Automotive Battery Current Detection System

Abstract

To provide a current detection system that allows differential detection of a magnetic field generated by a current in a conductor and efficient common mode noise cancellation in an interfering external magnetic field.SOLUTION: A current detection system comprises: a first magnetic tunnel junction device that is arranged adjacent to a current carrying conductor electrically connected to a battery of a vehicle and includes a V+ output and a V- output; a digital-analog converter that has a first input and a first output; a first band-pass filter that has a second input and a second output; a first switching unit that can switch between a first configuration in which the first output is connected to the first magnetic tunnel junction device and the V- output is connected to the second input, and a second configuration in which a power supply is connected to the first magnetic tunnel junction device and the V+ output is connected to the second input; and a processor that is operably connected to the second output and the first input and configured to control the first output through the first input based on the second output.SELECTED DRAWING: Figure 3

Description

[Technical Field]

[0001] (CROSS REFERENCE TO REFERENCED APPLICATION)

[0001] This application is related to and claims the benefit of priority from U.S. Provisional Patent Application No. 62 / 429,181, filed December 2, 2016, the contents of which are incorporated by reference in their entirety into this disclosure.

[0002] This application relates to current sensing systems, and more particularly to non-invasive automotive battery current sensing systems. [Background technology]

[0003]

[0003] In recent years, electric vehicles (EVs) and hybrid-electric vehicles (HEVs) have entered a new era of widespread consumer support. Compared with gasoline-powered vehicles, their reduced dependence on oil and lower emissions have made them attractive options for the future of the transportation industry. Electrical power for EVs is provided by a large series / parallel interconnection of rechargeable lithium-ion batteries. To ensure reliable and efficient battery operation and early fault diagnosis, it is essential to have a simplified solution for predicting the health of various subsystems within a vehicle. On the one hand, leakage currents (several milliamperes) between parallel-connected batteries may indicate inefficient impedance matching, while on the other hand, sharp spikes in current (hundreds of amperes) through wires may be an indicator of a short circuit path requiring immediate user attention. Therefore, it is crucial to have an integrated solution that can noninvasively measure both DC and AC currents over a wide range with high resolution.

[0004]

[0004] Several current measurement techniques have been proposed for EV / HEV applications, each with its own strengths and weaknesses. The shunt method is one of the most rudimentary methods for measuring current; the voltage drop across a resistor in series with the battery is used to calculate the current. Texas Instruments and SENDYNE have proposed shunt sensor designs for automotive applications that have galvanic isolation between the processing unit and the current-sensing circuit. However, shunt implementations are invasive and result in significant power losses when operating at high currents. Hall-effect sensors are also popular in current measurement applications due to their low cost and the galvanic isolation they provide. However, these sensors are highly sensitive to magnetic fields and are easily affected by stray magnetic fields, which can cause significant errors in small current measurements. Hall-effect sensors designed to accurately measure small currents (<10 A) must be shielded from stray magnetic fields and are invasive. Current transformers and Rogowski coils are current transducers that can operate over a wide frequency range. While these devices are non-invasive, they can only measure AC current and therefore cannot be used in EV / HEV applications. Another non-invasive technology for current measurement is the fluxgate current sensor. This sensor can measure low currents (≈50 mA) with a good dynamic range. However, fluxgate current sensors can be expensive and bulky due to their complex magnetic components and can have high self-heating due to their large quiescent current consumption. Therefore, improvements are needed in this area. Summary of the Invention [Problem to be solved by the invention]

[0005] [Means for solving the problem]

[0006] According to one aspect, the present disclosure provides a noninvasive current sensor comprising a TMR magnetic field sensor that utilizes the tunnel magnetoresistance (TMR) effect in a magnetic tunnel junction (MTJ) to generate a linear differential output voltage proportional to a magnetic field perpendicular to its package. An MTJ consists of a thin insulator sandwiched between two ferromagnetic materials. The orientation of the two magnetizations in the ferromagnetic film can be changed by an external magnetic field. When the magnetizations are in a parallel orientation, electrons are more likely to tunnel through the insulating film than when the magnetizations are in an opposite (antiparallel) orientation. Therefore, a change in the orientation of the ferromagnetic layers results in a similar change in the effective resistance at both ends of the device. As a result, such a junction can be smoothly transitioned through various resistance states by the application of an external magnetic field. When placed on a current-carrying conductor in an electric vehicle, the presently disclosed current sensor enables measurement of currents ranging from 10 mA to 150 A with a resolution of 10 mA.

