs. 8 to 11 are circuit diagrams showing modifications of the second embodiment. Fig. 12 is a circuit diagram showing a third embodiment of the present invention. Figs. 13(a) to 13(g) are timing charts explaining the current waveforms of the circuit of Fig. 12 and the timing of the switching elements. Figs. 14 to 16 are circuit diagrams showing modifications of the third embodiment. Fig. 17 is a circuit diagram for explaining a further advantageous feature of the present invention. Fig. 18 is a graph presenting the region of the allowable inductances values. Fig. 19 is a diagram showing a possible structure of the inductance value changing control circuit. Fig. 20 is a circuit diagram for explaining further advantageous features of the present invention. Fig. 21 is a timing chart showing operations of the circuit diagram in Fig. 20; Fig. 22 is a graph presenting the region of allowable inductances values. Fig. 23 is a diagram showing the structure of the oscillation control circuit of the circuit in Fig. 20; Fig. 24 is the waveform control circuit of the prior art. Fig. 25 and 26 are timing charts for the circuit of Fig. 24. Fig. 27 is a circuit diagram showing another example of the prior art. Fig. 28 is a timing chart for the circuit for Fig. 27. The waveform control device of the present invention will be described in connection with several embodiments, with reference to the accompanying drawings. Fig. 1 is a circuit diagram showing a first embodiment of the present invention. Switching elements appearing in Fig. 1 are exemplified by MOSFETs but may comprise other electrical switches such as semiconductor switches generally. In Fig. 1, there is connected in parallel with a first DC power source B₁₀ a first series circuit 10, which includes a switching element TR₁ and a diode D₁₀, having a node 15 defined between them. A second series circuit 12, including a second DC power source B₂₀, a diode D₂₀ and a switching element TR₂, is also connected in parallel with the first DC power source B₁₀. Node 14 is defined between the power source B₂₀ and the diode D₂₀ and node 16 is defined between the diode D₂₀ and the switching element TR₂. A switching element TR₃ is connected between the node 15 in the first series circuit 10 and the node 14 in the second series circuit 12. Connected to node 16, at one output terminal 21 of the waveform control device, is workpiece 2. An electrode 1 is connected at the other output terminal 20, which also is tied to an internal node 17. A reactor L₂ is connected between the electrode 1, through output terminal 20, and the node 15. A first diode D₃₀ is connected between the node 17 and a node 18, located between the first DC power source B₁₀ and the second DC power source B₂₀. The components are sized so that a machining current may be fed between the electrodes. In the preferred embodiments, it is assumed that inductances 100 and 101 will exist for the electrode 1 and the workpiece 2, respectively, due to the wiring. The first DC power source B₁₀ will produce voltage V₁₀ in a range of 60 to 150 V, and the second DC power source B₂₀ will produce voltage V₂₀ in a range of 5 to 30 V. Figs. 2(a)-2(g) illustrate waveforms and timings that are relevant to the operation of the waveform control device of Figure 1. The waveform in Figure 2(a) is an optimum current waveform to be output by the waveform control device of the present invention. In this case, a base current I B is selected at about 1/3 of a peak current I p so that the output current may rise from I B to I p as quickly as possible. The gradient ϑ of the slope of the current rise reflects a constant rate of increase for the current. A single discharge comprises the combination of a discharge period T₁ and a breaking period T₂. The waveform in Figure 2(b) represents the actual output (or discharge) current from the device as a function of time while the waveform in Figure 2(c) illustrates the current of the reactor L₂ as a function of time. Numeral 22 designates the minimum or base current I B in the waveform of Figure 2(c). Figure 2(d) illustrates the timing for the inter-electrode voltage across the gap between the electrode 1 and workpiece 2. Figs. 2(e), 2(f) and 2(g) illustrate the timings for switching the switching elements TR₁, TR₂ and TR₃, respectively. Turning to a description of the operation of the first embodiment of the invention, reference is made to Figure 1 and Figures 2(a)-2(g). In the steady state, no discharge is caused in the circuit of Fig. 1 and the switching element TR₃ is switched between OFF and ON whereas the switching elements TR₁ and TR₂ are OFF. Thus, when the switching element TR₃ is ON, the base current I B flows through a path composed of the reactor L₂, the diode D₃₀, the second DC power source B₂₀ and the switching element TR₃. When the switching element TR₃ is OFF, on the other hand, the base current I B flows through a second loop composed of the reactor L₂, the diode D₃₀, the first DC power source B₁₀ and the diode D₁₀, all to maintain the current flowing through the reactor L₂ at a constant level. In short, switching element TR₃ is switched on and off to apply the voltage of power source B₂₀ to the