validating the effect of rise-slope in transient response of grounding system

Upload: bin-nguyen

Post on 05-Apr-2018

217 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    1/6

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    2/6

    Fig. 1. Transmission line circuit for an electrode

    The equations (1) can be presented by a equivalent circuit in Fig.1. In this,R,L(x,t), G(x,t) and

    C(x,t) are per-unit length resistance, inductance, conductance and capacictance of the electrode,

    respectively. These parameters are functions of space and time which can be calculated detailedly in

    [1].

    The grounding system and lightning current used for simulation

    A typical grounding system under towers of telecomunication or wireless systems is presented

    in Fig. 2. The three vertical grounding copper electrodes are 7.5mm in radius and 15m long. They

    are connected by copper wires which are 5mm in radius. The electrodes resistivity used in

    calculation is . The grouding system is buried at 0.5m depth in the soil which

    has relative permittivity and resistivity . In simulation, the lightning current is

    assumed to be conducted into the injected point and the mutual effect of the uper-soil structures as

    well as the skin-effect is neglected.

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    3/6

    Fig. 2. A grounding system for simulation

    The lightning currents are described as a double exponetial function () ( )

    with the rise-time, changing in a range from 1s to 8s. Besides, in oder to compare the effect of

    the lightning currents rise-time, these currents all have the same peak value of 1 kA. These

    ligntning currents parameters and wave-forms are shown in Tab. 1 and Fig. 3.

    Table 1. Parameter of lightning currents

    Num (s) Im(kA) a(s-1) b(s-1)

    1 1 1.029 23925 5452900

    2 2 1.062 24779 2287300

    3 3 1.101 25696 1345000

    4 4 1.146 26685 908650

    5 5 1.199 27750 662230

    6 6 1.261 28896 506050

    7 7 1.336 30150 3991908 8 1.426 31511 322060

    -5

    0

    5

    -5

    0

    5

    -20

    -15

    -10

    -5

    0

    5

    x(m)y(m)

    z(m)

    3 vertical

    groudingcopperelectrodes

    Connecting

    copper wires

    3m

    3m

    3mair

    15m 15m

    15m

    soil

    injectedpoint

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    4/6

    Fig. 3. Lightning current wave forms

    Simulation results

    Table 2. Peak value of over-voltages at the injected point when the rise-time changes from

    1s to 8s

    ( s ) 1 2 3 4 5 6 7 8

    Peak value (kV) 6,722 4,543 3,662 3,177 2,929 2,823 2,692 2,539

    0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2

    x 10-5

    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    t(s)

    Is(kA)

    1

    2

    34

    5

    6

    7

    8

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    5/6

    Fig. 4. Over-voltage at the injected point when the rise-time changes from 1s to 8s

    Fig. 5. Peak value of over-voltage at the injected point varies with the rise-time

    0 2 4 6 8

    x 10-6

    2

    2.5

    3

    3.5

    4

    4.5

    5

    5.5

    6

    6.5

    7

    s(s)

    Upeak(kV)

  • 8/2/2019 Validating the Effect of Rise-slope in Transient Response of Grounding System

    6/6

    From the simulation results in Fig. 4, 5 and Tab. 2, the smaller the rise-time is, the higher the

    over-voltage on the grounding systems is. That means the transient response on grounding systems

    is affected significantly by the rise-slope of the lightning current. The reason is that the inductance

    along electrodes of grounding systems can prevent the impulse current from passing by, and hence

    decrease the ability of grounding systems in dissipating this current into the surrounding ground.

    Conclusion

    Non-uniform transmission line model is applied to simulate the transient phenomenon of

    grounding systems in this research. Through the simulation results, the considerable effect of the

    rise-slope of the lightning currents to this issue can be clarify. This influcence can be sumarized

    briefly as the steeper this parameter is, the less effective the grounding systems are in distributing

    the lightning currents into the ground. Hence, grounding systems used for lightning protection have

    to be limited in their length or their building area to reduce the effect of inductances along their

    component electrodes.

    References

    [1]Yaqing Liu, Nelson Theethayi, and Rajeev Thottappillil, Member, IEEE An engineering modelfor transient analysis of grounding system under lightning strikes: Nonuniform transmission-line

    approach, IEEE Trans. Power Del, vol. 20, no. 2, pp. 722 730 , Apr 2005