Abstract:Abstract:The Medium Voltage (MV) Electricity Distribution Networks are frequently exposed to lightning and it is the main suspected reason for distribution transformer failures. Appreciable number of transformer failures occur due to insulation failures notably at points near line ends. The short rise time of a surge prompted by a lightning impulse can cause deterioration in the insulation and ultimately lead to a dielectric breakdown. The voltage distribution along transformer High Voltage (HV) winding become… Show more
“…On the other hand, the placement of the electrostatic shield depends on the location of the overvoltage surges. A study in [26] has placed the electrostatic shield at the outer layer of the HV winding due to overvoltage surges occurrence at that location. The resonant oscillations in the windings due to external transient overvoltage surges are generally different for each transformer.…”
Section: Resonant Overvoltage In Transformer Windingmentioning
This paper presents an investigation on the resonant oscillations of an 11 kV layer-type winding transformer under standard and chopped lightning impulse overvoltage conditions based on calculated parameters. The resistances, inductances and capacitances were calculated in order to develop the transformer winding equivalent circuit. The impulse overvoltages were applied to the high voltage (HV) winding and the resonant oscillations were simulated for each of the layers based on different electrostatic shield placement configurations. It is found that the placement of grounded shields between layer 13 and layer 14 results in the highest resonant oscillation and non-linear initial voltage distribution. The oscillation and linear stress distributions are at the lowest for shield placement between the HV and low voltage (LV) windings.
“…On the other hand, the placement of the electrostatic shield depends on the location of the overvoltage surges. A study in [26] has placed the electrostatic shield at the outer layer of the HV winding due to overvoltage surges occurrence at that location. The resonant oscillations in the windings due to external transient overvoltage surges are generally different for each transformer.…”
Section: Resonant Overvoltage In Transformer Windingmentioning
This paper presents an investigation on the resonant oscillations of an 11 kV layer-type winding transformer under standard and chopped lightning impulse overvoltage conditions based on calculated parameters. The resistances, inductances and capacitances were calculated in order to develop the transformer winding equivalent circuit. The impulse overvoltages were applied to the high voltage (HV) winding and the resonant oscillations were simulated for each of the layers based on different electrostatic shield placement configurations. It is found that the placement of grounded shields between layer 13 and layer 14 results in the highest resonant oscillation and non-linear initial voltage distribution. The oscillation and linear stress distributions are at the lowest for shield placement between the HV and low voltage (LV) windings.
“…2 and it was used as the input to the RLC equivalent circuit of the transformer model. Since, majority of the transformer winding failures occurred at the line ends [12], the lightning impulse was applied at the outermost layer. Hence, the present transient study is only focussed on HV layers.…”
Section: A Generation Of Lightning Impulsementioning
confidence: 99%
“…The Cll for layer 1 to 12 of the HV winding can be calculated based on (11). The capacitance between end phase of the winding and the transformer tank, Cgt was calculated based on (12) [16], (12) where h = h + d, h is height of the winding, do is the outer diameter of the inner layer, d is the gap between two layers, t is the internal width of the tank, which is 383.15 mm. The windings are concentrically arranged around the core.…”
Section: B Calculation Of Rlc Parameters For Transformer Modelingmentioning
This paper investigates the transient voltage distribution in a 11 kV layer type winding transformer under a standard 1.2/50 µs lightning impulse. The winding parameters known as resistance (R), inductance (L) and capacitance (C) were obtained through numerical calculation which were used to simulate the lumped equivalent circuit model. The calculated and simulated voltage distributions in all the layers of HV winding were analyzed. There is a steep and linear distribution of simulated and calculated voltage.
“…Oscillatory shape of the surge is created by the coupling of winding inductance and capacitances, and to understand the phenomena, different circuit models are proposed [6,7]. But analyzing with complicated models can be troublesome since it can be unvarying and takes a lot of time.…”
Section: Introductionmentioning
confidence: 99%
“…But analyzing with complicated models can be troublesome since it can be unvarying and takes a lot of time. A three phase transformer model has been used to investigate the influence of mutual coupling of LC components, with analysis conducted in both the time and frequency domains [6,7].…”
Due to high grounding resistance and soil conditions surge arrester performance decreases. Even though in installation the standard earthing resistance is achieved with time the earthing resistance would be at a high value. When a high voltage arrives at the surge arrestor it discharges the excess voltage by providing low impedance shunt path to ground and providing protection for the transformer. Because of high impedance path the voltage would not divert to the ground and carry on its original path and damage the transformer. Therefore, for areas with high earthing resistances protection must be improved for distribution substations. Throughout this research method of reducing the peak and the rate of rise of surge was analyzed for providing extra protection for the transformer. The selected substation was AV047 it was selected because of lightning occurrence in the selected area, Replacement of the transformer due to damages cause by overvoltage surges and high earthing resistance of the installed substation. Usage of the surge absorber for additional protection was investigated throughout the research. By this method proposed by the research group it was able to provide the sufficient protection for the transformer during surge conditions and reduce the peak and the rate of rise of the surge. Losses of the surge absorber were also analyzed at different conditions. Further an algorithm was developed so that the surge absorber could be implemented to any MV and HV networks for protection of the transformer.
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