GB2296348A - Direct current resistance welding machine - Google Patents
Direct current resistance welding machine Download PDFInfo
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- GB2296348A GB2296348A GB9602165A GB9602165A GB2296348A GB 2296348 A GB2296348 A GB 2296348A GB 9602165 A GB9602165 A GB 9602165A GB 9602165 A GB9602165 A GB 9602165A GB 2296348 A GB2296348 A GB 2296348A
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- primary current
- welding
- current
- upper limit
- limit frequency
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- G—PHYSICS
- G09—EDUCATION; CRYPTOGRAPHY; DISPLAY; ADVERTISING; SEALS
- G09F—DISPLAYING; ADVERTISING; SIGNS; LABELS OR NAME-PLATES; SEALS
- G09F27/00—Combined visual and audible advertising or displaying, e.g. for public address
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K11/00—Resistance welding; Severing by resistance heating
- B23K11/24—Electric supply or control circuits therefor
- B23K11/25—Monitoring devices
- B23K11/252—Monitoring devices using digital means
- B23K11/257—Monitoring devices using digital means the measured parameter being an electrical current
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- Mechanical Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Theoretical Computer Science (AREA)
- Generation Of Surge Voltage And Current (AREA)
Abstract
A direct current resitance welding machine for controlling a primary current with an inverter having switching devices driven by pulses, comprising: a welding transformer fabricated by setting an upper limit frequency of the primary current supplied to the welding transformer based on the amount of change in primary current per unit time during either the rise or fall of said primary current, and on the turn ratio of the primary and secondary windings of the transformer, and having a cross-sectional area of the iron core of the transformer selected based on said set upper limit frequency. <IMAGE>
Description
DIRECT CURRENT RESISTANCE WELDING MACHINE
This invention relates to a direct current resistance
welding machine.
This application is divided from UK Patent Application No.
9311765.3 which discloses a method of controlling a direct current resistance welding machine, comprising: ~ a first step of detecting the primary current of a welding transformer coupled to an inverter having a plurality of switching devices controlled by corresponding pulses having a predetermined frequency and a time width corresponding to the value of the desired secondary current;
a second step of detecting rise and fall times of said detected primary current; and
a third step of computing an upper limit frequency of the primary current based on said time width and said rise and fall times,
whereby the primary current of said welding transformer is controlled by controlling said switching devices based on pulses having a frequency falling within said upper limit frequency;
and a diret current resistance welding machine,
comprising::
an inverter having a plurality of switching devices
controlled by corresponding pulses having a predetermined
frequency and each said pulse having a time width
corresponding to the value of the desired secondary current;
detecting means for detecting the primary current of a welding transformer coupled to said inverter;
differentiating means for differentiatIng said detected primary current;
first and second comparing means for comparing the level of an output produced from said differentiating means with a first predetermined level and for comparing the level of said output with a second predetermined level respectively;
first and second measuring means for measuring output producing periods of said first and second comparing means respectively; and
computing means for computing an upper limit frequency of the primary current of said welding transformer based on the periods measured by said first and second measuring means and said time width,
whereby the frequency of the primary current of said welding transformer is controlled by controlling saint switching devices based on pulses having a within said upper limit frequency.
Varying the frequency of a primary current in the welding transformer according to variations in a load on the secondary side, in an inverter-type,direct current resistance welder or welding machine, has been disclosed in
Japanese Patent Application Laid-Open Publication No. 63273575.In such an inverter-type direct current resistance welding machine, the welding transformer is controlled within a range of the frequency at which the iron core of the welding transformer is magnetically unsaturated, by supplying a primary current of a high frequency when the value for setting a welding current is small or, supplying a primary current of a low frequency when the welding current setting value is large
When the conventional control such as slow-up control for successively increasing the welding current at the beginning of energization, waveform control effected for the duration of energization, etc. is effected, the frequency of the primary current varies each time according to the state of the load on the secondary side. The frequency of the primary current of the welding transformer thus cannot be accurately set up.
Therefore, an operator usually made combinations of test pieces and their corresponding welding guns and measures welding conditions including the frequency of the primary current. Further, the operator inputted the measured welding conditions to a control unit in advance.
Then, the operator specified the welding conditions which had been inputted in advance based on the objects to be welded and the welding gun to be used before welding.