[0007] In the following description and drawings, like reference numerals have been used, where possible, to designate like features that are common to the drawings. [Brief explanation of the drawings]

[0008] [Figure 1(a)] FIG. 1 illustrates a TMR magnetic field sensor according to one embodiment. [Figure 1(b)] 1(a) is a schematic diagram of the sensor of FIG. 1(a) according to one embodiment. [Figure 1(c)]

[0009] FIG. 1 illustrates the response of an example TMR magnetic field sensor to applied magnetic fields in the range of + / −5×10 4 / 4π (A / m) (50 Oe) when the TMR2905 is biased at 1 V. [Figure 2]

[0010] FIG. 1 illustrates a differential sensor arrangement according to one embodiment. [Figure 3]

[0011] 1(a) is a system diagram of an example incorporating the sensor of FIG. [Figure 4]

[0012] FIG. 1 shows the frequency response of an analog bandpass filter using R1=82Ω, R2=200KΩ, and C1=C2=1nF. [Figure 5]

[0013] FIG. 1( c) illustrates a method for sensing current through a conductor using the sensor of FIG. 1( c) according to one embodiment. [Figure 6]

[0014] FIG. 1( c) illustrates an example current sensing system for mounting the sensor of FIG. 1( c) according to one embodiment.

[0009]

[0015] The accompanying drawings are for illustrative purposes and are not necessarily to scale. DETAILED DESCRIPTION OF THE INVENTION

[0010]

[0016] In the description that follows, some aspects will be described in terms that would typically be implemented as a software program. Those skilled in the art will readily recognize that the equivalent of such software can likewise be constructed in hardware, firmware, or microcode. Because data manipulation algorithms and systems are well known, the present description will be directed in particular to algorithms and systems forming part of, or cooperating more directly with, the systems and methods described herein. Other aspects of such algorithms and systems, and the hardware or software for generating or otherwise processing the signals involved in the algorithms and systems, not specifically shown or described herein, are selected from such systems, algorithms, components, and elements known in the art. In view of the systems and methods as described herein, software not specifically shown, suggested, or described herein that is useful in implementing any aspect is conventional and within the skill of the art.

[0011]

[0017] FIG. 1(a) illustrates a TMR magnetic field sensor used as a current sensor, according to one embodiment. Figure 1(b) shows an example of a TMR2905 sensor 102. Figure 1(b) shows a schematic diagram of the relevant components. As shown, the TMR can be implemented as a push-pull Wheatstone bridge configuration of four unshielded MTJ elements 104 acting as a magnetic field dependent variable resistor, as shown in Figure 1(b). The push-pull design provides a highly sensitive differential output that is linearly proportional to the magnetic field applied perpendicular to the surface of the sensor package (along the z-axis) as shown in Figure 1(a). Figure 1(c) shows the ±5×10 V differential output when the TMR2905 is biased at 1 V. 4 1 shows the response of a TMR (in the example shown, TMR2905 from Multidimension Technology Co., Ltd.) to an applied magnetic field in the range of 1 / 4π(A / m) (50 Oe).

[0012]

[0018] To further improve the sensitivity of the TMR sensor 102, the sensor output needs to be highly amplified. Experiments reveal that V≠V for the sensor even in the absence of a magnetic field, i.e., there is an inherent offset in the differential voltage. This necessitates a method for efficiently canceling the offset so that the differential voltage actually caused by the external magnetic field is accurately measured. Furthermore, for reliable and low-resolution current sensing, several noise cancellation procedures are used in both the analog front end and the digital front end. In one embodiment, to cancel any common-mode noise and interfering magnetic fields, a differential arrangement of two of the sensors 102 is provided, as shown in FIG. 2. As shown, the sensors 102 are mounted 180° apart on a current-carrying circular conductor 110 (with insulator 112) to enable differential sensing of the magnetic field 108 generated by the current in the conductor 110 and efficient common-mode noise cancellation of the interfering external magnetic field 106. Additionally, the sensor 102 may be mounted to a substrate 114 (eg, a metal-free PCB board) as shown to maintain the position of the sensor 102 relative to the conductor 110 .

