Source: https://patents.google.com/patent/EP1111693A2/en
Timestamp: 2020-07-10 22:19:30
Document Index: 800258634

Matched Legal Cases: ['art 43', 'art 43', 'art 43', 'art 43', 'art 81', 'art 82', 'art 83', 'art 84', 'art 85', 'art 83', 'art 83']

EP1111693A2 - Large current detector having a Hall-effect device - Google Patents
Large current detector having a Hall-effect device Download PDF
EP1111693A2
EP1111693A2 EP00126092A EP00126092A EP1111693A2 EP 1111693 A2 EP1111693 A2 EP 1111693A2 EP 00126092 A EP00126092 A EP 00126092A EP 00126092 A EP00126092 A EP 00126092A EP 1111693 A2 EP1111693 A2 EP 1111693A2
EP00126092A
EP1111693B1 (en
EP1111693A3 (en
1999-12-20 Priority to JP36117899A priority Critical patent/JP4164615B2/en
1999-12-20 Priority to JP36117899 priority
2000-11-29 Application filed by Sanken Electric Co Ltd filed Critical Sanken Electric Co Ltd
2001-06-27 Publication of EP1111693A2 publication Critical patent/EP1111693A2/en
2004-10-13 Publication of EP1111693A3 publication Critical patent/EP1111693A3/en
2006-05-03 Publication of EP1111693B1 publication Critical patent/EP1111693B1/en
A current detector for detecting or measuring an electric current, comprising a Hall-effect device (1) for generating a voltage proportional to magnetic field strength, a metal-made baseplate (2, 2a-2e) mechanically supporting the Hall-effect device, and two current path terminals (3 and 4) for the inflow and outflow, respectively, of a current to be detected or measured. For handling a current of greater magnitude than a comparable prior art device, the baseplate is slitted to delimit an elongate path (34, 34a-34e) along which the current is to flow. The current path extends contiguous to the primary working part (23) of the Hall-effect device for causing the same to generate a voltage proportional to the magnitude of the current. The pair of opposite extremities of the current path are connected respectively to the current path terminals (3 and 4).
This invention relates to current detectors, and particularly to that utilizing a Hall-effect device for obtaining a voltage proportional to the magnitude of the current detected. More particularly, the invention deals with how to increase the current magnitude that can be handled by such a current detector.
By the term "Hall-effect device" used herein and in the claims appended hereto is meant the voltage generator built on the familiar Hall effect to give an output voltage in direct proportion to the magnetic field applied. Disposed contiguous to a current path, the Hall-effect device: will be subjected to the magnetic field that is generated in proportion to the magnitude of the current flowing through the path. The result will be the production of a voltage proportional to the current magnitude. It is self-evident, then, that the current path should lie as proximate as feasible to the Hall-effect device for maximum possible detection sensitivity.
The present invention aims at the provision of a current detector of the type incorporating a Hall-effect device, that is capable of accurately detecting or measuring a current of far greater magnitude than heretofore.
The above and other objects, features and advantages of the invention and the manner of rea'izing them will become more apparent, and the invention itself will best be understood, from the following description taken together with the attached drawings showing the preferred embodiments of the invention.
FIG. 2 is a section through the current detector, taken along the line A-A in FIG. 1;
FIG. 7 is an enlarged, fragmentary section through the FIG. 1 current detector, taken along the line B-B therein;
FIG. 19 is an enlarged section through the FIG. 17 embodiment, taken along the line C-C in FIG. 18; and
The general makeup of the first preferred form of current detector according to the invention, shown in FIGS. 1-9, wili become apparent from a study of FIGS. 1 and 2 in particular. The representative current detector comprises:
3. Two current path terminals 3 and 4 formed in one piece with the baseplate 2 and joined directly to the opposite ends of the current path in the baseplate, for the inflow and outflow, respectively, of the current to be detected.
6. A shielding layer 10 between Hali-effect device 1 and insulating plate 9.
With reference to FIGS. 7 and 8 in particular, generally in the shape of a rectangular sheet of silicon, the semiconductor substrate 18 has four other semiconductor regions 23, 24, 25 and 26 than the aforesaid four semiconductor regions 19-22. Of n conductivity type, the fifth semiconductor region 23 takes the form of an island of cruciate shape, as seen in a plan view as in FIG. 8, formed in the middle of the p-type eighth semiconductor region 26 which occupies most part of the semiconductor substrate 18.