Thereafter, the welding was carried out under the specified welding conditions. Complex welding conditions such as slow-up control, waveform control, etc., required much time to determine.
According to the inverter type-direct current resistance welding machine, it has been known that the iron core of the welding transformer can be reduced in sectional area by increasing the frequency of the primary current, thereby making it possible to reduce the welding transformer in size and weight.
In the method of reducing the welding transformer in size by increasing the frequency of the primary current, however, an output voltage V0 is greatly reduced at a predetermined frequency, e.g., 1 kHz or higher according to time intervals required for the primary current of the welding transformer te rlse and fall. Thus, even if the welding transformer is reduced in size by simply increasing the frequency, the desired output cannot be obtained.
It is an aim of the present invention to provide a direct current resistance welding machine for previously computing an upper limit frequency of a primary current for obtaining a welding current required for a load on the secondary side and controlling the primary current within the range of the computed upper limit frequency and to provide a method of controlling the direct current resistance welding machine.
It is another al.m of the present invention to provide a direct current resistance welding machine having a small-sized, light and high efficiency welding transformer, fabricated based on the correlation between the ratio of the number of turns in the primary winding to the number of turns in the secondary winding and the amount of change in primary current, which appear during rise and fall times of a primary current.
Accordingly, the present invention provides a direct current resistance welding machine for controlling a primary current with an inverter comprised of switching devices driven by pulses, which comprises:
a welding transformer fabricated by setting an upper limit frequency of the primary Current supplied to the welding transformer based on the amount of change in primary current per unit time, which appears during either one of rise and fall times of the controlled primary current and the ratio of the number of turns in the primary winding to the number of turns in the secondary winding of the welding transformer and by determining a sectional area of an iron core selected based on the set upper limit frequency.
According to the method of controlling the direct current resistance welding machine of the present invention, the primary current of the welding transformer at the time that the switching devices of the inverter are controlled based on the corresponding pulses having the predetermined frequency and each having the time width corresponding to the value of the required secondary current is detected in the first step. Further, the rise and fall times of the detected primary current are detected in the second step.
Moreover, the upper limit frequency of the primary current is computed based on the time width of each pulse referred to above and the rise and fall times in the third step.
Thus, the primary current of the welding transformer is controlled by controlling the switching devices based on the pulses having the frequency which falls within the upper limit frequency of the primary current of the welding transformer.
According to the direct current resistance welding machine of the present invention, the primary current of the welding transformer at the time that the switching devices of the inverter are controlled based on the corresponding pulses having the predetermined frequency and each having the time width corresponding to the value of the required secondary current, is detected by the detecting means.
Then, the detected primary current of the welding transformer is differentiated by the differentiating means.
The level cf the differentiated output produced by the differentiating means and the first and second predetermined levels are respectively compared by the first and second comparing means. Thus, a rise time of the primary current of the welding transformer is detected by the first comparing means and a fall time of the primary current thereof is detected by the second comparing means.
Further, the rise time of the primary current of the welding transformer is measured by the first measuring means, whereas the fall time of the primary current thereof is measured by the second measuring means. Based on the measured rise and fall times and the pulse time width, the upper limit frequency of the primary current of the welding transformer is computed by the computing means. Thus, the frequency of the primary current of the welding transformer is controlled by controlling the switching devices based on the pulses having the frequency falling within the upper limit frequency which has been computed by the computing means.
Furthermore, the direct current resistance welding machine of the present invention has the welding transformer fabricated based on the value obtained by determining the upper limit frequency of the pulse-shaped primary current supplied to the welding transformer by the relationship between the amount of change in primary current per unit time, which occurs during either one of the rise and fall times of the primary current and the primary-to-secondary turns ratio of the welding transformer, and the value obtained by determining the sectional area of the iron core of the welding transformer based on the determined upper limit frequency.
