Background
An Oscilloscope (Oscilloscope) is an electronic measuring instrument with wide application, can convert an electric signal invisible to the naked eye into a visible image, and is convenient for people to research the change process of various electric phenomena.
In the process of utilizing an oscilloscope to evaluate the junction temperature of a power unit consisting of an Insulated Gate Bipolar Transistor (IGBT)/silicon carbide (SiC) semiconductor module, a driver, a thin film capacitor and a busbar, on-loss and off-loss parameters are calculated through double-pulse tests under multiple working conditions, and a thermal simulation model is extracted through a thermal simulation tool to obtain the junction temperature evaluation method. The turn-on loss and turn-off loss parameters are the integral of the current and voltage over a certain period of time. When the current waveform and the voltage waveform measured by the oscilloscope have phase difference, the obtained value has larger deviation with the true value, so that the junction temperature estimation is not true.
Disclosure of Invention
In order to solve the technical problem, the application provides a phase delay acquisition device and an acquisition method of an oscilloscope, so as to solve the problem that the error of a junction temperature evaluation result is large due to the phase delay of the oscilloscope.
In order to achieve the technical purpose, the embodiment of the application provides the following technical scheme:
an apparatus for acquiring a phase delay of an oscilloscope, comprising: the power supply, the first IGBT, the second IGBT, the first inductor and the second inductor; wherein the content of the first and second substances,
the power supply, the first inductor, the first IGBT and the second IGBT are connected in series;
two ends of the second inductor are respectively connected with the first end and the second end of the first IGBT;
the control end of the second IGBT is used for receiving a control signal, and the control signal comprises at least two pulse signals separated by preset time; the control end of the first IGBT is suspended;
the first end and the second end of the second IGBT are used for an oscilloscope to measure voltage signals, the second end of the second IGBT is used for the oscilloscope to measure current signals, and the voltage signals and the current signals obtained through measurement are used for calculating phase delays of the voltage signals and the current signals.
A phase delay obtaining method of an oscilloscope is realized based on any one of the phase delay obtaining devices of the oscilloscope, and the phase delay obtaining device of the oscilloscope comprises the following steps: the phase delay acquiring method of the oscilloscope comprises the following steps:
providing a control signal for a control end of the second IGBT, wherein the control signal comprises at least two pulse signals separated by preset time;
measuring a current signal of a second end of the second IGBT by using a current probe of an oscilloscope;
measuring voltage signals at two ends of the second IGBT by using a differential probe of an oscilloscope;
and calculating the phase delay of the voltage signal and the current signal according to the voltage signal and the current signal obtained by measurement.
Optionally, the calculating the phase delay of the voltage signal and the current signal according to the voltage signal and the current signal obtained by measurement includes:
intercepting a voltage signal and a current signal within a preset time period after the starting moment of a second pulse signal in the control signal to obtain a voltage waveform to be processed and a current waveform to be processed;
discretizing the current waveform to be processed, wherein the discretized current waveform to be processed comprises a plurality of discrete points;
obtaining a plurality of voltage drop process curves according to the first inductor and the discretized current waveform to be processed;
fitting the voltage drop process curve to obtain a voltage fitting curve;
determining a voltage fitting curve which is most similar to the voltage waveform to be processed from a plurality of voltage fitting curves;
and determining stray inductance and phase difference time according to the determined voltage fitting curve, wherein the phase difference time is the phase delay of the voltage signal and the current signal.
Optionally, the obtaining a plurality of voltage drop process curves according to the first inductor and the discretized current waveform to be processed includes:
dividing the first inductor into a plurality of inductor values within a preset inductor range according to a preset inductor step length;
according to the adjacent discrete points, determining the time interval and the current value interval of the adjacent discrete points;
and calculating to obtain the multiple voltage reduction process curves according to the multiple inductance values, the time intervals and the current value intervals of the adjacent discrete points.