The first and the second semiconductor region 19 and 20 are of n + type, higher in impurity concentration than the fifth semiconductor region 23, and are formed as islands, spaced from each other in the y direction in FIG. 8, in the fifth semiconductor region 23. The first and the second electrode 12 and 13 are in ohmic contact with these semiconductor regions 19 and 20. When the control current supply circuit 16 is connected to the electrodes 12 and 13 as in FIG. 9, the control current Ic is to flow through the fifth semiconductor region 23 from first 19 to second 20 semiconductor region, as indicated by the arrow in FIG. 8.
Of n + type, with an impurity concentration higher than that of the fifth semiconductor region 23, the third and the fourth semiconductor region 21 and 22 lie approximately centrally of the fifth semiconductor region 23 in the y direction in FIG. 8, which is at right angles with the x direction, with a spacing from each other in the x direction. These semiconductor regions 21 and 22 are partly contiguous to the fifth semiconductor region 23, partly to the p type sixth and seventh semiconductor regions 24 and 25, and are in ohmic contact with the third and fourth electrodes 14 and 15. The semiconducter regions 24 and 25 are intended to limit the areas of contact of the semiconductor regions 21 and 22 with the semiconductor region 23.
The Hall voltage is to be obtained between the third and the fourth semiconductor region 21 and 22 when the control current Ic is made to flow between the first and the second semiconductor region 19 and 20, with a magnetic field perpendicular to the direction of current flow. Therefore, the term "primary working part" of the Hall-effect device, as used herein and in the claims appended hereto, may be construed at least as that part of the fifth semiconductor region 23 which lies between the first and the second semiconductor region 19 and 20 and, additionally, between the third and the fourth semiconductor region 21 and 22. More broadly, however, the fifth semiconductor region 23 as a whole may be considered to constitute the primary working part of the Hall-effect device.
FIG. 5 best indicates that the metal-made baseplate 2 is approximately square in shape, having a pair of opposite edges 29 and 30 and another pair of opposite edges 31 and 32. The current path terminals 3 and 4 project approximately right-angularly from the edge 29 of the baseplate 2, so that this baseplate is to serve itself as a path of the current from terminal 3 to terminal 4.
The baseplate 2 with the current path terminals 3 and 4, as well as the Hall-effect-device terminals 5-8, can all be fabricated from a sheet-metal punching shown in FIG. 6 and therein generally designated 33. Typically made from sheet cooper with nickel plating, the punching 33 has a frame portion 34 bridging the current path terminals 3 and 4, another frame portion 35 bridging the Hall-effect-device terminals 5-8, and still other frame portions 36 bridging the frame portions 34 and 35. All the terminals 3-8 are to be cut off the frame portions 33 and 34 along the dot-and-dash lines after the current detector has been encapsulated in the plastic envelope 11, FIGS. 1, 2 and 5. FIG. 6 shows a punching fragment for the baseplate 2 and terminals 3-8 of one current detector according to the instant invention; in practice, there may be fabricated such punchings each including the baseplates and terminals of many such current detectors.
The slits delineating the current path 34 includes, perhaps most importantly, a slit 35 in the shape of an inverted J bounding one, or inner, side edge of the U-shaped current path. This J slit 35, as it will be so called hereinafter, is cut into the baseplate from its edge 29 in a position intermediate the two current path terminals 3 and 4 joined thereto. More specifically, the J slit 35 is constituted of a longer straight limb 35a extending rectilinearly from the edge 29 of the baseplate 2 toward, and terminating some distance short of, the opposite edge 30, a bight 35c bent right-angularly from the longer straight limb 35a toward the edge 31 of the baseplate, and a shorter straight limb 35b extending from the bight 35c approximately halfway back toward the edge 29 of the baseplate in parallel spaced relationship to the longer straight limb 35a.
