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a smart grid application – street lighting ... - Scientific Bulletin

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316 Dan Simhas, Claudiu Popovici<br />

ΔU<br />

ΔU [%] = ⋅100<br />

(2)<br />

U spl<br />

where U spl is the actual supply phase voltage of the network.<br />

Voltage drop formula [15] is considered:<br />

where:<br />

r ⋅ P + x ⋅Q<br />

1<br />

(3)<br />

1 1<br />

ΔU<br />

p<br />

=<br />

U<br />

spl<br />

r 1 – specific resistance [Ω/m],<br />

x 1 – inductive reactance [Ω/m],<br />

P, Q – active and reactive phase power [kW], [kVAr].<br />

Considering a constant power factor cos φ for every P k , Q k it can be written:<br />

Using (4) and (3),<br />

For the first lamp, (1) becomes:<br />

P<br />

Q<br />

P<br />

k<br />

Q<br />

= tgϕ<br />

(4)<br />

P<br />

k<br />

=<br />

( r + x ⋅tgϕ)<br />

P<br />

U<br />

1<br />

(5)<br />

1 1<br />

Δ<br />

p<br />

=<br />

U<br />

spl<br />

= P ⋅( K + K ⋅ ΔU<br />

1[%])<br />

(6)<br />

L1 N 1 2 p<br />

Power losses in the lamps power supply line [16] are computed:<br />

where:<br />

r<br />

2 2<br />

⋅ l ⋅ ( Ea<br />

+ Er<br />

)<br />

( U ⋅T<br />

) 2<br />

ΔP pl – are power losses of the supply wire [kW],<br />

0<br />

Δ Ppl<br />

=<br />

(7)<br />

spl int

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