An embodiment of the present invention will now be described hereinbelow with reference to the accompanying drawings, in which:
FIG. 1 is a block diagram showing the structure of an inverter type direct current resistance welding machine to which one embodiment of the present invention has been applied;
FIG. 2 is a timing chart describing the operation of a
PWM modulator employed in the inverter type direct current resistance welding machine shown in FIG. 1;
FIG. 3 is a timing chart describing the relationship between PWM modulated outputs and the waveform of a primary current of a welding transformer both produced in the embodiment of the present invention;
FIG. 4 is a chart describing respective waveforms of outputs produced from a differentiating circuit and comparators both employed in the embodiment of the present invention;;
FIG. 5 is a flowchart describing an upper limit frequency computing routine executed in the embodiment of the present invention;
FIG. 6 is a timing chart describing the computation of an upper limit frequency of the primary current flowing in the welding transformer employed in the embodiment of the present invention;
FIG. 7 is a graph describing the relationship between the turn ratio of the welding transformer and the amount of change in the primary current flowing, in the welding transformer;
FIG. 8 is a graph describing the relationship between the upper limit frequency of the primary current and the sectional area of an iron core of the welding transformer; and
FIG. 9 is a graph describing the relationship of the turn ratio of the welding transformer, the upper limit frequency of the primary current and the weight of the welding transformer.
A direct current resistance welder or welding machine and a method of controlling the direct current resistance welding machine, according to the present invention will be described in detail with reference to the accompanying drawings in which a preferred embodiments is shown by way of illustrative example, in connection with a system for effecting the above method.
FIG. 1 is a block diagram showing the structure of an inverter type direct current resistance welding machine 10 to which one embodiment of the present invention has been applied.
In machine 10, a rectifying circuit 12 converts electric power represented in the form of alternating current, i.e., alternating-current power which has been supplied from an alternating-current power source 11, into direct current. Then, an inverter 13 comprised of switching devices S1 through S4 such as transistors, converts the electric power outputted by the rectifying circuit 12 into alternating-current power. Thereafter, the inverter 13 supplies a primary current to a welding transformer 14.
Further, a full-wave rectifier 15 effects full-wave rectification on a secondary current in the welding transformer 14 and supplies the resultant current to a welding gun '16 so that objects 17 to be welded are subjected to resistance welding.
Further, a current detecting coil 18 detects the - primary current flowing in the welding transformer 14.
Then, a rectifying circuit 19 effects full-wave rectification on the detected primary current. Thereafter, an A/D converter 20 converts the rectified output into digital data. On the other hand, a current detecting coil 21 detects the secondary current flowing in the welding transformer 14 and a smoothing circuit 22 smooths the detected secondary current. Thereafter, an A/D converter 23 converts the smoothed output into digital data.
To compute an upper limit frequency f to be described later, machine 10 supplies the output of the rectifying circuit 19 to a differentiating circuit 24 where the output is differentiated. In addition, machine 10 causes a comparator 26 to compare the level of a first set output produced from a level setter 25 and the level of an output produced by the differentiating circuit i4. Then, machine 10 causes a comparator 27 to compare the level of a second set output produced by the level setter 25 and the level of an output produced by the differentiating circuit 24.
Further, machine 10 causes a counter circuit 29 to count the number of clock pulses outputted by a clock pulse generator 28 during a period in which the output of the comparator 26 is being generated. Moreover, machine 10 causes a counter circuit 30 to count the number of the clock pulses generated by the clock pulse generator 28 during a period in which the output of the comparator 27 is being produced. Thereafter, machine 10 supplies the counts of the counter circuits 29 and 30 to a control device 31 to be described later, thereby computing the upper limit frequency f,. Now, the frequency of the clock pulses generated by the clock pulse generator 28 is set up based on the output of the control device 31.
The control device 31 is functionally provided with a welding current controlling means for effecting slow-up control for on-off controlling the switching devices S1 through S4 in response to the outputs of the A/D converters 20 and 23 thereby to effect slow-up control for slowly increasing the secondary current of the welding transformer 14 based on welding conditions, and waveform control for controlling the waveform of current flowing during energization, for example, and an upper limit frequency computing means for computing the upper limit frequency fflAx.
Further, the control device 31 also has a central processing unit ("CPU") 32, a ROM 33 having programs stored therein for effecting processes such as an upper limit frequency computation and the welding current control as well as having data corresponding to an ON period TN of the switching devices, which is associated with the required secondary current, a RAM 34 having data storage areas in addition to working areas, and an input/output ("-I/O") port 35. The control device 31 effects predetermined control based on information inputted from an input device 36, which is indicative of a combination of the welding guns 16 and the objects 17 to be welded, information about the instruction for the measurement of the upper limit frequency, etc.
Furthermore, the machine 10 also has a PWM modulator 37 for generating both a PWM modulated output and a PWM modulated output adjusted so as to have a phase shift of 1800 with respect to the former PWM modulated output in response to switching device control data and a frequency setting timing pulse both outputted by control device 31.
