The present invention relates to an apparatus for representing and displaying the coil temperature of an electrical power transformer as well as a limiting circuit suitable for that purpose.
Transformers designed for high levels of power in electrical energy mains are termed power transformer. These power transformers are in that case subject in part to strong physical loads which are attributable to, for example, too-high load currents. These can be accompanied by excessive ageing phenomena within the power transformer and thus damage, which bring with them serious consequences for operational reliability. However, not only operational reliability, but also the service life of these expensive capital-cost items critically depend on operation of each individual power transformer in a manner which is as preserving as possible. One possibility for ensuring frictionless operation of a power transformer is to monitor the coil temperature of the power transformer.
In order to simulate and indicate the coil temperature of a power transformer a method has become known from, for example, DE 196 48 332 [U.S. Pat. No. 6,086,249] in which the measured and indicated temperature is formed from the temperature of the coolant for cooling the power transformer and the temperature of an electric heating means, which in turn is supplied with a current proportional to the load of the power transformer. For temperature measurement use is made of a thermometer which comprises a hollow measuring sensor, a mechanical measurement transducer, which is connected with the measuring sensor by a capillary tube, for actuation of a mechanical indicating device and a plurality of switches, wherein the interconnected cavities of the measuring sensor, capillary tube and measurement transducer form a closed pressure chamber filled with a measurement medium, the volume of which changes in dependence on temperature. The temperature of the coolant of the power transformer is directly measured with the help of the measuring sensor and through a direct heating, which is separate from measurement of the temperature of the coolant, of the measurement medium with the help of the electrical heating means immersed in the measurement medium an additional measurement pressure corresponding with the coil temperature of the power transformer is generated.
The electric heating means is arranged in an insulated heating chamber which is preferably connected by a capillary tube with the pressure chamber of measuring sensor and measurement transducer.
A further method, which is known from the prior art and which concerns indirect measurement of the coil temperature at power transformers, is known from DE 89 11 078 U1. In this method a hollow measuring sensor is arranged in an immersion sleeve for installation in a liquid-filled transformer casing and is surrounded by an insulating hose around which in turn is wound an electrical heating resistance, which for its part is encased by a further insulating hose. A current, termed CT signal current in the following, proportional to the load of the transformer is conducted, with the help of a power converter, via the heating resistance, the magnitude of which is so set to the heating resistance and the heat transfer in the direction of the measuring sensor and coolant that the temperature measured by the measuring sensor corresponds with the respective mean or maximum coil temperature of the power transformer.
The immersion sensor is in that case installed in the transformer casing in such a manner that the immersion sleeve is immersed in the cooling liquid of the transformer. In that case, the temperature difference between transformer coil and cooling liquid depends on the respective current in this coil. A current converter which detects the current, which is flowing across the transformer, as CT signal current is therefore associated with the transformer. The CT signal current of this current converter is now proportional to the current flowing across the transformer. the CT signal current subsequently flows via a heating resistance, which is associated with the temperature sensor, and thereby generates an indicating plot, which corresponds with the respective transformer load, relative to the actually measured oil temperature. As a consequence of a calibration undertaken before placing in operation it is possible in this indirect manner to obtain an indication of the mean or maximum coil temperature for a given current load of the power transformer, i.e. the display of display device, which is downstream of the heat temperature sensor, in a thermal image of the processes within the power transformer. The display can then take place, after appropriate amplification of the measurement signals, in a control room distant to a greater or lesser extent. It is alternatively also possible to electronically further process the relevant measurement values in a control and regulating installation, for example to form optical and/or acoustic warning signals. All these evaluating circuits of the CT signal current in that case, however, require a separate energy supply.
This form of simulation and indication of the coil temperature of an electrical power transformer has proved satisfactory in practice, but has the disadvantage that the evaluating circuits which measure, evaluate, analyze or indicate the current of a CT signal current circuit have to be supplied from a source, which is separate from the CT signal current, with the energy needed for their own requirements. For this purpose it is always necessary to install at least one further line, which conducts supply energy, additionally to the line of the CT signal circuit for power supply of the heating resistance as well as to provide a separate energy source. However, in the environment of devices conducting high voltage this means not only a substantial costs outlay, but also additional risks with respect to electromagnetic influencing of the supplied measuring device. This risk can in turn be remedied only with a substantial outlay in terms of safety technology.
It is therefore the object of the present invention to indicate an apparatus for representing and displaying the coil temperature of an electrical power transformer, which does not need an additional energy source for power supply of the measuring device for evaluation of the CT signal current.
This object is fulfilled by an apparatus for representing and displaying the coil temperature of an electrical power transformer with the features of the first claim. The subclaims in that case relate to particularly advantageous developments of the invention.
The present invention is in that case based on the general idea of using the CT signal current not only for supply of, for example, the heating resistance of a measuring sensor, but also to couple out the CT signal current energy by way of transformer via an electronic limiting circuit for power supply of the connected measuring device so that ultimately a separate energy source can thus be eliminated. For that purpose the primary winding of a transformer, termed tapping transformer in the following, is inserted into the CT signal current and limits the voltage, which decays by way of the primary winding and secondary winding of the tapping transformer, in that a triac, which is triggered by way of two diodes connected in parallel, short-circuits as soon as the corresponding half-wave of a threshold value is reached and opens again only with the next current zero transition of the CT signal current. Thus, in accordance with the invention additional lines or energy sources are no longer required for power supply of the evaluating circuit. The power supply of the connected evaluating circuit is, in addition, completely electrically separated from the CT signal current. The risk of entry of electromagnetic disturbances into the evaluating circuit is thus significantly reduced, which increases the reliability and service-life length of the components used and thus reduces costs.
The invention shall be explained in more detail in the following by way of example on the basis of figures, in which:
This has the consequence that the energy extraction in the case of the positive half-wave is limited to the energy flowing away in the charging of the capacitor C1. In the case of the negative half-wave, no energy is conducted into the downstream evaluating circuit 2 by way of the terminals X3 and X4, which if required can be subsequently optimized by use of a rectifier bridge. If in the case of a further rise of the instantaneous current in the course of the sine curve of the CT signal current through the resistive component of the primary side 7 of the tapping transformer L1 the voltage dropping across that now exceeds a specific value than the tapping transformer L1 is thereby short-circuited at its primary side 7. This voltage is determined by the breakdown voltage of two diodes D2 and D3, which are connected in anti-parallel arrangement and inserted into the gate path of the triac D5, as well as the gate voltage of a triac D5 electrically connected with the two diodes D2 and D3. In other words: the triac D5 short-circuits the primary side of the tapping transformer L1 exactly when the amount of the current through its gate has exceeded the trigger threshold. This is the case when the voltage between X1 and X2 in terms of amount exceeds the sum of the breakdown voltage of the diode D3 (positive half-wave) or D2 (negative half-wave) plus the gate threshold voltage of the triac D5.
Number | Date | Country | Kind |
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102011107375.6 | Jul 2011 | DE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2012/059789 | 5/25/2012 | WO | 00 | 2/19/2014 |