Further, in order to delimit the other, or outer, edge of the current path 34, a plurality of, seven in this particular embodiment, additional slits 36-42 are formed in the baseplate 2. All these additional slits are straight. The first straight slit 36 extends from the baseplate edge 30 toward the opposite edge 29 and terminates short of the bight 35c of the J slit 35. The second straight slit 37 extends from the corner between the baseplate edges 30 and 31 toward the geometric center of the baseplate 2 and terminates short of the J slit 35. The third and the fourth straight slit 38 and 39 extend from the baseplate edge 31 toward the opposite edge 32 and terminates short of the shorter straight limb 35b of the J slit 35. The fifth straight slit 40 extends from the corner between the baseplate edges 30 and 32 toward the geometric center of the baseplate 2 and terminates short of the J slit 35. The sixth and the seventh straight slit 41 and 42 extend from the baseplate edge 32 toward the opposite edge 31 and terminates short of the longer straight limb 35a of the J slit 35.
FIG. 8 is explanatory of the positional relationship between the J slit 35 in the baseplate 2 and the semiconductor region 23, the primary working part, of the Hall-effect device 1, as seen in a plan view as in this figure, or in a direction normal to the plane of the baseplate 2. It will be observed that the semiconductor region 23 is mostly surrounded by the J slit 35, or thoroughly contained within the outer edges of the J slit, or, as will be noted by referring back to FIG. 5 for example, thoroughly contained between the pair of parallel limbs of the U-shaped current path 34. More specifically. the distance between the outer edges of the two straight limbs 35a and 35b of the J slit 35 is equal to, or just slightly more than, the maximum dimension of the semiconductor region 23 in the x direction. Further the total dimension of the straight limb 35b and bight 35c of the J slit 35 in the y direction is approximately equal to the dimension of the semiconductor region 23 in the same direction.
The "primary working part" of the Hall-effect device 1 has been previously broadly defined as the fifth semiconductor region 23. It has also been stated, however, that the "primary working part" in the more strict sense of the term is that part of the fifth semiconductor region 23 which lies between the first and the second semiconductor region 19 and 20 and between the third and the fourth semiconductor region 21 and 22. In compliance with this more strict definition of the term, the size of the J slit 35 may be redefined as such that the strict "primary working part" of the Hall-effect device is thoroughly contained inside the outer edges of the J slit.
With reference to FIG. 5 again, the midpart 43 of the baseplate 2 which is surrounded by the J slit 35 is joined to the current path 34 as the limb 35b of the J slit is made shorter than the other limb 35a. This midpart 43 is left to serve as the head radiator and the mechanical support for the Hall-effect device 1. The fins 44, so to say, which are likewise left outside the J slit 35 do not take part in the current path but serve as heat radiators and mechanical supports for the Hall-effect device 1.
The insulating plate 9, FIGS. 1, 2, 4 and 9, is an approximately square piece of sheet ceramic, among other insulating materials, which is slightly larger in size than the Hall-effect device 1. Overlying the baseplate 2 as in FIGS. 2 and 7 and bonded thereto via an electrically insulating adhesive layer 46, the insulating plate 9 functions to insulate the Hall-effect device 1 from the baseplate and to mechanically support the Hall--effect device as well as the shielding layer 10 directly overlying the insulating plate.
The shielding layer 10 Is a sheet of copper or like material. attached to the conductor layer 28 on the underside of the Hall-effect device 1 via a layer 45 of a nonmagnetic bonding material such as solder. The shielding layer 10 shields the Hall-effect device 1 from the influence of external electric fields. It is understood that the shielding layer 10 is electrically connected to the control current supply terminal 6, which is grounded.
For detection or measurement of the current Is flowing through any desired electric circuit, by the current detector of the above described construction, the current path terminals 3 and 4 may be connected to that electric circuit. Further the control current input terminals 5 and 6 may be connected to the control current supply circuit 16, FIG. 9, for causing the control current Ic, FIG. 8, to flow through the fifth semiconductor region 23 from the first 19 to the second 20 semiconductor region, and the voltage output terminals 7 and 8 to the differential amplifier 17.