reactor L₂ to maintain the current through the reactor L₂ at a generally constant level. In any case, as seen from the initial portions of the waveforms in Figures 2(c)-2(g), prior to time t₁₁ when TR₂ goes ON, the current is steady at I B and no voltage appears across the interelectrode gap. If the switch element TR₂ is turned ON at time t₁₁ of Fig. 2(g), while TR₃ is ON and after the steady state base current I B has been established as described above, a voltage is applied between the output terminals 20 and 21, i.e., across the electrode gap between the electrode 1 and the workpiece 2, as shown in Fig. 2(d). The voltage applied is the voltage V₁₀ of the first DC power source B₁₀, and is called the "unloading voltage". Discharge will be effected at this voltage level. If discharge takes place at time t₁₂, the switching element TR₃ is turned OFF and the switching element TR₁ is turned ON, while TR₂ remains ON. This switching state is illustrated in Fig. 2(e), and the output current at this time begins to increase rapidly as seen in Fig. 2(b). Also, at this time, the inter-electrode voltage between the electrode 1 and the workpiece 2 has dropped to a discharge voltage V₁₁ which is lower than the unloading voltage V₁₀ by 25 to 40 V. Accordingly, with node 17 being at V₁₁ and node 18 being at V₁₀, a reverse bias is placed across diode D₃₀ and the base current I B , which had been flowing through the diode D₃₀ in the first steady state loop, begins to flow through the output terminal 20 to the electrode 1. Since the reactor L₂ already had a current flow via the first steady state loop, the output current I B rises steeply to the base current level I B , as indicated at 23 in Fig. 2(b). The output current continues a stepped rise as switch TR₁ is repeatedly switched, as indicated at 24, until it reaches the peak current I p . Once at the peak current I p , the switching element TR₁ continues to be switched in order to maintain the output current 25 at the peak level I p . When TR₁ is ON, voltage V₁₀ is applied to the electrode directly and current rises while when TR₁ is OFF, output current drops slightly. The TR₁ ON time is larger than the OFF time during the current rise but once the peak current is reached, the OFF time is longer. Due to the effect of reactor L₂, element TR, may be turned off and left off some time before the end of the discharge period T₁. After lapse of the discharge period T₁, the switching element TR₂ is turned OFF at time t₁₃ of Fig. 2(g). Since switches TR₁ and TR₃ already are OFF, the output current flow at the level I p drops. Specifically, due to the effect of the wiring inductances 100 and 101 between the output terminals 20 and 21 and the electrode 1 and the workpiece 2, respectively, the output current that was flowing through the electrode 1, now flows through the diode D₂₀, the second DC power source B₂₀ and the diode D₃₀ and abruptly drops, as indicated at 26 in Fig. 2(b). This current is called the "breaking current". At this same time, current is flowing forward in the reactor L₂, as indicated at 27 in Fig. 2(c), and thus in the forward direction through diode D₃₀, so that the breaking current can flow backward through the diode D₃₀. This results in currents flowing in opposite directions at D₃₀ that will cancel each other. This feature causes the output current to drop quickly, notwithstanding the effect of the wiring inductances. As a result, the surge voltage applied to the switching element TR₂ is clamped at the sum of the voltage V₁₀ of the first DC power source B₁₀ and the voltage V₂₀ of the second DC power source B₂₀. This clamping will prevent the switch TR₂ from being burned out by the voltage surge. Viewed another way, the circuit of D₂₀, D₃₀ and B₂₀ will act as an absorbing circuit for the current flow due to the wiring inductances. As noted above, the current through the reactor L₂ decreases for the period (from the time t₁₃ to t₁₄) indicated at 27 in Fig. 2(c), because all the switching elements TR₁, TR₂ and TR₃ are OFF. This decrease is promptly effected because the peak current I p is fed back through the reactor L₂, the diode D₃₀, the first DC power source B₁₀ and the diode D₁₀ by turning the switch element TR₂ OFF, as shown in Fig. 1. When the peak current I P decreases to the level of the base current I B , as seen in the quiescent period between portions 27 and 22 of Figure 2(c), the switching element TR₃ begins performing its switching at the time t₁₄ of Fig. 2(g) to maintain the current of the reactor L₂ at the base current I B . With the switching timings specified above, the current waveform for electrical discharge machining can be controlled to output the optimum discharge current, to achieve low consumption of the electrode 1 and high machining speed. Next, Fig. 3 shows a modification, in which the switching elements TR₁, TR₂ and TR₃ and the diodes are shifted from the positions of Fig. 1. This modification operates in a manner similar to the circuit of Fig. 1. Fig. 4 shows another modification, in which the switching elements of Fig. 1 are exemplified by P-channel MOSFETs. This modification accomplishes the operations of the circuit of Fig. 1 by making