Optionally, the obtaining, by calculation, the multiple voltage drop process curves according to the multiple inductance values and the time intervals and the current value intervals between adjacent discrete points includes:
substituting the plurality of inductance values, the time intervals and the current value intervals of the adjacent discrete points into a first preset formula to calculate and obtain a plurality of voltage reduction process curves;
the first preset formula includes:
(ii) a Wherein Vt represents the voltage drop process curve, Dt represents a time interval adjacent to the discrete point, Di represents a current value interval adjacent to the discrete point, and Ls represents the inductance value.
Optionally, the value of the preset inductance step length is one thousandth of the total length of the preset inductance range.
Optionally, the determining a voltage fitting curve that is closest to the voltage waveform to be processed from the plurality of voltage fitting curves includes:
determining the slope of each of the voltage fit curves;
and determining the voltage fitting curve with the smallest difference between the slope of the plurality of voltage fitting curves and the slope of the voltage waveform to be processed as the voltage fitting curve which is closest to the voltage waveform to be processed.
Optionally, the intercepting a voltage signal and a current signal within a preset time period after a start time of a second pulse signal in the control signal to obtain a to-be-processed voltage waveform and a to-be-processed current waveform includes:
and intercepting a voltage signal and a current signal in a preset time period after the start time of the second pulse signal in the control signal, and performing recursive mean filtering on the intercepted current signal and voltage signal to obtain a to-be-processed voltage waveform and a to-be-processed current waveform.
Optionally, the value range of the preset time includes 10 ± 5 μ s.
It can be seen from the above technical solutions that the present application provides a phase delay obtaining apparatus and a phase delay obtaining method for an oscilloscope, where the phase delay obtaining apparatus for an oscilloscope includes a power supply, a first IGBT, a second IGBT, a first inductor, and a second inductor, in a test process, a control terminal of the second IGBT receives at least two pulse signals with a preset interval, a control terminal of the first IGBT is suspended, when the second IGBT is turned on for the second time under the control of the control signal, a current flowing through the second IGBT starts to increase, but does not reach a rated current of a first terminal of the second IGBT, a body diode of the first IGBT is in a freewheeling state at this time, due to the existence of the first inductor, a gap may occur in a voltage signal measured by the oscilloscope, and a phase delay of the voltage signal and a phase delay of a current signal measured by the oscilloscope may be calculated according to the gap, the purpose of obtaining the phase delay of the oscilloscope is achieved, the whole device is achieved by utilizing the existing power unit, the cost is low, and the phase delay generated by selecting different oscilloscope channels can be compensated.
Detailed Description
As described in the background art, in the process of evaluating the junction temperature of the power unit, a phase difference may exist between a current waveform and a voltage waveform measured by an oscilloscope, so that a large deviation exists between a current value and a voltage value obtained and a real value, and the junction temperature estimation is not real.
To solve this problem, researchers in the related art have provided the following two solutions:
the first scheme is as follows:
referring to fig. 1 and 2, a square wave pulse passes through a 50 Ω resistor to GND by the input signal PWM _ IN 5V. The current probe of the oscilloscope is sleeved in the 5T ring to measure current, and the voltage probe of the oscilloscope is respectively clamped in the test points 1,2 and 3 and is used for measuring voltage with GND. The phase delays of the current and voltage square waves were then compared by an oscilloscope (see fig. 2, in fig. 2, V)PWM_INRepresenting the input signal waveform, H represents a high level, L represents a low level, V represents the oscilloscope-measured voltage waveform, and I represents the oscilloscope-measured current waveform).
However, because the current generated in the loop has a value of 100mA, the wide-range current probe cannot adopt the scheme to carry out phase difference correction.
Scheme II:
referring to fig. 3 and 4, fig. 3 (in fig. 3, V)DSRepresenting the voltage probe of an oscilloscope IDShowing a current probe of an oscilloscope) is a structural block diagram of a scheme 2, a signal PWM _ IN 15V square wave pulse is input, when the square wave pulse is at a high level, an MOS tube is conducted, and current is generated IN a loop, wherein the current probe is sleeved below a non-inductive resistance loop to measure the current flowing through the MOS tube, and a voltage probe is clamped between a drain electrode and a source electrode of the MOS tube to measure the voltage at two ends of the MOS tube. The phase delays of the current square wave and the voltage square wave were then compared by an oscilloscope (see fig. 4, in fig. 4, V)PWM_INRepresenting the waveform of an input signal, H representing high level, L representing low level, V representing the waveform of a voltage measured by an oscilloscope, and I representing the waveform of a current measured by the oscilloscope).