Drivers 38 and 39 respectively amplify the modulated outputs produced by the PWM modulator 37 and respectively effect the
ON-OFF control of the switching devices S1 through S4 based on the amplified outputs.
As is known, the PWM modulator 37 causes a D/A converter 40 to convert the switching device control data outputted by the control device 31 into an analog signal.
In response to the frequency setting timing pulse outputted by the control device 31, the PWM modulator 37 causes a oneshot multivibrator 41 to generate a timing pulse and causes a sawtooth generator 42 inputted with the timing pulse to generate a sawtooth output synchronized with the timing pulse. Further, the PWM modulator 37 causes a comparator 43 to compare the level of the analog signal converted by the
D/A converter 40 and the level of the sawtooth output generated by the sawtooth generator 42, and allows the comparator 43 to produce a PWM modulated output based on the result of comparison.Then, the PWM modulator 37 causes a two-phase pulse generator 44 to make a 1800 phase shift with respect to the input PWM modulated output and supplies a PWM modulated output which is a o e phase shift, i.e., in phase with the input supplied by the comparator 43, and a PWM modulated output 180 out of phase with the input, to their corresponding drivers 38 and 39.
In machine 10 constructed as described above, an operator fits the objects 17 to the welding guns 16 as test pieces for the computation of the upper limit frequency.
Further, the operator inputs an instruction for the combination of the test pieces and the welding gun 16 and an instruction for computing the upper limit frequency using the input device 36. The operation of machine 10 for controlling the secondary current based on the input instructions will be described next.
Data about the value of the required secondary current to be outputted to the objects 17 used as the test pieces by the welding transformer 14, is read from ROM 33 based on the above instructions. Further, both a timing pulse based on the read data and switching device control data synchronized with the timing pulse are outputted by the control device 31. The one-shot multivibrator 41 supplied with the timing pulse outputs a train of pulses (FIG. 2 line (a)) in synchrony with the timing pulse. The sawtooth generator 42 outputs a sawtooth wave (FIG. 2 line (b)) based on the train of pulses outputted by the one-shot multivibrator 41.
On the other hand, the D/A converter 40 supplied with the switching device control data produces an analog signal (FIG. 2 line (c)) in synchrony with the timing pulse. - Then, the comparator 43 compares the level of the sawtooth wave (FIG. 2 line (b)) outputted by the sawtooth generator 42 and the level of the converted signal outputted by the D/A converter 40 (FIG. 2 line (c)) outputted by the D/A converter 40. During the period in which the level of the sawtooth wave is less than or equal to the level of the converted signal, the comparator 43 produces a PWM modulated output a (FIG. 2 line (d)) having a duty ratio obtained based on the cycle or period of the sawtooth wave and the level of the converted signal.In response to the PWM modulated output a supplied by the comparator 43, the twophase pulse generator 44 re-generates or passes through the
PWM modulated output a, and also generates a PWM modulated output b (FIG. 2 line (e)), which is produced by making a 1800 phase shift with respect to the PWM modulated output a.
Then, the PWM modulated output a produced by the twophase pulse generator 44, is amplified by the driver 38 from which the amplified output is applied to the switching devices S1 and S4, with the result that they are maintained in an ON condition during the period of generation of the
PWM modulated output a.
On the other hand, the PWM modulated output b produced by the two-phase pulse generator 44 is amplified by the driver 39 from which the amplified output is supplied to the switching devices S2 and S3, with the result that they are maintained in an ON condition during the period of generation of the PWM modulated output .
A secondary current of the welding transformer 14 is produced in response to the primary current (having the waveform of FIG. 3 line (b)) and flows in the objects 17 used as the test pieces through the welding gun 16, thus joining the objects 17 to each other by resistance welding.
It is known that the pulse width of each of the PWM modulated outputs a and b is controlled so as to be brought into the required or desired secondary current in this way.
The waveforms of the PWM modulated outputs a and b are illustrated in FIG. 3, line (a).
As is also apparent from FIG. 3 line (b), the primary current of the welding transformer 14 is represented in the form of a waveform changed in the following manner. For example, the PWM modulated output a abruptly rises from the leading edge thereof. After the PWM modulated output a has reached a substantially constant level, it rapidly falls from the trailing edge thereof. The primary current has a rise period, i.e., a rise time TH, a substantially constant time T1 and a fall time TL. TS (= Th + T1) is the width of the PWM modulated wave.
