As we saw earlier in the construction of Underground cables, a cable is basically a set of one (or three) conductors surrounded by a metallic sheath. This arrangement can be considered as a set of two long, coaxial, cylinders, separated by insulation. The current carrying conductor forms the inner cylinder while the metallic sheath acts as the outer cylinder. The sheath is grounded, and hence voltage difference appears across the cylinders. The dielectric fills the space between the charged plates (cylinders), making it a capacitor. Hence, capacitance of the cable becomes a very important aspect, and must be calculated.
Capacitance of single core cableA single core cable can be represented as shown below.
r = radius of the inner conductor and d = 2r
R = radius of the sheath and D = 2R
ε0 = permittivity of free space = 8.854 x 10-12
εr = relative permittivity of the medium
Consider a cylinder of radius x meters and axial length 1 meter. x be such that, r < x < R.
Now, electric intensity Ex at any point P on the considered cylinder is given as shown in the following equations.
Then, the potential difference between the conductor and sheath is V, as calculated in equations below.
After that, capacitance of the cable can be calculated as C= Q/V
When the capacitance of a cable is known, then its capacitive reactance is given by Xc = 1/(2πfC) Ω.
Then the charging current of the cable can be given as,
Ic= Vph / Xc A
Capacitance of three core cableConsider a three cored symmetric underground cable as shown in the following figure (i). Let Cs be the capacitance between any core and the sheath and Cc be the core to core capacitance (i.e. capacitance between any two conductors).
In the above figure (ii), the three Cc (core to core capacitance) are delta connected and the core to sheath capacitance Cs are star connected due to the sheath forming a single point N. The circuit in figure (ii) can be simplified as shown in figure (iii). Outer points A, B and C represent cable cores and the point N represents the sheath (shown at the middle for simplification of the circuit).
Therefore, the whole three core cable is equivalent to three star connected capacitors each of capacitance Cs + 3Cc as shown in fig. (iii).
The charging current can be given as,
Ic = 2πf(Cs+3Cc)Vph A
Measurement of Cs and CcIn order to calculate Cs and Cc we perform various experiments like:
- First, the three cores are connected together and capacitance between the shorted cores and the sheath is measured. Shorting the three cores eliminates all the three Cc capacitors, leaving the three Cs capacitors in parallel. Therefore, if C1 is the now measured capacitance, Cs can be calculated as, Cs = C1/3.
- In the second measurement, any two cores and the sheath are connected together and the capacitance between them and the remaining core is measured. If C2 is the measured capacitance, then C2 = 2Cc+Cs (imagine the above figure (iii) in which points A, B and N are short circuited). Now, as the value of Cs is known from the first measurement, Cc can be calculated.