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2.4.1.2.1 Parallel Representation

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The complex permittivity of any dielectric medium can be represented as εc, is denoted in (2.1),

(2.1)

where σ is the conductivity and ω is the frequency of the source. The real part εr is the measure of how much energy is stored by the material and the εr represents how dissipative a material can be in reaction to an external electric field. On the application of an AC sinusoidal voltage source to the lossy dielectric in parallel combination with resistance Rp and capacitance Cp, the resultant current I is composed of two components: the conduction current Ic and the displacement current Id, as seen in Figure 2.6a and b, which is related to the DDF as given in (2.2),


Figure 2.5 Comparison of ACBDV values of different oil samples.

Figure 2.6 (a) Parallel representation of the insulation. (b) Phasor diagram for parallel circuit. (c) Series representation of the insulation. (d) Phasor diagram for series circuit.

(2.2)

The power loss P can be represented in Eq. (2.3),

(2.3)

Alternative Liquid Dielectrics for High Voltage Transformer Insulation Systems

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