In the case of the PWM modulated output b, a primary current having a waveform identical (but having the opposite sign) to that of the primary current based on the PWM modulated output a, flows in the welding transformer 14.
Now, the rise time TH and the fall time TL of the primary current are substantially determined by the primary resistance and inductance of the welding transformer 14 and the required secondary current. Further, the time TN is decided by the required secondary current. Therefore, these times cannot be set to "O".
However, a time Tu provided between the primary current based on the PWM modulated signal or output a and the primary current based on the PWM modulated signal or output b can be shortened. Hence the upper limit frequency f is decided by setting the time T, to "O".
The primary current is detected by the current detecting coil 18. The detected primary current is subjected to full-wave rectification by the rectifying circuit 19, and the rectified output is differentiated by the differentiating circuit 24. The waveform of the output produced by the rectifying circuit 19 is shown in FIG. 4, line (a). Waveform 1 in FIG. 4 line (a) corresponds to the primary current based on the PWM modulated output a and waveform 2 in FIG. 4 line (a) corresponds to the primary current based on the PWM modulated output k The waveform of the differentiated output produced by the differentiating circuit 24 is illustrated in FIG. 4 line (b).
The comparator 26 compares the level of the differentiated output produced by the differentiating circuit 24 and the level (see level 3 in FIG. 4 line (b)) of the first set output produced by the level setter 25. The result of'comparison of the comparator 26 is represented as an output shown in FIG. 4 line (c). The comparator 27 compares the level of the differentiated output and the level (see level 4 in FIG. 4 line (b)) of the second set output produced by the level setter 25. The result of comparison of the comparator 27 is represented as an output shown in FIG. 4 line (d).
During the period in which output is being generated by the comparator 26 (in response to output a or b), the counter circuit 29 counts the clock pulses inputted by the clock pulse generator 28. Thus, the count of the counter circuit 29 corresponds to the rise time TM. During the period in which output is being generated by the comparator 27, the counter circuit 30 counts the clock pulses inputted by the clock pulse generator 28. Accordingly, the count of the counter circuit 30 corresponds to the fall time TL. The accuracy of counting of the pulses during the rise and fall times TN and T L depends on the frequency of the clock pulses generated by the clock pulse generator 28.
Since the instruction for the computation of the upper limit frequency has been inputted through the input device 36 by the operator, an upper limit frequency computing routine shown in a flowchart in FIG. 5 is next executed.
When the upper limit frequency computing routine is executed, the frequency of the clock pulses generated by the clock pulse generator 28 is established (Step Sol). Next, the control of the secondary current is started in accordance with a PWM modulated output based on the characteristic frequency f0 of the transformer 14 (Step S2), where f0 = (El/N)/(4-Ae-Bm), El is maximum primary voltage,
N is the turn ratio, Ae is the cross-sectional area of the core, and Bm is the magnetic flux density of the core.Then the pulse width of each of the PWM modulated outputs a and b, (that is, the duty ratio) is controlled until the value of the secondary current reaches a target secondary-current value inputted through the input device 36, which is associated with the welding gun and the test pieces (Step
S3). Control is effected by control device 31 in feedback relationship with secondary current detector 21, etc.
When the value of the secondary current has reached the target secondary-current value in Step S3, the counter circuits 29 and 30 are cleared (Step S4). Then, the time TN is stored as data in the RAM 34 (Step S5). During the continuation of the control in Step S3, the counts of the counter circuits 29 and 30 are read as described above (Step
S6). After the reading of the counts has been made, the upper limit frequency fMAX is repeatedly computed n times (Steps S7 and S8).
The upper limit frequency f is computed by the equation, fMAX S C1 - 2fo(TpW - TN))/t2(Th + TL)), derived as follows with reference to FIG. 6.
The period corresponding to half the frequency f0 (i.e.
1/(2fo)), is represented as (Th + T1 + TL + TU) (see FIG. 6 line (a)). The period corresponding to half the upper limit frequency fMAX (i.e. l/(2f )) is represented as (TH + TIA +
TL) (see FIG. 6 line (c)); or rewritten as TIA = {1/(2fMAX)} (Tx + TL).
