Field of the Invention
The invention relates to a sensor assembly and, more particularly, a sensor chip comprising a bridge circuit in the form of a Wheatstone bridge for measuring of gradients of the magnetic field strength, consisting of four magnetoresistive resistors which are symmetrically arranged in two areas at a distance from a common center axis into two series-connected resistors bridge branches of the Wheatstone bridge, with the resistors being designed as magnetoresistive laminated strips, and an arrangement for measuring of electrical currents with the help of such a sensor chip.
Background of the Invention
Measuring arrangements for determining of magnetic-field gradients serve in particular the potential-free measurement of the current intensity of an electric current, which causes such a magnetic field. Since the entire surroundings of a magnetic field to be determined in this manner has already large-area interference magnetic fields, it is obvious to differentiate between the field to be measured and the interference magnetic field.
Such arrangements are also already known from the Patents DD 155 220, DD 275 745 and from German Patent DE 42 12 737 C1. Magnetoresistive sensor elements are thereby utilized, since their sensitivity is sufficiently great in order to detect currents over a large measuring range. The linearity of such sensor elements is, however, limited. Its actually high sensitivity depends strongly on the temperature and on an auxiliary magnetic field to be applied to the sensor elements. Moreover the sensitivity of the individual sensor elements is very different. With regard to temperature, problems arise because components adjacent the sensor may unevenly heat the individual sensor elements. This uneven heating causes the temperature of the individual sensor elements to vary so as to cause the output signal from the assembly to drift.
A sensor chip is therefore disclosed in the nonpublished patent application P 43 00 605.1-35 of the Applicant, in which the output signal is proportional to an electrical current to be measured, the sensitivity of which is ideally neither temperature nor auxiliary-field dependent, and which is supposed to have at all times an approximately equal sensitivity. To compensate the interference magnitudes this arrangement thereby assumes that the areas each include a resistor of the one and a resistor of the other bridge branch and that these are arranged symmetrically with respect to the center axis.
Summary of the Invention
The invention takes over the idea of the symmetrical arrangement of the laminated magnetoresistive strips and has the purpose to improve a sensor chip with respect to its dependency on a temperature gradient effective on it, and to disclose an arrangement for measuring of electrical currents with such a sensor chip. The output signal is proportional to the electrical current to be measured and the sensitivity of the sensor chip is neither temperature nor auxiliary-field dependent and is always supposed to be approximately constant.
The invention attains the purpose in a surprisingly simple manner. The output signal of the sensor chip has a nonlimited linearity range and is neither temperature nor auxiliary-magnet dependent. The sample scattering is extremely low since the topography of the sensor chip can be very precisely manufactured with the help of the microstructuring.
Since the distance of the two areas, namely the base length of the gradiometer, is kept to a minimum, the influence through interference magnetic fields is also insignificant, whereas the sources of which are spaced a large distance from the measuring arrangement.
An arrangement with a sensor chip of the invention has a high degree of geometric symmetry as the condition for a symmetrical heating up of the sensor chip during operation. The symmetrical design of the paired, in-parallel-connected laminated strips substantially eliminates the effects of any temperature gradient in the individual bridge branches so that later compensation is not needed. Through symmetrical temperature increases caused by the operating current, an equal rotation of the magnetization and consequently an equal resistance change is caused in all laminated magnetoresistive strips of the Wheatstone bridge. With this, also the temperature-dependent zero-point drift in the sensor chip is substantially eliminated.
Brief Description of the Drawings
The invention will be discussed in greater detail hereinafter in connection with one exemplary embodiment and the drawings, in which:
FIG. 1 shows a Wheatstone bridge according to the state of the art,
FIG. 2 shows a sensor chip according to the invention,
FIG. 3 shows the connection of a sensor chip of the invention to a circuit for measuring the current flowing therein, and
FIG. 4 shows the design of the connecting contacts and of the power supply in an arrangement according to FIG. 3.
Detailed Description
FIG. 1 illustrates a bridge circuit in the form of a Wheatstone bridge, in which two series-connected magnetoresistive resistors 1 and 2 are arranged in a first bridge branch A and two series-connected magnetoresistive resistors 3 and 4 in a second bridge branch B. The Wheatstone bridge is supplied with an operating voltage U.sub.b, an output voltage U.sub.a serves as the output signal. Below at least one of the resistors 1 to 4 there is provided a thin-layer strip line insulated against said resistor; in order to obtain the same structural parts, it is suggested that below each one of the resistors 1 to 4 there is provided a single thin-layer strip line 17. A control current I.sub.st flows through the control line 11 through the thin-layer strip line 17.