the same connections while inverting the polarities of the first DC power source B₁₀ and the second DC power source B₂₀. Fig. 5 shows still another modification in which the circuit of Fig. 1 is effectively duplicated and joined into a single circuit. In this modification, two series circuits, i.e., a series circuit 10A, composed of a switching element TR₁₁ and a diode D₁₁, and a series circuit 10B, composed of a switching element TR₁₂ and a diode D₁₂, are connected in parallel with the first DC power source B₁₀. With the series circuits 10A and 10B, there are connected in parallel a switching element TR₃₁ and a reactor L2A, and a switching element TR₃₂ and a reactor L2B. These two circuits (referred to as "A and B" hereafter) can accomplish the switching operations independently or simultaneously so that the present modification has the several advantages over the circuit of Fig. 1. Particularly, if the current shown in Fig. 2(c) has a long decreasing time period 27, it may fail to reach the base current I B by the time of the next discharge. By switching between the aforementioned pair of circuits A and B alternatively, however, the decreasing time period can be long and still permit the base current I B to be reached before the next discharge. This approach is effective when the reactor has a high inductance or when the breaking time T₂ of Fig. 2(a) is short. It permits a short OFF time between pulses to be obtained and enhances operating efficiency. Reactors L2A and L2B can have identical inductances. In such case, the cycles in each of circuits A and B may be conducted concurrently, then currents can be added and higher pulse frequency obtained. If the reactors have different inductances, the difference can be used to control current ripple. For example, if the reactor L2A has a larger inductance than reactor L2B, the circuit A performs operations similar to those of the circuit of Fig. 1 and it operates if the peak current I p is large. If, on the other hand, the reactor L2B is made to have a larger inductance than that of the reactor L2A, the circuit B can provide a stable output current having little ripple even for a small output current. The existence of a large peak output current I p will permit the differences in current ΔI to be ignored but when I p is small, a problem arises with the difference in current ΔI where: ΔI = v₁ - v arc L Δ where ΔT is the ON time of the switch that causes the ripple, V arc is the voltage across the gap between workpiece 2 and electrode 1 and V₁ is the voltage of B₁₀. Clearly, where I p is small, the reactor inductance value should be large and vice versa, as explained further in connection with Figure 17, because a large inductance means a smaller ΔI and a small inductance means a large ΔI. Thus, when there are different inductance values used in different ones of the circuits A, B, etc. the circuit having an inductance that minimizes ripple for a given I p can be selected . Although the present invention is exemplified in Figure 5 by a two circuit configuration, it can attain similar effects with a structure having more than two circuits. Also a variable inductance may be used, as later described. Fig. 6 is a circuit diagram showing a second embodiment of the present invention. This second embodiment is different from the circuit of Fig. 1 in that a second series circuit 12A is constructed to only include the diode D₂₀ and the switching element TR₂. The second DC power source B₂₀ is connected in series with a fourth diode D₃₀ and a node 14 is defined between them. Moreover, the switching element TR₃ and the first diode D₄₀ are connected in series between the node 14 and a node 15 defined between the switching element TR₁ and the diode D₁₀ of the first series circuit 10. The remaining structures are similar to those of Fig. 1. Figs. 7(a) to 7(g) are timing charts like those of Figs. 2(a)-2(g). One difference in this case, however, is that the unloading voltage V₁₂ is the difference between the voltage V₁₀ of the first DC power source B₁₀ and voltage V₂₀ of the second DC power source B₂₀, i.e., V₁₂ = V₁₀ - V₂₀. Since the unloading voltage V₁₂ can be made lower than that of the circuit of Fig. 1, the inter-electrode gap can be controlled more finely to improve the machining accuracy. As in the first embodiment, during the steady state with no discharge, the switching element TR₃ performs its switching operation, but the switching elements TR₁ and TR₂ are OFF. As a result, the base current I B flows through the path composed of the reactor L₂, the second DC power source B₂₀, the diode D₄₀ and the switching element TR₃, while the switching element TR₃ is ON, and through the path composed of the reactor L₂, the diode D₃₀, the first DC power source B₁₀ and the diode D₁₀, while the switching element TR₃ is OFF. As before, the current flowing through the reactor L₂ is maintained constant, at the base current level I B . If a discharge is to take place, the switching element TR₃ is turned OFF, and the switching element TR₁ performs its switching operation. As a result, the inter-electrode voltage between the electrode 1 and the workpiece 2 assumes a value equal to the discharge