Insulation may be simply modeled as a capacitor in parallel with a resistor as shown in (Figure 1). The current flows that results will comprise two components: the capacitive current (Ic) and the resistive current (Ir). (Figure 2) shows the time domain graph of the two currents.
Insulation with an AC voltage applied
Insulation current with AC voltage applied
For good insulation Ic is higher than 100 times Ir and Ic is leading Ir by close to 90o
For marginal insulation: Ic is higher than 50 times Ir and Ic is leading Ir by close to 80o
Note that the currents discussed in this chapter are the insulation currents NOT load currents
When DC current is involved, insulation may be modeled in a slightly different way. Consider (Figure 3). When switch S1 is closed, the DC supply is connected to the insulation system. In the DC model an extra capacitor has been added (dashed lines). The current that flows through this new capacitor is called the dielectric absorption current (Ida) (Figure 4) shows the time relationship for these three currents. The following paragraphs explain each of the three currents.
Insulation with DC voltage applied
DC current flow in good insulation
The capacitive current charges the capacitance in the system. It normally stops flowing few seconds (at most) after the DC voltage is applied. The short burst of capacitive current flow may put a rather substantial stress on any test equipment that is applied to very large insulation systems such as cables or large rotating machine.
The applied insulation voltage puts a stress on the molecules of the insulation. The positive side of the molecules is attracted to the negative conductor and the negative side of the molecules is attracted to the positive conductor. The result is an energy that is supplied to realign the molecules much like force will realign a network of rubber bands. Like Ic, Ida usually dies off fairly quickly as the molecules realign to their maximum extent.
This is the electron current flow that actually passes through the insulation. In good insulation the resistive current flow will be relatively small and constant. In bad insulation the leakage current may be fairly large and it may actually increase with time