In view of this, an embodiment of the present application provides a phase delay acquiring apparatus for an oscilloscope, including: the power supply, the first IGBT, the second IGBT, the first inductor and the second inductor; wherein the content of the first and second substances,
the power supply, the first inductor, the first IGBT and the second IGBT are connected in series;
two ends of the second inductor are respectively connected with the first end and the second end of the first IGBT;
the control end of the second IGBT is used for receiving a control signal, and the control signal comprises at least two pulse signals separated by preset time; the control end of the first IGBT is suspended;
the first end and the second end of the second IGBT are used for an oscilloscope to measure voltage signals, the second end of the second IGBT is used for the oscilloscope to measure current signals, and the voltage signals and the current signals obtained through measurement are used for calculating phase delays of the voltage signals and the current signals.
The phase delay acquisition device of the oscilloscope comprises a power supply, a first IGBT, a second IGBT, a first inductor and a second inductor, in the test process, the control end of the second IGBT receives at least two pulse signals with preset time intervals, the control end of the first IGBT is suspended, when the second IGBT is turned on for the second time under the control of the control signal, the current flowing through the second IGBT starts to increase, but not reach the rated current of the first end of the second IGBT, at the moment, the body diode of the first IGBT is in a free-wheeling state, because of the existence of the first inductor, a gap appears on the voltage signal measured by the oscilloscope, the phase delay of the voltage signal and the current signal measured by the oscilloscope can be calculated and obtained according to the gap, the purpose of obtaining the phase delay of the oscilloscope is realized, the whole device is realized by using the existing power unit, the cost is low, and the phase delay generated by selecting different oscilloscope channels can be compensated.
The technical solutions in the embodiments of the present application will be clearly and completely described below with reference to the drawings in the embodiments of the present application, and it is obvious that the described embodiments are only a part of the embodiments of the present application, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present application.
The embodiment of the present application provides a phase delay obtaining apparatus of an oscilloscope, as shown in fig. 5, including: the power supply, the first IGBT, the second IGBT, the first inductor and the second inductor; wherein the content of the first and second substances,
the power supply, the first inductor, the first IGBT and the second IGBT are connected in series;
two ends of the second inductor are respectively connected with the first end and the second end of the first IGBT;
the control end of the second IGBT is used for receiving a control signal, and the control signal comprises at least two pulse signals separated by preset time; the control end of the first IGBT is suspended;
the first end and the second end of the second IGBT are used for an oscilloscope to measure voltage signals, the second end of the second IGBT is used for the oscilloscope to measure current signals, and the voltage signals and the current signals obtained through measurement are used for calculating phase delays of the voltage signals and the current signals.
Referring to fig. 6, fig. 6 is a timing diagram of the control signal, and in the test process, a second pulse signal of the control signal is mainly used, so that only two pulse signals are generally needed for one control period of the control signal, a feasible value of an interval time of the two pulse signals may be about 10 μ s, and in an embodiment of the present application, a value range of the preset time includes 10 ± 5 μ s.
Still referring to fig. 5, when the control signal is high, the second IGBT is turned on, and there are two loop currents in the entire loop, one being the loop current from the power supply through the first inductor, the second inductor, and the second IGBT (I1), and the other being the loop current from the second inductor through the body diode of the first IGBT (I2). In fig. 5, D1 denotes the body diode of the first IGBT, D2 denotes the body diode of the second IGBT, VCEIndicating oscilloscopeMeasure a voltage signal between the first and second terminals of the second IGBT, ICThe current probe representing the oscilloscope measures the current signal flowing through the second IGBT, T1 represents the first IGBT, T2 represents the second IGBT, L2 represents the second IGBTsRepresents the first inductance, LairRepresenting the second inductance.
The control terminals of the first IGBT and the second IGBT may refer to bases of the first IGBT and the second IGBT, and the first terminal and the second terminal of the first IGBT and the second IGBT refer to collectors and emitters of the first IGBT and the second IGBT, respectively.