voltage V₁₁ which is lower than the unloading voltage V₁₂ by about 25 to 40 V. The base current I B , flowing through the second DC power source B₂₀ flows through the output terminal 20 to the electrode 1. Since the current has already been flowing through the reactor L₂, the current rises quickly from the base current I B , as indicated at 23 in Fig. 7(b). The slope current 24 continues to rise, as switch TR₁ continues to repeat its switching. When the peak current I p is reached, the current is maintained at the constant value 25 by the TR₁ switching operations, until the discharge period T₂ begins. When the discharge period begins, the switching element TR₂ is turned OFF. As a result, the current that had been flowing through the electrode 1 is diverted to the diode D₂₀, the diode D₃₀ and the second DC power source B₂₀ by the wiring inductances 100 and 101. The diversion continues as the output current drops, as indicated at 26 in Fig. 7(b). This breaking current can flow backward through the diode D₃₀ because diode D₃₀ is rendered conductive by the forward flow of current 27 through the reactor, as seen in Fig. 7(c). As a result, the surge current applied to the switching element TR₂ is clamped to the voltage V₁₀ of the first DC power source B₁₀ so that no high voltage is generated across TR₂. The peak current I p is promptly reduced, when the switching element TR₂ is turned OFF, by the feedback through the reactor L₂, the second DC power source B₂₀, the diode D₃₀, the first DC power source B₁₀ and the diode D₁₀. When the peak current I p drops to the level of base current I B , the switching element TR₃ is restored to its switching operation to maintain the current of the reactor L₂ at the base current I B as in the case of Fig. 1. Figs. 8 to 10 show modifications of the second embodiment that are entirely similar to the modifications of the first embodiment shown in Figs. 3 to 5, respectively. The operation of these circuits will be apparent from an understanding of the first and second embodiments, and the modifications of the first embodiment, as presented in detail herein. Figure 11 shows a circuit which is similar to the circuit of Figure 6, however at node 17, a third power source B₃₀ is placed in a series circuit with diode D₄₀ and switch TR₃ connected to node 15, forming a loop separate from that of the loop containing a series connection of diode D₃₀ and power source B₂₀. Thus, by contrast to Figure 6, in Fig. 11, only the feedback current flows through the third DC power source B₃₀, which acts to create the I B current, whereas the breaking current flows through the second DC power source B₂₀, which acts to absorb the surge current. Otherwise, this circuit functions in a manner similar to that of the circuit of Fig. 6. Next, Fig. 12 is a circuit diagram showing a third embodiment of the present invention. This third embodiment is different from the circuit of Fig. 1 in that not only the first and second series circuits 10 and 12 but also a third series circuit 13 composed of the diode D₃₀ and the switching element TR₃ is connected in parallel with the first DC power source B₁₀. Moreover, the reactor L₂ is connected between the node 15 and the node 19 defined between the diode D₃₀ and the switching element TR₃ of the third series circuit 13. The switching element connects node 19 to one terminal of power source B₁₀, rather than to a terminal of auxiliary power source B₂₀. A fourth diode D₅₀ is connected between the node 19 and the output terminal 20. The remaining structures are similar to those of Fig. 1. The diode D₅₀ is added to prevent the voltage between the electrode 1 and the workpiece 2 from dropping when the switching element TR₃ is turned ON. Figs. 13(a) to 13(g) are timing charts of the circuit of the third embodiment, which are similar to those of Fig. 2(a)-2(g) except that the switching timings of the switching element TR₁ are slightly different. The third embodiment performs operations similar to those of the first and second embodiments. However, what flows through the second DC power source B₂₀ is the breaking current, having a current level far lower than the peak current I p . Accordingly, the second DC power source B₂₀ need have only a small current capacity. Figs. 14 to 16 show modifications of the third embodiment that are similar to the modifications to the first embodiment shown in Figs. 3 to 5, respectively. The operations of these circuits are again apparent from an understanding of the first and second embodiments and modifications thereof, as presented in detail herein. In the embodiments thus far described, the reactor L₂ as the discharge current restricting element has been assumed to have a fixed inductive value. In the following case, however, a variable type reactor is used to shorten the breaking period T given by the foregoing equation (7). Fig. 17 is a circuit diagram incorporating a variable type reactor L3 as a further advantageous feature. The circuit will be described, for purposes of simplicity, as an improvement to the conventional circuit of Fig. 27, although the principles of this circuit are applicable to each of the previous embodiments. In Fig. 17, reference