The unshielded cables of LV networks lie parallel and close
to each other. Therefore, these wires are closely coupled via mutual
crosstalk. The line resonances of single wires are damped
by transferring power through crosstalk to other lines [11]. The
resistance of the single cables is quite high, caused by small
wire diameters, and, consequentially, the Q-factor of cable resonances
is low. Regarding narrowband resonances with high
Q-factor the LV network harness is rather kind [11]. In contrast,
HV networks have high conductor diameters and the shielding
effectively prevents crosstalk between the lines. Thus, line
resonances of HV networks have a high Q-factor and cable
resonances are hardly damped [12], [19].