Abstract:
A method and system of generating a ringing magnetic pulse for the treatment of flowing liquids include&#39;s a coil and an SCR coupled in series with the coil to form a first loop. An electronic switch is coupled in series with the coil to form a second loop. An AC voltage signal is applied to the coil having first and second half-cycles. Current is conducted through the first loop during the first half-cycle when the SCR is forward biased while preventing current from conducting through the second loop. Current is conducted through the second loop during a portion of the second half-cycle while current is prevented from conducting through the first loop. Current is interrupted through the second loop during another portion of the second half-cycle upon the coil current reaching a predetermined value to interrupt current flowing through the coil, thereby generating a ringing magnetic pulse.

Description:
CROSS-REFERENCE TO RELATED APPLICATION  
       [0001]     This application is entitled to the benefit of and incorporates by reference essential subject matter disclosed in Provisional Patent Applications No. 60/634,959 filed on Dec. 10, 2004. 
     
    
     FIELD OF THE INVENTION  
       [0002]     This invention relates generally to the treatment of flowing water or other liquids, and more particularly to the treatment of such liquids with a ringing magnetic pulse.  
       BACKGROUND OF THE INVENTION  
       [0003]     In the past, various different devices and methods have been proposed for treating liquid with electromagnetic flux for the purpose of reducing the scaling propensity of the liquid, for reducing the number of living microorganisms contained in the liquid or for other purposes. For example, an apparatus for treating flowing liquid with electromagnetic flux is disclosed in U.S. Pat. No. 6,063,267 assigned to Clearwater Systems, LLC, the disclosure of which is herein incorporated by reference.  
         [0004]     Some of these prior devices have used either stationary or movable permanent magnets for producing a magnetic flux, and others have used electrical coils arranged in various different ways with respect to pipes conducting the liquid, with the coils being energized by either a direct current power source or an alternating current power source to create an electromagnetic flux used as the liquid treatment factor. In the case of devices using electromagnetic flux, it is known from U.S. Pat. No. 5,702,600 to provide an apparatus including a plurality of electrical coils surrounding different separate longitudinal sections of a liquid conducting pipe, with two of the coils being wound on top of one another, a diode being so connected in circuit with the coils and with the power source that current from the power source is conducted through the coils only during alternate half-cycles of one voltage polarity, with some current of a ringing nature apparently flowing through each coil following the end of each half-cycle of diode conduction. However, the ringing current, and the electromagnetic flux produced appears to be weak and of very short duration so as to be of small effectiveness.  
         [0005]     Prior systems for treating flowing liquids with a ringing magnetic pulse used a diode switch to interrupt the coil current when the current reversed polarity. For example, a prior analog control system produced a relatively small “ringing” pulse on the coil voltage when the current was blocked by the diode because there was still voltage remaining on the coil capacitance. The analog control system was modified to generate a much larger “ringing” voltage of up to ten times that of the above-mentioned previous analog control system. This design used in place of the diode, a switch comprising up to ten parallel-connected 450 volt MOSFETs. This switch interrupted the current flow before the coil current reached zero, leaving stored magnetic energy in the coil which powered the larger “ringing” pulse. With this approach, a switch is needed that can be electronically “turned off”, and such switches tend to be low current devices with relatively high “011 state” resistance. As a result, ten switches in parallel are needed to handle the full coil current.  
         [0006]     Digital control systems have been developed in order to improve stability of operation relative to that of the above-mentioned prior analog control systems. However, there is still a need to lower the complexity and cost of such digital control systems.  
         [0007]     Accordingly, it is a general object of the present invention to provide a system and method of treating liquid with a ringing magnetic pulse which overcomes the above-mentioned drawbacks and disadvantages of prior systems and methods of treating liquids.  
       SUMMARY OF THE INVENTION  
       [0008]     The present invention resides in a method of generating a ringing magnetic pulse for the treatment of flowing liquids. An inductive coil and a silicon controlled rectifier (SCR) coupled in series with the coil are provided to form a first electrical loop. An electronically controlled switch, such as a MOSFET, is coupled in series with the coil to form a second electrical loop. The switch is preferably electrically connected generally in parallel with the SCR. An AC voltage signal is applied to the coil. The AC voltage signal has a period including a first half-cycle and a second half-cycle of opposite polarity to that of the first half-cycle. Current is conducted through the first loop during at least a portion of the first half-cycle when the SCR is forward biased while preventing current from being conducted through the second loop. Current is conducted through the second loop during a first portion of the second half-cycle while current is prevented from being conducted through the first loop when the SCR is reverse biased. Current is prevented from flowing through the second loop during a second portion of the second half-cycle upon the current flowing through the coil reaching a predetermined value to interrupt current flowing through the coil and to thereby generate a ringing magnetic pulse.  