character L₃ designates a reactor having a variable inductance, which is controlled by a control means 7. The inductance value L selected for the variable inductance L₃ is determined by the allowable current ripple value I and the allowable minimum breaking time T min . If the minimum ON period of the switching element TR₁ is designated as T, the allowable minimum current ripple value is expressed, using Equation (3) as follows: ΔI = (E₁ + E₂ - V arc )/L x ΔT(A) From this Equation, it is found that the ripple value becomes smaller as the inductance L becomes higher. From Equation (7), it is also found that the allowable breaking minimum period T min can be made shorter as the inductance L becomes lower. The optimum inductance value may be determined by considering both of these offsetting factors. If the allowable ripple ratio is set at ΔI/I p = R, then ΔI = I p x R. The inductance valve L permitted in view of the allowable ripple is determined from the following Formula: L ≧ (E₁ + E₂ - V arc )/(I p x R) x ΔT If the minimum allowable breaking period is designated by T min , the allowable inductance value L is determined from Equation (7) as follows: L ≦ T min x E₁/(I p - I B ) Here, for I B = k x I p (k: a proportional constant < 1), Formula (11) can be rewritten into the following form: L ≦ T min x E₁/(1 - k) I p Hence, the inductance value L is defined by the following Formulas (from the Formulas (10) and (12)): |(E₁ + E₂ - V arc )x ΔT|/(I p x R) ≦ L ≦ E₁ x T min /(1 - k)I p Fig. 18 presents the region which is defined by Formula (13), located between curves defined by Formulas (10) and (12). The hatched portion 8 indicates the allowable inductance region. The values R and T min appearing in Formula (13) can be changed according to the value I p . For example, those values would be larger for the region of large I p than for the region of small I p . Fig. 19 is a diagram showing the structure of the variable capacity reactor L₃ and the control means 7. In Fig. 19, coil 31 may have its inductance value changed and set according to the position of a sliding contact 32 moveable by a pulse stepping motor 33. The step motor 33 is controlled by a command pulse number sent to a comparator 35 from a memory 34, such as a ROM which may store a data table having pulse numbers corresponding to inductance values selectable in accordance with various values of I p . The comparator 35 compares the command with the value of a counter 36 to determine the rotating direction of the motor 33 and sends an UP/DOWN signal to a pulse motor driver 37 and the counter 36. Moreover, the comparator 35 takes the difference between the value of the counter 36 and the current command to provide an oscillator 38 with a movement number. Then, oscillator 38 sends the commanded number of pulse to the pulse stepping motor driver 37 so that the pulse stepping motor 33 is enabled to position the sliding contact 32 to the commanded position to obtain a desired inductance value. These pulses are also sent to the counter 36 so that the present value can be up dated. The inductor 37 is of the variable capacity type, however as an alternative structure, as further advantageous features, a plurality of coils having different inductance values may be selectively switched into the circuit. Fig. 20 is a circuit diagram including these advantageous features which is yet another improvement of the conventional circuit of Figure 27. Unlike the improvement of Figure 17, the inductance value is not changed. Instead, reactors having equal inductance values are used to construct a plurality of circuits. (The circuits of Figs. 5, 10 and 16 correspond to the case in which the inductance values may be different, but the concept of Fig. 20 can be applied specifically to the case of a common inductance value.) Fig. 20 shows the case of two overlapping circuits, which have their respective components suffixed by letters A and B. In order to prevent each of the two circuits from feeding current to the other, switching elements TR 2A and TR 2B are inserted at positions in the path of each reactor connection to the electrode 1. In Fig. 20, the operations of any one circuit are identical to those of Fig. 27. The two circuits operate alternately in Fig. 20, as shown in Fig. 21, and the breaking time for each circuit is (OFF time x 2 + ON time + unloading time). The current ripple ΔI calculated in Equation (9) can thus be reduced to about one third if the inductance value L of Equation (7) can be increased about three times. As shown in Fig. 22, moreover, the inhibition region of T min of Fig. 19 is not violated for one value L₀. Next, the switching elements TR 2A and TR 2B and an oscillation control circuit 3 will be described with reference to Fig. 23. Reference numeral 41 designates an oscillator for generating and sending oscillation pulses (ON-OFF times) to each of AND gates 42 and gate selectors 43. These gate selectors 43 are operated by the pulses sent from the oscillator 41 and the AND array 42 to send out signals cyclically The selectors drive their corresponding transistors TR 2A , TR 2B , - - -, and TR 2B by ANDing the AND array outputs and the oscillation pulses.