Introduced into the current detector from the current path terminal 3, for instance, the current Is to be measured will flow through the baseplate 2 along the U-shaped current path 34, which is disposed very close to the fifth semiconductor region 23, the primary working part, of the Hall-effect device 1. The magnetic field H will be generated which, according to the Ampere rule, will be oriented in the direction indicated by the broken-line arrows in FIG. 7. This direction of the magnetic field is perpendicular to the direction of the control current Ic flowing through the semiconductor region 23, so that the Hall voltage will be generated between the semiconductor regions 21 and 22, FIGS. 8 and 9, hence between the electrodes 14 ard 15, and hence between the Hall voltage output terminals 7 and 8. The Hail voltage is proportional to the strength of the magnetic field H, which in turn is proportional to the magnitude of the current Is, so that this current is detectable from the Hall voltage.
3. The current path in the basepiate is narrowed by creating straight slits 36-42. Concentrated current flow through this path results in an increase in magnetic lines of flux actually working on the Hall-effect device.
5. The inside of the U-shaped current path is also left largely unremoved, being bounded by the J slit. The unremoved part 43, FIG. 5,serves as a heat radiator and mechanical support for the Hail-effect device.
10. The baseplate 2 and the terminals 3-8 are inexpensively fabricated from common sheet-metal punchings.
FIG. 10 shows a modified baseplate 2a according to the invention, for use in the FIGS. 1-9 current detector in substitution for its baseplate 2. The modified baseplate 2a features a pair of straight slits 51 and 52 cut in the baseplate 2a in place of the J slit 35, FIG. 5, of the first disclosed baseplate 2 for delineating the inside boundary of the U-shaped current path 34a. The other details of construction are as set forth above with reference to FIG. 5. Thus, for example, the outer periphery of the current path 34a is bound by the slits 36-42.
The pair of slits 51 and 52 extend in parallel spaced relationship to each other from the edge 29 of the baseplate 2a halfway toward the opposite edge 30. The distance between the left-hand edge, as seen in FIG. 10, of the left-hand slit 51 and the right-hand edge of the right-hand slit 52 is approximately equal to the dimension in the x direction, FIG. 8, of the fifth semiconductor region 23 of the FIGS. 1-9 current detector, so that the primary working part of the Hall-effect device is substantially contained between the outer edges of the slits 51 and 52.
The tongue-like part 43a of the baseplate 2a, left between the slits 51 and 52, does not take part in carrying the current to be detected but serves merely to radiate heat and mechanically support the Hall-effect device.
In FIG. 11 is shown another modified baseplate 2b featuring a straight slit 53 of much greater width than the FIG. 5 J slit 35 or FIG. 10 parallel straight slits 51 and 52, for bounding the inner edge of the U-shaped current path 34b. The baseplate 2b is akin in the other details of construction to the FIG. 5 baseplate 2.
The wide, straight slit 53 extends from the edge 29 of the baseplate 2b halfway toward the opposite edge 30. The width of this slit is approximately equal to the dimension of the fifth semiconductor region 23, FIG. 8, of the Hall-effect device 1 in the x direction and less than the dimension of the semiconductor substrate 18 in the same direction. The length of the slit 53 is greater than the dimension of the semiconductor region 23 in the y direction.
Thus the current path 34b is formed so, as to substantially surround the semiconductor region 23 of the Hall-effect device. The current detector employing this base plate 2b will therefore gain all but the fifth of the ten advantages set forth in conjunction with the FIGS. 1-9 embodiment.
Still another modified baseplate 2c shown in FIG. 12 is similar to the FIG. 5 baseplate 2 in having the J slit 35 defining the inner boundary of the U-shaped current path 34c, but different therefrom in not having the three straight slits 37-39 defining part of the outer periphery of the current path. Employed in lieu of these absent slits is a single straight slit 54 extending from the edge 30 more than halfway toward the opposite edge 29. Thus does the current path 34c have its outer periphery bounded by this additional straight slit 54 and the remaining straight slits 36 and 40-42.
Another difference is that the baseplate 2c is of greater dimension in the x direction, having a current path extension 55 which is partly set off from the U-shaped current path 34c by the additional straight slit 54 but which is joined directly to one end of that current path as the slit 54 terminates short of the edge 29. The first current path terminal 3 is joined to this current path extension 55 at the baseplate edge 30. The second current path terminal 4 is in the same position as in all the previous embodiments.