         [0009]     The present invention also resides in a system for generating a ringing magnetic pulse. The system includes an inductive coil to be powered by an AC voltage signal having a period including a first half-cycle and a second half-cycle of opposite polarity to that of the first half-cycle. A silicon controlled rectifier (SCR) is coupled in series with the coil to form a first electrical loop. An electronically controlled switch is coupled in series with the coil to form a second electrical loop. The switch is electrically connected generally in parallel with the SCR. The system further includes means for conducting current through the first loop during at least a portion of the first half-cycle when the SCR is forward biased while preventing current from being conducted through the second loop. Means are provided for conducting current through the second loop during a first portion of the second half-cycle while current is prevented from being conducted through the first loop when the SCR is reverse biased. The system further includes means for preventing current from flowing through the second loop during a second portion of the second half-cycle upon the current flowing through the coil reaching a predetermined value to interrupt current flowing through the coil and to thereby generate a ringing magnetic pulse.  
         [0010]     The invention also resides in other details of method of operation and construction of the system as set forth in the appended claims, and these details will be apparent from the following detailed description of the preferred embodiment of the invention, from the accompanying drawing and from the claims themselves.  
     
    
     BRIEF DESCRIPTION OF THE DRAWING  
       [0011]      FIG. 1  is a schematic circuit diagram of a system for generating a ringing magnetic pulse for treating flowing liquid in accordance with the invention.  
         [0012]      FIG. 2  is an oscilloscope trace showing a single large ringing pulse according to the invention.  
         [0013]      FIG. 3  is an oscilloscope trace showing a “natural” ringing pulse followed by more than one large ringing pulse according to the invention.  
         [0014]      FIG. 4  is an oscilloscope trace showing a series of six full large ringing pulses according to the invention. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT  
       [0015]     With reference to the FIGURE, a system for generating a ringing magnetic pulse for treating flowing liquids in accordance with the present invention is indicated generally by the reference number  10 . The system  10  comprises an input power transformer  12  having first and second output terminals  14 ,  16 , a coil IS, an SCR  20 , a triac  22 , a MOSFET  24  serving as an electronically controlled switch, a current level switch  26 , a peak voltage detector  28 , and a programmable digital microcontroller  30 .  
         [0016]     It has been discovered that digital control systems for generating a ringing magnetic pulse can be modified in order to be of simpler construction and less expensive by substituting a single silicon controlled rectifier (SCR) switch for a MOSFET switch assembly. SCRs are available with higher current ratings and lower losses relative to MOSFETs, and a single device can easily handle the coil current. However, SCRs cannot be electronically turned off as a MOSFET can, so that the high voltage “ringing” pulse has to be produced some other way than by interrupting the coil current pulse, as will be explained more fully below.  
         [0017]     Referring again to the FIGURE, the coil  18 , having an inductance and a capacitance connected in parallel, has a first end coupled to the first terminal  14  of the transformer  12 . The illustrated capacitance can be and is herein taken to be comprised solely of the capacitance of the coil, but in some coils the stray capacitance may be supplemented by a discrete capacitor converted in parallel with the coil. The SCR  20  has a cathode coupled to a second end  31  of the coil  18 , and an anode coupled to the second output terminal  16  of the transformer  12 . As shown, the anode of the SCR  20  is coupled to electrical ground. The triac  22  serves as an SCR gate switch. As shown in the FIGURE, the triac  22  is an optically-coupled triac having a first terminal  32  coupled to the gate of the SCR  20  via a gate resistor  34 , and a second terminal  36  coupled to ground potential. The triac  22  further includes a light emitting diode (LED)  38  that when energized to emit light closes the gate switch to enable current flow between the first and second terminals  32 ,  36  of the triac  22 .  
         [0018]     The microcontroller  30  includes a first output  40  coupled to an anode of the LED  38  via a resistor  42 , a second output  44  coupled to the current level switch  26 , and a third output  46  coupled to the peak voltage detector  28 . The current level switch  26  includes a first output  48  coupled to the microcontroller  30 , and a second output  50  coupled to the gate of the MOSFET  24 . The peak voltage detector  28  includes an output  52  coupled to the microcontroller  30 . A digitally controlled current reference potentiometer  54  is coupled to an input of the current level switch  26 , and is adjustable by the microcontroller  30 . A digitally controlled voltage reference potentiometer  56  is coupled to the peak voltage detector  28 , and is adjustable by the microcontroller  30 .  