The current which flows in a load, is determined by secondary voltage of the welding transformer. The secondary voltage is substantially outputted only for either a time T1 (the general case) or TIA (the maximum frequency case) during which the primary current flows. If V2P is the peak secondary voltage, then the average secondary voltage V2AVG of pulse-shaped secondary voltages at the frequency f0 is determined by the equation, V2AVG = {T1/2(fo)} x V2p.When the same average secondary voltage V2AVG is obtained at the upper limit frequency f, then V > vc = fT1A/(2fMAx)) x V2P, from which it follows that TI/{1/(2fo)} = TIA/{1/(2fMAX)}. This can be rewritten as TIA = (fo/fMAX)TI, or TIA = (fo/fMAX) (.Tpw - Tx), with reference to FIG. 6 line (c). Combining with the definition of TXA , above, results in: {1/(2fMAX)} - (TH + TL) = (fo/fMAX) (TPW - TH). Solving for fMAX, the desired formula is arrived at.
When the upper limit frequency fMAX is computed n times in Step S8, the arithmetic mean or average of the upper limit frequencies f, is computed (Step S9), and stored in
RAM 34 as data (Step S10). Then, control for a target secondary current is continuously effected for a predetermined period of time at the averaged f, and then the routine is completed (Steps Sli and S12).
According to the present invention, as has been described above, the required secondary current is supplied to the test piece. At this time, the upper limit frequency fMAX of the primary current supplied to the welding trans former 14 is computed based on the times T, and TL required for the primary current of the welding transformer 14 to rise and fall, and the time TN determined by the desired secondary current. Upon welding, the switching devices are controlled based on a train of pulses whose frequency falls within the upper limit frequency fz. Thus, the control for the primary current supplied to the welding transformer 14 can be accurately effected.
The upper limit frequency fMAX corresponding to the necessary secondary current is computed and stored each time objects to be welded and their corresponding welding guns are combined. By doing so, the setting of the upper limit frequency f can be omitted from a welding system which makes it necessary to set complex welding conditions. It is thus possible to shorten the time required to search and set the welding conditions.
Sometimes, the secondary current produced by supplying the primary current (whose upper limit frequency is fJ) to the welding transformer, is insufficient for some welding purposes. It is thus necessary to increase the upper limit of the frequency of the primary current and to design a welding transformer 14 capable of supplying the desired secondary current. A method for producing such a welding transformer 14 will be explained next.
The primary current in the form of a train of pulses has a rise time Tx and a fall time TL as described above.
The amount A t of change in the primary current (i.e., the primary current change rate, which occurs during either the rise time Tx or the fall time TL) is determined by both the primary resistance and the inductance of the welding transformer 14. Thus, when specifications such as a sectional area of the iron core of the welding transformer 14, the number of turns in the primary coil and the number of turns in the secondary coil are decided, A t becomes a constant value based on the specifications.Therefore, a welding transformer 14 of a type wherein the rise time TH and the fall time Tt have been shortened, can be produced to have an even higher upper limit frequency, fMAX
When the primary current flows in the welding transformer 14, an electromotive force V1 developed in the primary coil is determined by the following general equation, where 9 is the magnetic flux induced by the primary current, and N is the turn ratio: V1 = N (A/At).
When # = kNI1 is substituted, and k is a constant, then V1 = kN2 (A11/At), or rewritten, (A11/At) = Vl/(kN2).
This equation represents the relationship between N, the turn ratio, and AI1/At, the amount of change in primary current during either the rise time TH or the fall time TL of the primary current. Assuming constant k and constant
V1, then the current change rate #I1/#t with respect to the turn ratio N is determined by computation, as represented by curve (a) of FIG. 7.
When the computed primary current change rate #I1/#t with respect to the turn ratio N is compared with measured experimental values, represented by FIG. 7 curve (b), a very satisfactory correlation is obtained therebetween. It is thus confirmed that the equation is sufficiently practical.
Further, the upper limit frequency fMAX is computed based on each primary current change rate AI1/At, thereby to determine the relationship between the upper limit frequency fMAX and the turn ratio N.