Perhaps the most pronounced feature of this baseplate 2c is that the two current path terminals 3 and 4 project in opposite directions therefrom. This terminal arrangement can be convenient in some applications of the invention.
FIG. 13 shows a slight modification 2d of the FIG. 12 baseplate 2c. Instead of the J slit 35 of the baseplate 2c there are formed a pair of straight slits 51 and 52 akin to those designated by the same reference numerals in FIG. 10. The baseplate 2d is identical with the baseplate 2c in the other details of construction.
FIG. 14 shows a further modified current detector in a view similar to FIG. 2. This modified current detector differs from that of FIGS. 1-9 only in that the insulating plate 9 has an extension 9a which is angled downwardly, as seen in FIG. 14, to intervene between the baseplate 2, which may be any of the constructions disclosed herein, and the set of lead terminals 5-8. The insulating plate extension 9a is designed for better insulation of the lead terminals from the baseplate.
Notwithstanding the teachings of the FIGS. 1-9 and FIG. 14 embodiments the provision of the insulating plate 9 is not a necessity. Thus, in FIG. 15, a current detector is shown, also in a view similar to FIG. 2, which has no insulating plate, and no shielding layer either.
Experiment has proved that no inconvenience occurs without the insulating plate 9. Without the shielding layer 10, too, the Hall-effect device is protected from external noise by the semiconductor substrate 18, if it is of silicon, which is relatively high in conductivity. This current detector may therefore be put to use in locations immune from noise, as it possesses the same advantages as the FIGS. 1-9 embodiment in all other respects.
Any of the current detectors herein disclosed may be formed in one piece with the amplifier shown at 17 in FIG. 9. FIG. 16 shows a semiconductor substrate 18a on which there are formed both a Hall-effect device 61 and an amplifier 62. The current detector built as taught by this invention, and incorporate not only the Hall-effect device 61 but also the amplifier 62, will be easier of handling, and the amplifier will be less in cost of manufacture.
FIGS. 17-20 are directed to the final embodiment of the invention, which differs from all the preceding ones in incorporating two Hall-effect devices for conjointly detecting a current. The two Hall-effect devices, seen at 1 and 1' in FIGS. 18-20, are both of the same construction as that of the FIGS. 1-9 embodiment. The various parts of the first Hall-effect device 1 are therefore indicated in FIGS. 18-20 by the same reference numerals as used to denote the corresponding parts of the FIGS. 1-9 device 1, and the various parts of the second Hall-effect device 1' by priming the reference numerals designating the corresponding parts of the first device 1.
As pictured in FIG. 19, both Hall-effect devices 1 and 1' are fabricated in one and the same semiconductor substrate 18b, although the two devices could be formed in separate substrates. This substrate 18 b is mounted on a baseplate 34e via the shielding layer 45 and insulating plate 9, just as the substrate 18, FIG. 7, of the Hall-effect device 1 of the FIGS. 1-9 embodiment is. Any further repetitive description of the Hall-effect devices 1 and 1' is considered redundant.
The baseplate 2e of this current detector is modified as shown in FIG. 17 both for mechanically supporting the two Hall-effect devices 1 and 1' and for providing a recumbent-S-shaped current path 34e along which the current is to flow in proximity to the semiconductor regions 23 and 23', the primary working parts, of both devices. The S-shaped current path 34e is defined by two J slits 35 and 35' and eight straight slits 36, 36', 40-42, and 40'-42'. It will be understood that the J slit 35 and four straight slits 36 and 40-42 are cut in the baseplate 2e just like their counterparts in FIG. 5, defining the right hand half, as seen in FIG. 17, of the S-shaped current path 34e.
The left hand half of the current path 34e, then, is defined by the other J slit 35' and the other straight slits 36' and 40'-42'. The J slit 35', which is of the same shape and size as the J slit 35, is cut into the baseplate 2e from its edge 30. The straight slit 36' extends from the baseplate edge 29 toward the opposite edge 30 and terminates short of the bight of the J slit 35'. The straight slit 40' extends from the corner between the baseplate edges 29 and 31 toward the geometric center of the baseplate 2e and terminates short of the J slit 35'. The straight slits 41' and 42' extend from the baseplate edge 31 toward the opposite edge 32 and terminate short of the J slit 35'.