         [0019]     The MOSFET  24 , such as the illustrated n-channel IGFET with substrate tied to source, includes a source coupled to ground potential, and a drain coupled to the second end  31  of the coil  18  via a current sense resistor  58 . A high voltage Schottky diode  60  has an anode coupled to the second end  31  of the coil  18  and a cathode coupled to an input  62  of the peak voltage detector  28 .  
         [0020]     The system  10  is generally preferably mounted on a printed circuit board (not shown). However, two components are preferably external to the printed circuit board (PCB), namely, the coil  18  and the power transformer  12 . The transformer  12  provides a 50-60 Hz AC voltage to power the coil  18 . The main power component on the PCB is the SCR  20  which is preferably heat-sinked and which functions as a controllable diode. When an ordinary diode is forward-biased (anode voltage positive with respect to the cathode) it conducts current. When an SCR is forward-biased it will not conduct current unless the gate (control) lead is also forward-biased. Both an SCR and an ordinary diode will block current if they are reverse-biased.  
         [0021]     When the SCR gate lead is connected to its anode (via a resistor), the SCR will conduct current when the SCR anode is positive with respect to its cathode. This occurs during the negative voltage half-cycle (as referenced to the SCR anode which is considered to be circuit ground in the FIGURE). Since the coil  18  is predominantly inductive (with some small internal resistance) at 60 Hz, negative current will continue to flow for a large portion of the positive voltage half-cycle. When the current drops to zero, the SCR  20  will block positive current flow (from cathode to anode) as does a diode rectifier. When the SCR  20  turns off, the voltage across the SCR will jump to a positive level during the remainder of the positive voltage half-cycle. It is during this positive voltage period that the microcontroller  30  generates resonating current and voltage pulses within the coil  18 .  
         [0022]     A ringing voltage pulse across the coil  18  is created by first closing the MOSFET solid-state switch  24  for a brief period at any time during the positive voltage cycle when the SCR  20  is off. The MOSFET  24  is closed, or made to conduct, by applying a positive voltage to its control electrode or gate via the current level switch  26 . Positive current will build up in the coil  18  while the MOSFET  24  is closed (the rise time is determined by the value of the current sense resistor  58  and the inductance of the coil  18 ). When the current level reaches a designated trigger value, the MOSFET switch  24  is abruptly opened by the current level switch  26  (the current level switch removes the positive voltage from the gate of the MOSFET  24 , which causes the MOSFET to become non-conducting). The inductance and capacitance values of the coil  18  will determine the frequency of the resulting resonating current flow within the coil and the magnitude of the ringing voltage as viewed across the SCR  20 . The decay time of the ring is determined by the internal resistance of the coil  18 . Multiple ringing pulses can be generated during the positive voltage period (the number of which is primarily limited by the decay time of the coil resonance).  
         [0023]     The gate resistor  34  of the SCR  20  must be disconnected from the anode of the SCR during the positive voltage period to prevent the SCR from turning on when ringing pulses are generated—which would quickly terminate the ring. Multiple methods of switching the gate resistor  34  were tried (such as a MOSFET and a transistor, directly and optically coupled) all of which presented operational and performance problems. The best method for switching the gate resistor  34  was determined to be an optically-coupled triac (as shown in the FIGURE). The triac  22  need only be energized prior to the start of the negative voltage half-cycle. Once current starts to flow in the SCR  20 , the triac  22  can be de-energized. The SCR  20  will continue to conduct until current drops to zero and the cathode-to-anode voltage across the SCR is positive. Interestingly, a small ringing pulse in the coil  18  occurs when the SCR  20  switches off which is caused by the charge stored in the coil capacitance.  
         [0024]     The operation of the system  10  is primarily implemented using the programmable digital microcontroller  30  coupled to and aided by the peak voltage detector  28  and the current level switch  26 . The microcontroller  30  does not directly interface with the coil  18 , the SCR  20  and the MOSFET  24 —nor does the microcontroller directly view the coil voltage level. The coil voltage is presented to the current level switch  26  and the peak voltage detector  28  through the high voltage Schottky diode  60 . The current level switch  26  and the peak voltage detector  28  compare the incoming voltage level to a reference voltage level set by the digitally controlled potentiometers  54 ,  56 , respectively to determine its action.  
