ENCYCLOPEDIA OF RADIO ELECTRONICS AND ELECTRICAL ENGINEERING Compensating current sensor with magnetic shunt. Encyclopedia of radio electronics and electrical engineering Encyclopedia of radio electronics and electrical engineering / Measuring technology The described design of the sensor used in measuring high currents differs from similar devices currently used in the presence of a magnetic shunt, which reduces the power consumption, weight and dimensions of the device. To measure high currents (of the order of tens of kiloamperes), the classical circuit of a compensation type sensor (Fig. 1), on which industrial products are built [1], is unacceptable. The principle of operation of such sensors is based on the compensation of the magnetic field created in the magnetic circuit by the measured current by means of the current of the compensation winding. The current transformer TA1 is a closed magnetic circuit with a winding, covering a bus with a measured current, in the gap of which a Hall sensor (U1) is installed. When current passes through the bus, a magnetic flux is created in the magnetic circuit that surrounds it, causing a voltage proportional to the measured current to appear in the Hall sensor. This voltage, amplified by an operational amplifier (DA1) and a power amplifier on transistors VT1, VT2, causes a current in the TA1 winding, which compensates for the magnetic flux in the magnetic circuit. To compensate for the magnetic field created, for example, by a current of 100 kA, the current through the compensation winding must be equal to 100/n kA, where n is the number of turns of this winding. In this case, the power of the output amplifier and the mass of the sensor may be too large. To reduce the compensation current in the proposed sensor (Fig. 2), the magnetic flux is compensated not in the entire section of the magnetic circuit 2, but in a limited area with a magnetic resistance less than the resistance of the entire magnetic circuit. At the installation site of the Hall sensor 3, where the magnetic flux bifurcates (AB), the magnitude of the magnetic induction created by the measured current I in bus 1, B = μμ0I / 2l (at l "d), where μ is the magnetic permeability of the magnetic circuit material; μ0 is the magnetic vacuum permeability. To compensate for the magnetic flux created by the measured current in this section, the current of the compensation winding 4 I1 = Vx2s1/μμ0 = Ixd/l. The current of the compensation winding I1 is less than the measured current I by l/d times, which makes it possible to implement a sensor of acceptable weight and dimensions. In the proposed sensor l=100 mm, d = 1 mm, therefore, with a measured current of 100 kA, the compensation current is created by a current of 1/n kA, where n is the number of turns of the compensation winding. A compensation sensor with a magnetic shunt of this design has the following characteristics.
The implementation of such a design is possible when using a magnetic circuit with a high saturation induction, for example, GAMMAMET 440C1 with a linear magnetization characteristic up to 1...1,2 T [2, 3]. To reduce the influence of external magnetic fields, it is advisable to use two magnetic circuits and Hall sensors in the design shown in Fig. 3. Here, the gap l in the magnetic circuit around bus 1 with current is divided into two equal sections between the magnetic circuits 2, 3. The currents of the compensation windings 6 and 7 in this circuit are summed up. If the external magnetic field at the installation site of one of the Hall sensors (4 or 5) coincides in direction with the magnetic field created by the measured current, then at the installation site of the other Hall sensor it is opposite in direction. If the signals of the Hall sensors 4, 5, due to the magnetic field of the measured current, have the same polarity, then the signals from the external magnetic field are pickups of different polarity, and therefore the resulting signal from the external magnetic field is zero. An amplifier for such a device needs a fairly low-power one - its current consumption is not more than 0,25 A at a supply voltage of +15 V. If it is impossible to purchase the necessary magnetic circuit, you can use cold-rolled electrical steel grades E310, E320, for which the saturation induction is also quite high, and with a measurement error of about 1%, this material is quite suitable. Literature
Author: A. Aldokhin, Chernihiv, Ukraine See other articles Section Measuring technology. Read and write useful comments on this article. Latest news of science and technology, new electronics: The world's tallest astronomical observatory opened
04.05.2024 Controlling objects using air currents
04.05.2024 Purebred dogs get sick no more often than purebred dogs
03.05.2024
Other interesting news: ▪ BlackBerry owners can chat for free ▪ Ordinary dogs accepted the robot into their company ▪ Mystery of natural mushroom factory solved News feed of science and technology, new electronics
Interesting materials of the Free Technical Library: ▪ section of the site Tools and mechanisms for agriculture. Article selection ▪ article And the smoke of the fatherland is sweet and pleasant to us. Popular expression ▪ Article Aspiano officinalis. Legends, cultivation, methods of application ▪ article VHF FM radio station. Encyclopedia of radio electronics and electrical engineering
Leave your comment on this article: All languages of this page Home page | Library | Articles | Website map | Site Reviews www.diagram.com.ua |