Thus the S-shaped current path 34e is constituted of first part 81 between baseplate edge 31 and J slit 35', second part 82 between J slit 35' and baseplate edge 29, third part 83 between J slits 35 and 35', fourth part 84 between J slit 35 and baseplate edge 30, and fifth part 85 between J slit 35 and baseplate edge 32. The current path terminal 3 is joined to the baseplate edge 30 in a position forming one end of the current path 34e. The other current path, terminal 4 is joined to the baseplate edge 29 in a position forming the other end of the current path 34e.
It will also be observed from FIG. 17 that the primary working region 23 of the first Hall-effect device 1 lies between the third 83 and the fifth 85 part of the current path 34e. The primary working region 23' of the second Hall-effect device 1' lies between the first 81 and the third 83 part of the current path 34e. The midpart 83 of the current path 34e is thus shared by both devices 1 and 1'.
FIG. 20 is explanatory of how the two Hall-effect devices 1 and 1' are connected to a control current supply circuit 16a and an amplifier circuit 17a, which are both adapted for use with current detectors having two Hall-effect devices. The electrodes 12 and 13, set forth for the FIGS. 1-9 embodiment with reference to FIG. 9, of the first Hall-effect device 1, and the corresponding electrodes 12' and 13' of the second Hall-effect device 1, are both connected to the four outputs of the control current supply circuit 16a
The amplifier circuit 17a comprises three differential amplifiers 71, 72 and 73. The first amplifier 71 has a noninverting input connected to the electrode 14, and an inverting input connected to the electrode 15, of the first Hall-effect device 1. The second amplifier 72 has a noninverting input connected to the electrode 14', and an inverting input connected to the electrode 15', of the second Hall-effect device 1'. The outputs of the amplifiers 71 and 72 are connected to the third amplifier 73.
Operation of Ninth Form
As the current Is flows along the S-shaped current path 34e in the baseplate 2e in the direction of the arrow in FIG. 17, from terminal 3 to terminal 4, the magnetic fields H acting on the two Hall-effect devices 1 and 1' will be oriented in the opposite directions indicated by the arrows in FIG. 19. Thus the differential amplifiers 71 and 72 will put out Hall voltages Vh 1 and -Vh 2 of opposite polarities. Inputting these Hall voltages, the third differential amplifier 73 will provide an output voltage according to the equation, Vh 1 - (-Vh 2) = Vh 1 + Vh 2. The output from the amplifier 73 will thus be the sum of the absolute values of the outputs Vh 1 and -Vh 2 from the two amplifiers 71 and 72. The same output could be obtained, of course, by providing an inverter on the output stage of the amplifier 72 and by providing an adder in place of the amplifier 73.
2. Despite use of two Hall-effect devices, the resulting increase in size is reduced to a minimum as they share the midpart 83, FIG. 17, of the S-shaped current path 34e.
3. Since the two Hall-effect devices are acted upon in the opposite directions by the magnetic fields H due to the flow of the current Is along the S-shaped current path 34e, cancellation will occur between the noise components of the output voltages of both devices due to external magnetic fields. Let Vo be the Hall voltage of each Hall-effect device due to an external magnetic field. Then the output from the first amplifier 71 is defined as Vh 1 + Vo, the output from the second amplifier 72 as - Vh 2 + Vo, and the output from the third amplifier 73 as Vh 1 + Vo - (-Vh 2 + Vo) = Vh 1 + Vh 2 .
2. Only a prescribed fraction of the incoming current could be made to flow along the current path in the baseplate for measurement of its total magnitude..
A current detector for detecting or measuring an electric current, comprising a Hall-effect device (1) for generating a voltage proportional to magnetic field strength, a metal-made baseplate (2, 2a-2e) mechanically supporting the Hall-effect device, and two current path terminals (3 and 4) for the inflow and outflow, respectively, of a current to be detected or measured, characterized in that the baseplate is slitted to provide an elongate current path (34, 34a-34e) having a pair of opposite ends connected respectively to the current path terminals (3 and 4), the current path extending in proximity to the Hall-effect device for causing the same to generate a voltage proportional to the magnitude of a current flowing through the current path.