The amplitude of the high level of the control signal is set in advance according to a set value.
The control end of the first IGBT is suspended, that is, the control end of the first IGBT does not apply any signal and keeps the first IGBT turned off. During the turn-on process of the second IGBT, the current flowing through the second IGBT starts to increase, but does not reach the rated current of the collector of the second IGBT, at which time the body diode of the first IGBT is in a freewheeling state, and the voltage of the collector and emitter of the first IGBT is zero. Due to the presence of the stray inductance of the commutation loop, i.e. the first inductance, the voltage between the collector and the emitter of the second IGBT will exhibit a notch Us as shown in fig. 7 and 8. In FIGS. 7 and 8, VPWM_INA waveform diagram showing the control signal, H denotes a high level, L denotes a low level, VCEA waveform representing the voltage signal ICThe waveforms representing the current signals, the waveforms of the control signals not being shown in fig. 8, and V not clearly shown in fig. 7GE,VGEA voltage waveform representing the control terminal of the second IGBT.
According to the gap Us, the phase delay of the current signal and the voltage signal measured by the oscilloscope can be obtained by utilizing a calculation method.
Specifically, the voltage signal and the current signal within a preset time period after the start time of the second pulse signal (i.e., the rising edge time of the second pulse signal) in the control signal are intercepted, and the intercepted signals are subjected to recursive mean filtering to smooth the waveform, so as to obtain the waveform of the voltage to be processed and the waveform of the current to be processed. The specific value of the preset time period is determined according to the size of the notch Us.
Dividing the first inductor into a plurality of inductor values within a preset inductor range according to a preset inductor step length; according to the adjacent discrete points, determining the time interval and the current value interval of the adjacent discrete points; substituting the plurality of inductance values, the time intervals and the current value intervals of the adjacent discrete points into a first preset formula to calculate and obtain a plurality of voltage reduction process curves;
the first preset formula includes:
(ii) a Wherein Vt represents the voltage drop process curve, Dt represents a time interval adjacent to the discrete point, Di represents a current value interval adjacent to the discrete point, and Ls represents the inductance value.
Optionally, the value of the preset inductance step length is one thousandth of the total length of the preset inductance range. That is, assuming that the preset inductance range is 0nH to 100nH, the total length of the preset inductance range is 100nH, the preset inductance step size is 0.1nH, and the preset inductance step size divides the preset inductance range into 1000 values. Meanwhile, when the current waveform to be processed is discretized, assuming that the phase difference is from-50 ns to 50ns, the discretization step length can also be selected to be 0.1ns, so that 1000 × 1000=1000K voltage drop process curves are obtained in total.
Optionally, the determining a voltage fitting curve that is closest to the voltage waveform to be processed from the plurality of voltage fitting curves includes:
determining the slope of each of the voltage fit curves;
and determining the voltage fitting curve with the smallest difference between the slope of the plurality of voltage fitting curves and the slope of the voltage waveform to be processed as the voltage fitting curve which is closest to the voltage waveform to be processed.
Correspondingly, the embodiment of the application also provides a phase delay acquisition method of the oscilloscope, and the phase delay acquisition method of the oscilloscope described below can be referred to by the phase delay acquisition device of the oscilloscope described above in a corresponding way.
Optionally, the method for obtaining the phase delay of the oscilloscope is implemented based on the device for obtaining the phase delay of the oscilloscope according to any of the embodiments, and the device for obtaining the phase delay of the oscilloscope includes: the phase delay acquiring method of the oscilloscope comprises the following steps:
providing a control signal for a control end of the second IGBT, wherein the control signal comprises at least two pulse signals separated by preset time;
measuring a current signal of a second end of the second IGBT by using a current probe of an oscilloscope;
measuring voltage signals at two ends of the second IGBT by using a differential probe of an oscilloscope;
and calculating the phase delay of the voltage signal and the current signal according to the voltage signal and the current signal obtained by measurement.