         [0025]     The primary function of the peak voltage detector  28  is to compare the level of the coil ringing voltage signal to the reference level set by the digital potentiometer  56  associated with the peak voltage detector. If the peak level exceeds the given reference level, the peak voltage detector  28  will store that event so that it can be later read by the microcontroller  30 . The stored event is cleared after it is read by the microcontroller  30 . The peak voltage detector  28  is used to determine that the peak voltage exceeds the minimum desired value and also that it does not exceed a maximum value. A secondary function of the peak voltage detector  28  is to determine the value of the transformer voltage on start-up. The microcontroller  30  needs to know the transformer voltage because the ring signal rides on top of the transformer voltage. The transformer voltage reading is added to the desired ring voltage level when the reference voltage is set.  
         [0026]     The current level switch  26  controls the MOSFET  24  used to generate the coil ringing pulse. The microcontroller  30  sends a trigger pulse to the current level switch  26  to initiate a ring. When triggered, the current level switch  26  raises the voltage on the gate lead of the MOSFET  24 , thereby turning it on. The “on” resistance of the MOSFET  24  is much less than the value of the current sense resistor  58 . The MOSFET  24  is held “on” until the voltage at the current sense resistor  58 —coil junction (the cathode of the SCR  20 ) exceeds the reference voltage set by the current reference potentiometer  54  associated with the current level switch  26 . The value of the resistor  58  and the reference voltage is not as important as ensuring that the current value at which the MOSFET  24  turns off is repeatable for a given potentiometer setting. The role of the microcontroller  30  is to adjust the potentiometer  54  of the current level switch  26  to achieve the desired voltage level for the coil “ring”.  
         [0027]     The overall operation of the microcontroller  30  is executed in software embedded within the microcontroller. The functions of that software program are now described. When the system  10  is first powered-up, the SCR  20  and the MOSFET  24  are both off (i.e. no current flows through the coil  18 ). The first task of the microcontroller  30  is to test for the presence of coil power voltage from the transformer  12 . This can be accomplished by setting the peak voltage detector  28  at a low level and monitoring the output. An alternative method is to monitor a tap provided in the current level switch  26  which reads zero when the coil voltage is negative and rises to +0.5V when the coil voltage goes positive. The microcontroller  30  waits until it observes two alternating 50-60 Hz power line voltage cycles before proceeding. When the AC coil voltage is detected, the microcontroller  30  will measure its peak level by monitoring the output of the peak voltage detector  28  while it raises the level of the voltage reference potentiometer  56 . The peak level reading is retained in the microcontroller  30  and used as an offset for adjusting the level of the generated ring pulses which ride on the coil power voltage.  
         [0028]     The next software task is to turn on the SCR  20  which is a periodic task occurring once per voltage cycle. Just before the end of the positive voltage period (the SCR anode-to-cathode voltage is negative during this “positive” period, as the SCR anode is used as the ground-reference), the SCR gate switch or triac  22  is turned on by powering its optically coupled LED  38 . When the negative voltage across the SCR  20  is approximately 2 volts, the SCR will begin to conduct current at which time power to the gate switch LED  38  is removed. The SCR  20  will remain latched on without the gate switch  22  being powered, until the SCR  20  current flow drops to zero.  
         [0029]     The ringing pulses are produced by a second periodic software task. This task waits until the SCR  20  turns off and a positive coil voltage is detected (which is a sharp jump nearly the height of the peak coil voltage). The task waits a few milliseconds to allow the small coil ring (which occurs when the SCR  20  turns off) to die out. To generate a high voltage ringing pulse the software sends a trigger signal to the current level switch  26 , which turns on the MOSFET  24 , allowing positive current flow to rise in the coil  18 . The task monitors the current level switch  26 , waiting for the current level switch to signal that the current level has risen to the trigger point and the MOSFET  24  has turned off. The task waits for a few milliseconds to ensure that the coil ring has died out before proceeding. As many as six ring pulses can be generated within the positive coil voltage period.  