A current detector as claimed in claim 1, characterized in that the current path (34, 34a-34d) in the baseplate (2, 2a-2d) is in the shape of a U.
A current detector as claimed in claim 2, wherein the Hall-effect device has a primary working part (23) for the development of the voltage proportional to the magnitude of the current flowing through the current path in the baseplate, characterized in that the primary working part is substantially thoroughly contained within the U-shaped current path (34, 34a-34d) in the baseplate (2, 2a-2d) as seen in a direction normal to the baseplate.
A current detector as claimed in claim 2, characterized in that the baseplate has formed therein at least one slit (35, 51, 52, 53) bounding one side edge of the U-shaped current path, and at least one other slit (36-43) bounding another side edge of the current path.
A current detector as claimed in claim 4, characterized in that said other edge of the current path is bounded by a plurality of straight slits (36-43) cut into the baseplate.
A current detector as claimed in claim 2, characterized in that the U-shaped current path is defined at least in part by a J-shaped slit (35) cut into the baseplate.
A current detector as claimed in claim 2, characterized in that the U-shaped current path is defined at least in part by a pair of straight slits (51 and 52) cut into the baseplate and extending in parallel spaced relationship to each other.
A current detector as claimed in claim 2, characterized in that the U-shaped current path is defined at least in part by a single straight slit (53) cut into the baseplate.
A current detector as claimed in claim 2, wherein the baseplate (2, 2a, 2b) is a generally rectangular piece of sheet metal, characterized in that the current path terminals (3 and 4) are integrally joined to one edge (29) of the baseplate.
A current detector as claimed in claim 2, wherein the baseplate (2c, 2d) is a generally rectangular piece of sheet metal, characterized in that one current path terminal (3) is integrally joined to a first edge (29) of the baseplate and directly connected to one end of the U-shaped current path (34c, 34d), and wherein the other current path terminal (4) is integrally joined to a second edge (30), opposite to the first edge, of the baseplate and connected to the other end of the current path via an extension (55) thereof.
A current detector as claimed in claim 10, characterized in that the baseplate has at least one slit (35, 51-53) cut therein from the first edge (29) thereof to bound one side edge of the U-shaped current path, and another slit (54) cut therein from the second edge (30) thereof to form the extension (55) of the current path.
A current detector as claimed in claim 11, characterized in that said one edge of the U-shaped current path is bounded by a J-shaped slit (35).
A current detector as claimed in claim 11, characterized in that said one edge of the U-shaped current path is bounded by a pair of straight slits (51 and 52) cut into the baseplate so as to extend in parallel spaced relationship to each other.
A current detector as claimed in claim 1, characterized in that an insulating plate (9) is interposed between the baseplate and the Hall-effect device.
A current detector as claimed in claim 14, characterized in that a shielding layer (10) is interposed between the Hall-effect device and the insulating plate.
A current detector as claimed in claim 1, wherein the Hall-effect device has a plurality of lead terminals (6-9) for connection to external circuits, characterized in that the lead terminals are cut off from the same sheet metal punching as is the baseplate.
A current detector as claimed in claim 16, characterized in that an enclosure (11) of electrically insulating material encloses all the listed components of the current detector but parts of the current path terminals and the lead terminals.
A current detector as claimed in claim 1, characterized in that the Hall-effect device is formed in a semiconductor substrate (18a) in which there is also formed an amplifier (62) for amplifying the output voltage of the Hall-effect device.
A current detector for detecting or measuring an electric current, comprising two Hall-effect devices (1 and 1') each for generating a voltage proportional to magnetic field strength, a metal-made baseplate (2e) mechanically supporting the Hall-effect devices, and two current path terminals (3 and 4) for the inflow and outflow, respectively, of a current to be detected or measured, characterized in that the baseplate is slitted to provide an elongate current path (34e) having a pair of opposite ends connected respectively to the current path terminals, the current path extending in proximity to the Hall-effect devices for causing the same to generate voltages proportional to the magnitude of a current flowing through the current path, whereby the magnitude of the current flowing through the current path is detectable in terms of the sum of the absolute values of the output voltages of the Hail-effect devices.