Noting that TH is approximately equal to TL, then from
FIG. 6 line (c), it is apparent that
duty = TIA / CTlA + 2.I1MAX/(#I1/#t)} = 2.TIA.fMAX or fMAX = 1/2.{TIA + 2.I1MAX/(#I1/#t)} The minimum turns ratio is NMIN = IZAVG/I1MAX, where I2AVG is the average secondary current, and I1MAX is the maximum primary current. V2AVG = V2p x duty -= (V,,,,/N,,,) x (2.TIA.fMAX) or duty = 2.TIA.fMAX = V2AVC x NMIN / V1PEAK.
Accordingly, the desired secondary voltage is a boundary condition of design.
With NMIN thus determined, #I1/#t can be determined, either from FIG. 7 curve (b) or FIG. 7 curve (a) (or its underlying equation). Thus fMAX is determined.
Next, the weight of the welding transformer 14 at each upper limit frequency fMAX is computed from the relationship between the upper limit frequency fMAX and the sectional area of the iron core, shown in FIG. 8. The relationships between each upper limit frequency fMAX and the weight of welding transformer 14, and between each upper limit frequency t and each turn ratio N are determined. These relationships are shown in FIG. 9.
Thus, when the upper limit frequency fMAX of the primary current is decided, both the turn ratio N and the weight of welding transformer 14 can be easily determined from FIG. 9.
FIG. 9 shows the relationship between each of turn ratios No - Na and the weight of the welding transformer i4 at the upper limit frequency fMAX when the capacity of the welding transformer 14 is 140 kVA, for example. If the upper limit frequency tfflu is set to about 3.8 kHz, for example, then the turn ratio N is N4, and the weight of the welding transformer 14 is about 55% of the conventional weight.
According to the present embodiment, as has been described above, the relationship between the primary current change rate A t and the turn ratio N is determined by paying attention to the close relationship between the primary current change rate #I/#t developed during each of the rise and fall times TH and TL of the primary current and the turn ratio N of the welding transformer 14. Further, the relationship between the upper limit frequency t and the turn ratio N, and the relationship between the upper limit frequency LIAX and the cross-sectional area of the iron core of the welding transformer 14 will be apparent by determining the upper limit frequency fMAX from the primary current change rate Al/At. Thus, a small-sized and light welding transformer operable at a desired upper limit - frequency t can be obtained.
Having now fully described the invention, it will be apparent to those skilled in the art that many changes and modifications can be made without departing from the scope of the invention as set forth herein.
Claims (3)
1. A direct current resitance welding machine for controlling a primary current with an inverter having switching devices driven by pulses, comprising:
a welding transformer fabricated by setting an upper limit frequency of the primary current supplied to the welding transformer based on the amount of change in primary current per unit time during either the rise or fall of said primary current, and on the turn ratio of the primary and secondary windings of the transformer, and having a cross-sectional area of the iron core of the transformer selected based on said set upper limit frequency.
2. A machine according to claim 1, wherein said amount of change in primary current is inversely proportional to the square of said turn ratio.
3. A direct current resistance welding machine for controlling a primary current substantially as hereinbefore described with reference to the accompanying drawings.
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4155011A JP2755524B2 (en) | 1992-06-15 | 1992-06-15 | Inverter type DC resistance welding equipment welding transformer |
JP24781892A JP2614690B2 (en) | 1992-09-17 | 1992-09-17 | Method and apparatus for controlling a welding transformer |
GB9311765A GB2267982B (en) | 1992-06-15 | 1993-06-08 | Direct current resistance welding machine and method of controlling the same |
Publications (3)
Publication Number | Publication Date |
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GB9602165D0 GB9602165D0 (en) | 1996-04-03 |
GB2296348A true GB2296348A (en) | 1996-06-26 |
GB2296348B GB2296348B (en) | 1996-09-25 |
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Application Number | Title | Priority Date | Filing Date |
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GB9602165A Expired - Fee Related GB2296348B (en) | 1992-06-15 | 1993-06-08 | Direct current resistance welding machine |
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Country | Link |
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GB (1) | GB2296348B (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0237861A2 (en) * | 1986-03-07 | 1987-09-23 | Kabushiki Kaisha Toshiba | Power converter |
-
1993
- 1993-06-08 GB GB9602165A patent/GB2296348B/en not_active Expired - Fee Related
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0237861A2 (en) * | 1986-03-07 | 1987-09-23 | Kabushiki Kaisha Toshiba | Power converter |
Also Published As
Publication number | Publication date |
---|---|
GB2296348B (en) | 1996-09-25 |
GB9602165D0 (en) | 1996-04-03 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 20090608 |