         [0030]     During the negative voltage period, the microcontroller  30  determines if the peak voltage detector  28  has been triggered, which indicates that ringing signal exceeded the reference level set in the voltage reference potentiometer  56 . The voltage reference potentiometer  56  can be set to either the minimum or the maximum desired peak voltage level. If the voltage reference potentiometer  56  is set for the minimum peak voltage, and the peak voltage detector  28  has not been triggered, the microcontroller  30  will increase the level of the current reference potentiometer  54  and leave the voltage reference potentiometer  56  at the minimum level. If the voltage reference potentiometer  56  is set for the minimum peak voltage, and the peak voltage detector  28  has been triggered, the microcontroller  30  will hold the level of the current reference potentiometer  54  and change the voltage reference potentiometer  56  to the maximum level. If the voltage reference potentiometer  56  is set to the maximum level, and the peak voltage detector  28  has been triggered, the microcontroller  30  will decrease the level of the current reference potentiometer  54  and leave the voltage reference potentiometer  56  at the maximum level. If the voltage reference potentiometer  56  is set to the maximum level, and the peak voltage detector  28  has not been triggered, the microcontroller  30  will hold the level of the current reference potentiometer  54  and change the voltage reference potentiometer  56  to the minimum level. The preceding actions will move and hold the peak voltage level for the ring pulse between the minimum and maximum desired values. The above logic pattern serves as a digital voltage regulator for the ringing voltage pulse.  
         [0031]     Also during the negative voltage period, the microcontroller  30  reads the resistance value of a negative temperature coefficient (NTC) thermistor (not shown) affixed to the heat sink of the SCR  20 . If the resistance drops below the value equated to the maximum temperature designated for the SCR heat sink (which is lower than destruction level for the SCR  20 ) the microcontroller  30  will turn off the SCR and also cease generating ringing pulses. The microcontroller  30  will continue to periodically read the thermistor and when it is determined that the SCR temperature has dropped to a safe level, the microcontroller will automatically resume operation.  
         [0032]     On the bottom of the printed circuit board can be two status LEDs (not shown)—preferably one red and one green—viewable through holes in a controller cover. The green LED is lit when the microcontroller  30  has determined that the voltage level of the ringing pulses is within the desired range, otherwise the red LED is lit. A single-pole double-throw relay contact (not shown) is preferably provided for remotely monitoring the status—when the green LED is lit the relay is energized.  
         [0033]     The functioning of the above-described SCR-switched circuit is as follows:  
         [0034]     The SCR (Silicon Controlled Rectifier) acts like a diode with a controllable turn-on capability. When voltage is applied in the “forward direction” (forward-biased-anode positive with respect to cathode) a diode will conduct current. However, the SCR will NOT conduct when forward-biased unless a current is made to flow in its “gate” circuit. If no gate current is applied, the SCR will “block” the flow of current even when forward-biased. Both the SCR and the diode will block the flow of current when the direction of current flow reverses (cathode to anode is the reverse-current direction). The SCR cannot be turned off by removing its gate current after it has been turned on. It can only be turned off by reversing the direction of current flow. In this it acts the same as a silicon diode (rectifier). Hence its name, “silicon controlled rectifier”.  
         [0035]     With this as background, a normal cycle of the Dolphin proceeds as follows. The coil, transformer and SCR switch are all connected in series. When the time-varying (50 or 60 cycles per second) transformer voltage applies a forward bias to the SCR, gate current is applied and the SCR conducts current through the coil. The SCR has a very low voltage drop from anode to cathode when conducting (less than or equal to one volt typically) so it acts like an almost-perfect switch. On the circuit boards of prior devices MOSFETs (Metal-Oxide-Silicon Field Effect Transistors) are used as the switch, and these MOSFETs have a larger “forward” voltage drop than does an SCR and so dissipate more heat than the SCR. For this reason, in the prior devices ten parallel-connected MOSFETs are used to carry the coil current, where a single SCR will do the same job in devices according to the present invention with lower overall power loss.  
         [0036]     When the coil current attempts to reverse direction, the SCR turns off and allows voltage to rise across it, just as a diode would do. The SCR then blocks current flow when the current reverses. Because the voltage and current across the coil are almost 90 degrees out of phase with each other, the current crosses zero (reverses) when there is still substantial voltage across the coil. This frees the coil to “ring” at a low voltage level due to the energy stored in its stray capacitance.  
         [0037]     After this initial small or natural “ringing” pulse has died out, a small current is allowed to build up in the coil by closing a MOSFET switch. This switch does not carry the main coil current, so a small switch can be used for this “recharging” function.  
         [0038]     When this current has reached a preset level, the MOSFET is turned off, and the coil voltage “rings” again, this time producing a large ringing pulse at a higher voltage level, depending on the amount of current that is allowed to build up.  