[0013]

[0019] The magnetic field due to the current carrying conductor 110 at the location of the sensor 102 is B IN and the total external magnetic field is B ext and the magnetic field measured by each sensor is S 1,input =B IN +B ext S 2,input =-B IN +B ext can be written as

[0014]

[0020] The output of two TMR sensors when a magnetic field is applied is S 1,output =(B IN +B ext )C1 S 2,output =(-B IN +B ext )C2 can be written as

[0015]

[0021] where C1 and C2 incorporate the sensitivity of the two TMR sensors and the gain of the analog front end. If the system is perfectly symmetrical, the values ​​C1 and C2 will be identical, resulting in a differential output

[0016]

number

number

[0017] This will give you:

[0022] Differential measurements therefore reject common mode noise and stray magnetic fields (including the Earth's magnetic field).

[0018]

[0023] 3 illustrates an example architecture of a current sensing system 300 according to one embodiment. The heart of the sensing mechanism includes a sensor 102 (e.g., a TMR2905 magnetic field sensor) placed in proximity to a current-carrying conductor 110.

[0019]

[0024] This section demonstrates an exemplary implementation of the above-described method for non-invasive, high-resolution sensing of DC and AC currents. Figure 3 shows the experimental setup for each of the upper and lower sensors 102. Both the upper and lower sensors 102 have the same architecture, separately, except for the parallel orientation of the sensor z-axes (Figure 2) for efficient common-mode noise cancellation, as described above. For simplicity, we will describe the current sensing mechanism for DC currents here. The residual offset voltage in each of the upper and lower TMR sensors is canceled as follows:

[0020]

[0025] V + and V - The offset is positive ΔV (ΔV=V + -V - ) is assumed to be DCV by using an analog Single-Pole Double Throw (SPDT) switch driven by a 32.768KHz crystal. + and V - is upconverted to 32.768KHz. Figure 3 shows that both the bottom switch in the SPDT switch connects the 3.3V to the TMR sensor power supply and the V of the sensor to the input of the bandpass filter. + Figure 4 shows the establishment of the output connection. In the next phase, the DAC output connects to the input of the bandpass filter, thereby producing a square wave (rail-to-rail swing of ΔV) at the input of the bandpass filter. A multi-feedback topology is selected for the bandpass filter centered at 32.768 KHz (f0) to achieve a high-Q filter, thereby minimizing flicker noise from the op-amp while also eliminating undesired high-frequency noise components. For high-resolution current detection, the amplification ratio is set to ≈450. Figure 4 shows the frequency response of the analog bandpass filter using R1 = 82 Ω, R2 = 200 KΩ, and C1 = C2 = 1 nF.

[0021]

[0026] The resulting sine wave at the filter output is 327.68KHz (f S The DAC output voltage is V - V + , i.e., until the offset is reduced enough to result in a low amplitude non-saturating sine wave at the filter output. + -V - Any change in can be easily detected by detecting the change in the sine wave amplitude from its previous value.

[0022]

[0027] To estimate the current flowing through the wire, the sampled values ​​are subtracted from the two oppositely placed sensors to obtain a differential reading, thereby eliminating any common-mode noise, as described in the previous section. The resulting differential sine wave has exactly the same f0 and f S The equation governing optimal detection of the amplitude of the differential sine wave is:

[0023]

number

[0024] where f0 is the sine wave frequency (32.768KHz) and f S is the sampling frequency and N is the total number of samples in the calculation. y gives an estimate of the amplitude that is linearly related to the current flowing through the wire.