Optionally, the calculating the phase delay of the voltage signal and the current signal according to the voltage signal and the current signal obtained by measurement includes:
intercepting a voltage signal and a current signal within a preset time period after the starting moment of a second pulse signal in the control signal to obtain a voltage waveform to be processed and a current waveform to be processed;
discretizing the current waveform to be processed, wherein the discretized current waveform to be processed comprises a plurality of discrete points;
obtaining a plurality of voltage drop process curves according to the first inductor and the discretized current waveform to be processed;
fitting the voltage drop process curve to obtain a voltage fitting curve;
determining a voltage fitting curve which is most similar to the voltage waveform to be processed from a plurality of voltage fitting curves;
and determining stray inductance and phase difference time according to the determined voltage fitting curve, wherein the phase difference time is the phase delay of the voltage signal and the current signal.
Optionally, the obtaining a plurality of voltage drop process curves according to the first inductor and the discretized current waveform to be processed includes:
dividing the first inductor into a plurality of inductor values within a preset inductor range according to a preset inductor step length;
according to the adjacent discrete points, determining the time interval and the current value interval of the adjacent discrete points;
and calculating to obtain the multiple voltage reduction process curves according to the multiple inductance values, the time intervals and the current value intervals of the adjacent discrete points.
Optionally, the obtaining, by calculation, the multiple voltage drop process curves according to the multiple inductance values and the time intervals and the current value intervals between adjacent discrete points includes:
substituting the plurality of inductance values, the time intervals and the current value intervals of the adjacent discrete points into a first preset formula to calculate and obtain a plurality of voltage reduction process curves;
the first preset formula includes:
(ii) a Wherein Vt represents the voltage drop process curve, Dt represents a time interval adjacent to the discrete point, Di represents a current value interval adjacent to the discrete point, and Ls represents the inductance value.
Optionally, the value of the preset inductance step length is one thousandth of the total length of the preset inductance range.
Optionally, the determining a voltage fitting curve that is closest to the voltage waveform to be processed from the plurality of voltage fitting curves includes:
determining the slope of each of the voltage fit curves;
and determining the voltage fitting curve with the smallest difference between the slope of the plurality of voltage fitting curves and the slope of the voltage waveform to be processed as the voltage fitting curve which is closest to the voltage waveform to be processed.
Optionally, the intercepting a voltage signal and a current signal within a preset time period after a start time of a second pulse signal in the control signal to obtain a to-be-processed voltage waveform and a to-be-processed current waveform includes:
and intercepting a voltage signal and a current signal in a preset time period after the start time of the second pulse signal in the control signal, and performing recursive mean filtering on the intercepted current signal and voltage signal to obtain a to-be-processed voltage waveform and a to-be-processed current waveform.
Optionally, the value range of the preset time includes 10 ± 5 μ s.
In summary, the embodiment of the present application provides a phase delay acquiring device and an acquiring method of an oscilloscope, wherein the phase delay acquiring device of the oscilloscope comprises a power supply, a first IGBT, a second IGBT, a first inductor and a second inductor, in a test process, a control end of the second IGBT receives at least two pulse signals with a preset time interval, a control end of the first IGBT is suspended, when the second IGBT is turned on for the second time under the control of the control signal, a current flowing through the second IGBT starts to increase but does not reach a rated current of a first end of the second IGBT, a body diode of the first IGBT is in a freewheeling state at this time, due to existence of the first inductor, a gap may occur in a voltage signal measured by the oscilloscope, and a phase delay of the voltage signal and a phase delay of the current signal measured by the oscilloscope may be calculated according to the gap, so as to achieve a purpose of acquiring the phase delay of the oscilloscope, the whole device is realized by using the existing power unit, the cost is low, and the phase delay generated by selecting different oscilloscope channels can be compensated.
Features described in the embodiments in the present specification may be replaced with or combined with each other, each embodiment is described with a focus on differences from other embodiments, and the same and similar portions among the embodiments may be referred to each other.
The previous description of the disclosed embodiments is provided to enable any person skilled in the art to make or use the present application. Various modifications to these embodiments will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other embodiments without departing from the spirit or scope of the application. Thus, the present application is not intended to be limited to the embodiments shown herein but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.