Claims: A waveform control device for an electrical discharge machining apparatus operative to apply a current across a gap between an electrode (1) and a workpiece (2) being connected by wirings having an inherent inductance (100,101) comprising: a) first circuit means, including a first DC power source (B₁₀) having a first voltage; b) a second circuit means connected to said first circuit means and to said wirings of said electrode (1) and said workpiece (2), respectively, including a second DC power source (B₂₀) having a second voltage, a first and second switching means (TR₃, TR₂), a first and second diode means (D₃₀, D₂₀) and a reactor means (L₂); characterized in that, c) said first circuit means includes a first series circuit (10) connected in parallel to said first DC power source (B₁₀) and comprising a third switching means (TR₁) and a third diode means (D₁₀) connected to each other at a first node (15); d) said second circuit means comprises: d1) a second series circuit (12) connected in parallel to said first DC power source (B₁₀) and comprising said second DC power source (B₂₀), said second switching means (TR₂) and said second diode means (D₂₀), a second node (16) being defined between said second switching element (TR₂) and said second diode means (D₂₀); d2) said reactor means (L₂) being disposed in a series circuit arrangement including the electrode (1) and the workpiece (2) and connecting said first node (15) and said second node (16); d3) said first switching means (TR₃) being disposed in a series circuit arrangement connecting a third node (14) defined between said second DC power source (B₂₀) and said second diode means (D₂₀) and said first node (15); and d4) said first diode means (D30) being disposed in a circuit arrangement connecting a fourth node (18) defined between said first DC power source (B₁₀) and said second DC power source (B₂₀) and a fifth node (17) defined between said reactor means (L₂) and one of said electrode (1) and said workpiece (2). Waveform control device according to claim 1, characterized in that said voltage of said first power source (B₁₀) is greater than the voltage of said second power source (B₂₀). Waveform control device according to claim 1, characterized in that said first series circuit (10) comprises a plurality of series circuits (10a,10b) and said reactor means (L₂) comprises a plurality of reactors (L 2a ,L 2b ) and said first switching means (TR₃) comprises a plurality of switching elements (TR₃₁, TR₃₂), a respective one of said reactors (L 2a ,L 2b ) and one of said switching elements (TR₃₁, TR₃₂) being connected to a respective one of said series circuits (10a,10b). Waveform control device for an electrical discharge machining apparatus operative to apply current across a gap between an electrode (1) and a workpiece (2) connected by wirings having an inherent inductance (100,101), comprising: a) a first circuit means including a first DC power source (B₁₀) having a first voltage (V₁₀); and b) a second circuit means connected to said first circuit means and to said wirings of said electrode (1) and said workpiece (2), respectively, including a second DC power source (B₂₀) having a second voltage (V₂₀), a first and second switching means (TR₃, TR₂), a first and second diode means (D₄₀, D₂₀) and a reactor means (L₂); characterized in that c) a first series circuit (10) and a second series circuit (12a) are provided respectively connected in parallel to said first DC power source (B₁₀), said first series circuit (10) comprising a third switching means (TR₁) and a third diode means (D₁₀) and said second series circuit comprising said second switching means (TR₂) and said second diode means (D₂₀) with a node (18) defined between said first and second series circuits; d) said reactor means (L₂) is disposed in a third circuit comprising the electrode (1) and the workpiece (2) and connecting a node (15) between the third switching element (TR₁) and said third diode means (D₁₀) of said first series circuit (10) and a node (16) between the second switching element (TR₂) and said second diode means (D₂₀) of said second series circuit; said second DC power source (B₂₀) and a fourth diode means (D₃₀) being disposed in series in a circuit connecting a node (18) between said first DC power source (B₁₀) and said second series circuit (12A) and a node (17) between said reactor means (L₂) and one of said electrode (1) and said workpiece (2); and e) said first switching means (TR₃) and said first diode means (D₄₀) are disposed in a series circuit connecting a node (14) between said second DC power source (B₂₀) and said fourth diode means (D₃₀) and a node (15) between the third switching element (TR₁) and said third diode means (D₁₀) of said first series circuit (10). Waveform control device according to claim 4, characterized in that said first series circuit (10) comprises a plurality of series circuits (TR₁₂, D₁₂,TR₁₁,D₁₁) and said reactor means (L₂), said first switching means (TR₃) and said first diode means (D₄₀) comprise a plurality of reactors (L 2a ,L 2b ), a plurality of switches (TR₃₁,TR₃₂) and a plurality of diodes (D₄₁,D₄₂,) respectively, said plurality being a number which is the same number as that of said series circuits. Waveform control device for an electrical dischsarge machining apparatus operative to apply a current across a gap between an electrode (1) and a workpiece (2) connected by wirings having an inherent inductance (100,101), comprising: a) a first circuit means, including a first DC power source (B₁₀) having a first voltage; and b) a second circuit means connected to said first circuit means and to said wirings connected to said electrode (1) and said workpiece (2) including a second DC power source (B₂₀) having a second voltage, a first and second switching means (TR₃,TR₂), a first and second diode means (D₃₀, D₂₀) and a reactor means (L₂); characterized in that c) said first circuit means includes a first series circuit means (10) connected in parallel to said first DC power source (B₁₀) and comprising a third switching means (TR₁) and a third diode means (D₁₀) connected to each other at a first node (15); and d) said second circuit means include d1) a second series circuit means connected in parallel to said first DC power source (B₁₀) and comprising said second DC power source (B₂₀), said second switching means (TR₂) and said second diode means (D₂₀), a second node (16) being defined between said second switching means (TR₂) and said second diode means (D₂₀); and d2) a third series circuit means connected in parallel to said first DC power source (B₁₀) and comprising said first switching means (TR₃) and said first diode means (D 30. ) a third node (19) being defined between said first switching means (TR₃) and said first diode means (D₃₀); e) fourth diode means (D₅₀) is disposed in a series circuit arrangement comprising said electrode (1) and said workpiece (2) and connecting said third node (19) and said second node (16); and f) said reactor means (L₂) is connected between said first node (15) and said third node (19). Waveform control device according to claim 6, characterized in that each said first series circuit means and said third series circuit means comprise an equal number of series circuits, and said reactor means (L₂) comprises a plurality of reactors (L 2a ;L 2b ) and said fourth diode means (D50) comprises a plurality of diodes (D₅₂,D₅₁), a respective one of said reactors (L 2b ,L 2a ) and a respective one of said diodes (D₅₁,D₅₂) being connected to a respective one of said series circuits (D₁₂,TR₁₂;D₁₁,TR₁₁). Waveform control device according to claims 1,4 or 6, characterized in that said reactor means (L₂) is of a variable capacity type having its inductance value changed and controlled in accordance with a peak value of a discharge current. Waveform control device according to claims 3,5 or 7, characterized in that said plural reactors (L 2a ,L 2b ) have an identical inductance value, and cyclic operations of each circle are performed. Waveform control device according to claims 3,5 or 7, characterized in that at least two of said plural reactors L 2a ,L 2b have different inductance values and said values are selected in accordance with the peak value of the discharge current.

Inventors: KINBARA YOSHIHIDE C O MITSUBIS, NISHIKAWA MORIHISA C O MITSUBI, OZAKI YOSHIO C O MITSUBISHI DE, KINBARA, YOSHIHIDE, NISHIKAWA, MORIHISA, OZAKI, YOSHIO, KINBARA, YOSHIHIDE, C/O MITSUBISHI DENKI K.K., NISHIKAWA, MORIHISA, C/O MITSUBISHI DENKI K.K., OZAKI, YOSHIO, C/O MITSUBISHI DENKI K.K.
Applicants: MITSUBISHI ELECTRIC CORP, MITSUBISHI DENKI KABUSHIKI KAISHA
Application year: 1990
Main classification: B23H1
IPC codes: B23H1