[0025]

[0028] A flowchart describing the calculation steps in the above example embodiment is shown in FIG. 5. The process begins when the amplitude of the sine wave passing through the analog-to-digital converter is read. The system then checks to see if the amplitude is saturated. If so, the system increases or decreases the DAC analog output (e.g., by approximately 3.3 V) and rechecks the amplitude for saturation. Once an acceptable output (non-saturated) is reached, the system cross-correlates the acquired sine wave with an internally stored sine wave to estimate the amplitude. The amplitude is then used to determine the current flowing through conductor 110, since the current is linearly dependent on the detected amplitude. The current can then be displayed or otherwise received by the vehicle control system so that appropriate remedial action can be taken.

[0026]

[0029] FIG. 6 shows one example implementation that includes two housing portions, each with a TMR sensor 102 embedded therein, to allow the two sensors 102 to be mounted 180° apart on a conductor wire.

[0027]

[0030] In one embodiment, four sensors can be used, two on each side of the conductor, with the two sensors on either side mounted orthogonal to each other. Interference can be further canceled by using correlation between the measured outputs of the four sensors.

[0028]

[0031] The sensor 102 and other components listed herein may include or be connected to one or more computer processors and memories, which are communicatively connected and programmed to perform data processing and control functions. Program code includes computer program instructions that can be loaded into a processor and, when loaded into the processor, cause the processor to perform the functions, operations, or operational steps of various aspects of the present specification. Computer program code for performing operations for various aspects described herein can be written in any combination of one or more programming languages ​​and loaded into memory for execution. The processor and memory can be communicatively connected to external devices via a wired or wireless computer network to send and receive data.

[0029]

[0032] The present invention includes combinations of the aspects described herein. References to "a particular aspect" and the like refer to features that are present in at least one aspect of the invention. "An aspect" (also Separate references to "an embodiment" or "particular aspects" or the like do not necessarily refer to the same aspect or aspects. However, such aspects are not mutually exclusive unless so indicated or as would be readily apparent to one of ordinary skill in the art. The use of singular or plural when referring to a "method" or "methods" and the like is not limiting. In this disclosure, the word "or" is used in a non-exclusive sense unless expressly stated otherwise.

[0030]

[0033] Although the invention has been described in detail with particular reference to certain preferred embodiments thereof, it will be understood that changes, combinations, and modifications may be made by those skilled in the art within the spirit and scope of the invention.

Claims

1. A current detection system a first magnetic tunnel junction device disposed adjacent to a current carrying conductor electrically connected to a battery of a vehicle, the first magnetic tunnel junction device having a push-pull Wheatstone bridge structure with four magnetic tunnel junction elements, each having a magnetic field dependent variable resistance; ＋ V measured between the output and the other two of the magnetic tunnel junction elements in the second branch of the push-pull Wheatstone bridge structure. － a first magnetic tunnel junction device including an output; a digital-to-analog converter having a first input and a first output; a first bandpass filter having a second input and a second output; the first output is connected to an input of the push-pull Wheatstone bridge structure of the first magnetic tunnel junction device, and the V － a first configuration in which an output is connected to the second input; a power supply is connected to the input of the push-pull Wheatstone bridge structure of the first magnetic tunnel junction device; ＋ a first configuration in which the output is connected to the second input; and at least one processor connected to the second output and the first input, the at least one processor configured to adjust a digital signal for the first input in response to changes in an analog signal from the second output, thereby controlling the analog signal from the first output; A current sensing system comprising:

2. 2. The current sensing system of claim 1, a second magnetic tunnel junction device disposed adjacent to the current carrying conductor and on an opposite side of the current carrying conductor from the first magnetic tunnel junction device, the second magnetic tunnel junction device having a push-pull Wheatstone bridge structure including four magnetic tunnel junction elements each having a magnetic field-dependent variable resistance.

3. 2. The current sensing system of claim 1, the at least one processor comprises an analog-to-digital converter that converts the analog signal from the second output to a digital signal, and the first switching unit is configured to provide an output at a frequency that is lower than a sampling frequency of the analog-to-digital converter of the at least one processor.

4. 2. The current sensing system of claim 1, further comprising a wireless transmission unit coupled to the at least one processor; the at least one processor is configured to determine a current through the current-carrying conductor based on a measured magnetic field around the conductor; The current sensing system, wherein the wireless transmitting unit is configured to transmit data representative of the determined current to a vehicle monitoring system.

Images