2019
DOI: 10.25206/1813-8225-2019-168-70-74
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Research of temperature destruction effect on cables insulation operation life

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(6 citation statements)
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“…Within the framework of the applied problem we are solving, only one destabilizing factor is considered, due to the pulse current i p (t) flowing through the electric wires and cables with various ATPs. At certain (threshold) values I mpk of the amplitude I mp of current pulses i p (t) of one or another temporal shape flowing through the current-carrying parts (inner core and outer shell) of the CWP, due to the intense Joule heating of these metal parts of the wires (cables), processes of thermal destruction in their belt insulation can occur [1,6,7]. It should be noted that at values of the amplitudes I mp of pulse currents i p (t) of hundreds of kiloamperes, destructive processes in the polymer insulation of the studied CWP can also arise from the action of large electrodynamic forces on cables (wires) [2].…”
Section: State-of-the-art and Urgency Of The Problemmentioning
confidence: 99%
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“…Within the framework of the applied problem we are solving, only one destabilizing factor is considered, due to the pulse current i p (t) flowing through the electric wires and cables with various ATPs. At certain (threshold) values I mpk of the amplitude I mp of current pulses i p (t) of one or another temporal shape flowing through the current-carrying parts (inner core and outer shell) of the CWP, due to the intense Joule heating of these metal parts of the wires (cables), processes of thermal destruction in their belt insulation can occur [1,6,7]. It should be noted that at values of the amplitudes I mp of pulse currents i p (t) of hundreds of kiloamperes, destructive processes in the polymer insulation of the studied CWP can also arise from the action of large electrodynamic forces on cables (wires) [2].…”
Section: State-of-the-art and Urgency Of The Problemmentioning
confidence: 99%
“…where δ=Δ p /T p is the current damping coefficient; ω=2π/T p is the circular frequency of current oscillations; T p is the period of current oscillations; Δ p =ln(I mp1 /I mp3 ) is the logarithmic decrement of pulse current i p (t) oscillations with the first I mp1 and the third I mp3 amplitudes in electrical circuits; k p2 =[exp(-Δ p /2π•arcctgΔ p /2π)sin(arcctgΔ p /2π)] -1 is the normalizing factor for the damped sinusoidal current i p (t) flowing in the wire (cable). For the temporal shape (7) of the change in the wire (cable) of the current pulse i p (t) at t p =3T p in (2), the calculation expression for the action integral J CiA of the current pulse i p (t) flowing in the investigated low-and high-current circuits of modern electrical engineering takes the following approximate analytical form:…”
Section: State-of-the-art and Urgency Of The Problemmentioning
confidence: 99%
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