         [0039]     The regulator circuit measures the peak value of this “ringing” voltage and compares it to the desired value, which is stored as a number in the microprocessor “chip” on the circuit board. If the voltage is too low, then after the ringing pulse has died away the microprocessor turns the MOSFET on again and holds it “on” for a longer time, allowing more coil current to build up than before. The MOSFET is then turned off, and the large ringing pulse repeats.  
         [0040]     If the pulse voltage is too high, the microprocessor reduces the “on time” of the MOSFET switch for the next pulse, causing less coil current to build up. The MOSFET then turns off and the ringing voltage is again measured.  
         [0041]     When the ringing voltage has reached the desired level (it falls within a “window” range of voltages stored in the microprocessor), the regulator “remembers” this and fixes the MOSFET “on” time for subsequent pulses at this value unless the pulse voltage drifts outside the “window” again. This can occur if the coil resistance changes as the coil temperature changes during operation. If that occurs, preceding steps are repeated until the voltage is once again within the “window”.  
         [0042]     All the large “ringing” pulses are generated during the interval when the SCR switch is reverse-biased by the applied circuit voltage from the power transformer. The SCR allows the ringing pulses to occur (its gate current is zero during this interval), even though the ringing pulse voltage will at times cause the SCR voltage to switch over to the “forward” bias condition. The SCR will not turn on when this occurs, unlike a diode, as its gate current is held to zero by the gate driver switch. A diode switch could not be used as it would conduct and destroy the “ringing” pulses.  
         [0043]     Several large ringing pulses can be inserted in this reverse-bias time interval. If more voltage is desired, the “voltage window” numbers stored in the microprocessor are increased. The regulator then operates as above to force the voltage upward. More time is then required to “charge” the coil with current so fewer pulses can be generated in the interval; and vice versa.  
         [0044]     Other techniques can be used to generate ringing pulses similar to those described above. The preferred technique, as described above, uses the coil&#39;s inductance as an energy storage element to generate the ringing voltage, so it is a simpler method than others which must store the energy elsewhere. However, any device that stores the required pulse energy can be used to generate a ringing pulse. For example, a capacitor can be charged to 150 volts (or any other desired voltage) and switched across the coil during the “off time” of the coil current. This too will generate a ringing pulse, but it requires a high voltage power supply and an extra capacitor. This method also increases the capacitance in the “ringing” circuit, and causes a lower “ringing” frequency than our method does. The preferred method uses the unavoidable “stray” capacitance of the coil as the resonating capacitance, and generates the highest possible ringing frequency.  
         [0045]     A session testing the performance of a device such as shown by  FIG. 1  and as described above with a digital scope on a workbench produced the results shown in  FIGS. 2, 3  and  4 . As can be seen, the inventive control circuit can fit several (in this case six) large ringing pulses into the available “off” time window between transformer current pulses. The number of large ringing pulses is selectable by inputting a number to the control program via the computer programming interface.  
         [0046]      FIG. 2  shows a single pulse from the group; the printing at the left indicates the two horizontal cursor lines (white) were 208 volts apart. The sweep speed is 100 μs/division. The voltage scale is 50V/division.  
         [0047]     In  FIG. 3  is seen the first “natural” ring when the SCR turns off, about 75 volts peak-to-peak. Then come the large rings caused by the control circuit which large ringing pulses are between three and four times larger in voltage than the small “natural” ringing pulse. Note, there is more than one large ringing pulse visible in  FIG. 3 . The sweep speed here is 200 μs/division and the voltage scale is 50V/division.  
         [0048]     Finally, in  FIG. 4  we see a full six large ringing pulses. These fit into the approximately 8 millisecond “SCR off” time for this size (one inch) device. With larger coils, this time may be shorter and fewer pulses will fit in. The sweep speed here is 2 ms/division and the voltage scale is 50V/division.  
         [0049]     In summary, the system and method embodying the present invention employs an SCR for handling the main coil current and uses a single MOSFET switch to draw a relatively small current through the current coil(s) after the main current pulse has ended. One or more large ringing pulse or pulses is then produced by turning this switch off. Several ringing pulses can be produced in this way during the zero current interval through the coils, and the production of up to six pulses has been achieved.  
         [0050]     As will be recognized by those of ordinary skill in the pertinent art, numerous modifications and substitutions may be made to the above-described embodiment of the present invention without departing from the scope of the invention. Accordingly, the preceding portion of this specification is to be taken in an illustrative, as opposed to a limiting sense.