A current detector as claimed in claim 19, characterized in that the current path (34e) in the baseplate (2e) is in the shape of an S.
A current detector as claimed in claim 20, wherein the baseplate is a generally rectangular piece of sheet metai having a first edge (29), a second edge (30) opposite to the first edge, a third edge (31) at right angles with the first and the second edge, and a fourth edge (32) opposite to the third edge, characterized in that the baseplate has a first slit (35) cut into the baseplate from the first edge thereof to bound part of one side edge of the S-shaped current path (34e), and a second slit (35') cut into the baseplate from the second edge thereof to bound part of another side edge of the current path, that the current path is constituted of a first part (81) between the third baseplate edge (31) and the second slit (35'), a second part (82) between the first baseplate edge (29) and the second slit (35'), a third part (83) between the first and the second slit (35 and 35'), a fourth part (84) between the second basep.ate edge (30) and the first slit (35), and a fifth part (85) between the fourth baseplate edge (32) and the first slit (35), and that the two current path terminals (3 and 4) are joined respectively to the first and the second edge (29 and 30) of the baseplate in positions contiguous to the first and the fifth part (81 and 85) of the current path.
A current detector as claimed in claim 21, wherein each Hall-effect device (1, 1') has a primary working part (23) for the development of the voltage proportional to the magnitude of the current flowing through the current path in the baseplate, characterized in that the primary working parts of the two Hall-effect devices are substantially thoroughly contained respectively between the first and the third part (81 and 83), and between the third and the fifth part (83 and 85), of the current path, both as seen in a direction normal to the baseplate (2e).
A current detector as claimed in claim 19, characterized in that the two Hall-effect devices (1 and 1') are connected to an output circuit (17a) for combining the absolute values of the output voltages of the Hali-effect devices.
A current detector as claimed in claim 23, characterized in that the output circuit (17a) comprises two amplifiers (71 and 72) connected respectively to the Hall-effect devices (1 and 1'), and arithmetic means (73) connected to the amplifiers for providing an output indicative of the sum of the absolute values of outputs from the amplifiers.
EP00126092A 1999-12-20 2000-11-29 Large current detector having a Hall-effect device Expired - Fee Related EP1111693B1 (en)
JP36117899A JP4164615B2 (en) 1999-12-20 1999-12-20 Current detector having hall element
JP36117899 1999-12-20
EP1111693A2 true EP1111693A2 (en) 2001-06-27
EP1111693A3 EP1111693A3 (en) 2004-10-13
EP1111693B1 EP1111693B1 (en) 2006-05-03
ID=18472517
EP00126092A Expired - Fee Related EP1111693B1 (en) 1999-12-20 2000-11-29 Large current detector having a Hall-effect device
US (2) US6683448B1 (en)
EP (1) EP1111693B1 (en)
JP (1) JP4164615B2 (en)
DE (1) DE60027680T2 (en)
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1999-12-20 JP JP36117899A patent/JP4164615B2/en not_active Expired - Fee Related
2000-11-28 US US09/723,440 patent/US6683448B1/en active Active
2000-11-29 DE DE60027680T patent/DE60027680T2/en not_active Expired - Fee Related
2000-11-29 EP EP00126092A patent/EP1111693B1/en not_active Expired - Fee Related
2003-10-20 US US10/689,017 patent/US6791313B2/en active Active
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US6791313B2 (en) 2004-09-14
JP4164615B2 (en) 2008-10-15
US20040080307A1 (en) 2004-04-29
EP1111693B1 (en) 2006-05-03
DE60027680D1 (en) 2006-06-08
DE60027680T2 (en) 2007-04-26
JP2001174486A (en) 2001-06-29
EP1111693A3 (en) 2004-10-13
US6683448B1 (en) 2004-01-27
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EP1281974B1 (en) 2007-04-18 Hall-effect current detector
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US9297836B2 (en) 2016-03-29 Method and sensor for sensing current in a conductor
2004-10-13 RIC1 Information provided on ipc code assigned before grant
Ipc: 7G 01R 15/20 A
Ipc: 7H 01L 43/06 B
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