The details of the sensor chip of the invention can be recognized in the illustration of FIG. 2. The sensor chip 5 has two areas I and II, which respectfully include resistor pairs 1 and 2 and 3 and 4 which are equally spaced from a center axis 15. The resistors 1, 2, 3, 4 each consist of three laminated magnetoresistive strips 1', 2', 3', 4', respectively, which are parallel to one another and which have in a conventional manner barberpole structures 10. The barberpole structures 10 are symmetrical in all resistors 1, 2, 3, 4. Thus care is taken that only one applied field gradient controls the bridge. The resistor pairs 1/2 and 3/4 respectively form bridge branches A and B. This becomes also clear from the conductors 6 between the laminated strips 1', 2', 3', 4' and the conductors 8 leading outwardly from the laminated strips 1', 2', 3', 4'. Conductors 8 connect surface terminals 7 to the laminated strips 1', 2', 3', 4'. The surface terminals 7 form contacts projecting for the sensor chip 5 to which the operating voltage U.sub.b is applied and from which the output voltage U.sub.a is measured. Two additional surface terminals 7 serve as external contacts for supplying the control current I.sub.st. The surface terminals 7 are arranged symmetrically with respect to the center axis 15 in the center area III of the sensor chip 5.
As further observed in FIG. 2, the laminated strips 1' and 2' and 3' and 4' forming bridge branches A and B respectively are interleaved. In area I it can be seen that from the left sensor chip 5 has a first laminated strip 1' located adjacent two adjacent first and second laminated strips 2'.
As can also be seen by the orientation of the barberpole elements 10, the laminated strips 1', 2', 3', 4' are arranged so that when exposed to opposed magnetic fields through the application of current I.sub.o, the adjacent resistors undergo opposite changes in resistivity. Thus, resistors 1 and 2 undergo opposite changes in resistivity, resistors 3 and 4 undergo opposite changes in resistivity. Since resistors 1 and 3 have the same barber-pole orientation, they undergo opposite changes in resistivity. Since resistors 2 and 4 have the same barber-pole orientation, they undergo opposite changes in resistivity.
Furthermore an adjustable resistor 9, which in the illustrated manner is connected in series with the bridge branches A and B of the Wheatstone bridge is provided on the area of this center axis 15. The resistor 9 can be removed mechanically or by means of laser, with this removal being done in such a manner that the symmetry of the entire arrangement is maintained.
The output voltage U.sub.a is fed to an amplifier (not shown). Its output, the control current I.sub.st, is adjusted such that the effect of the outer magnetic-field gradient at the place of the laminated strips 1', 2', 3', 4' is cancelled. The control current I.sub.st forms the output signal of the arrangement. It is directly proportional to the magnetic-field gradient and does not depend on the temperature and large-area interference magnetic fields. For example, in some versions of the invention the terminals 7 across which U.sub.a is measured are tied to the opposed inputs of an operational amplifier; the amplifier's output is then feed back to strip line conductor 15 to function as the I.sub.st signal. A voltage representative of I.sub.st and the I.sub.o measured current is then measured across a resistor through which I.sub.st is tied to ground. The output current I.sub.st from the operational amplifier is employed as the measure of the current I.sub.o because it, unlike U.sub.a, varies substantially linearly with I.sub.o.
The inventive arrangement of the substantial axis symmetry at the sensor chip 5 takes care that the warming-up occurs in symmetry with the center axis 15. The resistance changes in the laminated strips 1', 2', 3', 4' caused by magnetorestriction are therefore the same all over and do not cause a change of the output voltage U.sub.a. Zero-point drift of output voltage as a function of temperature is thus substantially eliminated. Moreover, since the resistors forming the individual bridge branches A and B are located in the same areas I and II, respectively, of the sensor assembly the temperatures of the resistors forming each bridge branch should be substantially identical. This substantially eliminates the problem of U.sub.a signal drift occurring as a result of the individual bridge branch resistors having different temperatures. Thus, uneven heating of the sensor assembly owing to the asymmetric arrangement of adjacent heat generating components will not adversely effect the accuracy of the current measurements. Also, the trimming of the Wheatstone bridge is done in an axis-symmetrical manner since the resistor 9 is arranged in the center axis 15. In this manner it is possible to adjust the output voltage U.sub.a towards zero when no magnetic-field gradient exists.
FIGS. 3 and 4 show a single-package sensor assembly 20 that incorporates sensor chip 5 of this invention to measure current intensity I.sub.o of an electric current I.sub.o through lines 14 formed on a dual-in-line-pin package. The sensor chip 5 is electrically separated from the line 14 by an insulating layer 13. Two lines 14 are provided, through which current I.sub.o flows, as is illustrated in FIG. 3, in one direction relative to one bridge branch A and in the opposite direction through the other bridge branch B. With this magnetic-field gradient is created, which is proportional to the current I.sub.o in the line 14, interference magnetic fields, which can be caused by other currents passing nearby, do not have any effect on the output signal, the control current I.sub.st, since their magnetic fields act in the same degree on the two symmetrical areas I and II. What contributes to this is that the distances between the areas I and II are smaller than 1 mm.
FIG. 4 shows a single dual-in-line pin sensor assembly package 20 for the potential-free measuring of the current intensity I.sub.o. Both lines 14 are here formed such that again a magnetic-field gradient is created at the place of the sensor chip 5. The insulation 13 between the sensor chip 5 and the line 14 and the arrangement of the structural-element pins for the current I.sub.o and for supplying the sensor chip 5 on opposite sides of the structural element provide here for a high protective insulation voltage. In other versions of the invention sensor chip 5 may be packaged separately from the associated conductors 14.