Voltage Drop and Branching Circuit Design Calculations

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Voltage Drop and Branching Circuit Design Calculations Week 5-6-7

Voltage considerations Nominal Voltage The nominal voltage is the voltage by which the system is designated for example 230/400V, 400/690V, 120/208V etc. Rated values for 3ph IM Rated Voltage This is the nameplate voltage and it is the voltage at which the equipment is designed to operate for optimal performance.

Voltage considerations Service voltage The service voltage is the voltage at the point where the electrical of the supplier and the user are interconnected. This is normally at the meter. Maintaining an acceptable voltage at the service entrance is the utility s responsibility. Utilization voltage This is the voltage at the line terminals of utilization equipment. It is less than the service voltage by the amount of voltage drop in the facility from the service point to the utilization point. This voltage is the facility s responsibility. Equipment manufacturers should design equipment which operates satisfactorily within the specified limits. These limits allow for some voltage drop within a facility, so service voltage requirements are tighter than utilization requirements.

IEC and ANSI Standards European Union The voltage tolerance permitted depends on the prevailing standard in use. Today there are, the European IEC60034-1 and IEC60038 and the American ANSI C84.1. In the European Union the nominal voltages are now 230/400V with a tolerance range of±10% for equipment in general and of±5% for rotating electrical equipments. The ±10% limits set the voltage at 253/440V maximum and 207/360V minimum. The ± 5% limits set the voltages at 242/420V maximum and 218/380V minimum.

IEC and ANSI Standards United states In the United States the standard established two ranges for voltage variations designated as Range A and Range B. Basically Range A utilization voltage range is ±5% of nominal and Range B has the asymmetric range +6% to 12% of nominal. Utilization equipment is to be designed to give fully satisfactory operation throughout range A limits for utilization voltages. Range B allows for voltages above and below Range A limits. According to the standard when voltages are outside range A but inside range B, they shall be limited in duration, extent and frequency, and corrective measures should be taken within a reasonable time to restore the service voltage to range A limits.

Voltage profile diagram

Why do we need voltage drop calculations? 1% voltage drop can lead to reduction in tungsten lamp illumination by 3% Some home appliances which are operated by motors can be affected by reduction in voltage (P=VI cos (pi)) Reduction in voltage level will be accompanied by a rise in current level in circuit Since this voltage drop is within the 10% decrease, current will normally increase within the same limits without any tripping of the circuit breaker. On the long run, equipment will suffer from 10% current increase that could lead to equipment failure due to gradual temperature rise.

Voltage drop calculations in single phase circuit: V 1 Z=R+jX V 2 Voltage at the sending end P r +jq r Voltage at the receiving end = =2 = = = = = For each conductor, we call it go and return % = If you have more than one tap point in the same line i.e more points between V1 and V2, multiply each load by the distance TIBTECH Electrical conductivity (10.E6 Siemens/m) copper 58,5 1,7 Aluminium 36,9 2,7 Electrical resistivity (10.E-8 Ohm.m) Some of these values are smaller as they depend on the purity of copper so its subject to manufacturer data

حساب تیار قصر الدارة calculation: Short circuit Current Assume rated voltage is 220V, single phase, resistive load, copper cables are used whose cross section area is 6 mm2. Calculate voltage drop 6kW 4kW 2.5kW 1kW 20m 10m 10m 6m 2kW 1.5kW 1.5kW 1kW % = = 6 20+4 10+2.5 10+1 6 =2.35%

Voltage Drop Calculations 1. Radial-type feeder with one tapped-off load V s Z=R+jX V r P r +jq r = +IZ = +I.R.(cos φ)+i.x.(sin φ) I.R.cosφ+I.x.sin φ

= cos + sin R& X= ohms r & x= ohm/ unit length = 3 cos +3 sin + 3 ( ) ثابت= k 1 3 1000 : : r & x : Theeffectivelengthof thefeeder main(inkm) Thethree-phasekVA-Loading The resistance and inductive reactance parameters of the feeder main in Ohm/km. K: TheK-parameterinpu voltagedrop per kva-km is considered 0.9 as it is regulated and depends on the loads. Residential are usually higher than 0.9

2. Radial-type feeder with multi tapped-off loads V s V 1 Z 1 =R 1 +jx 1 Z 2 =R 2 +jx 2 O I 1 A I 2 P L 1 +jq L1 I r B P L 2 +jq L2 VD I 1 (R 1 cosψ 1 +X 1 sinψ 1 )+ I L 2 (R 2cosφ 2 +X 2 sinφ 2 ) V s Single line diagram V 1 0 o r + jx is the impedance per unitlengthofthefeedermain φ 1 φ 2 V r I 2 =I L 2 VD n VD = I L i l i (rcosφ i +xsinφ i ) i=1 I L 1 Phasor diagram o I 1 =I 1 ψ 1

3. Radial-type feeder with uniformly distributed load Many times it can be assumed that loads are uniformly distributed along a line where the line can be a three-phase, or a single-phase feeder or lateral. This is certainly the case on single phase laterals where the same rating transformers are spaced uniformly over the length of the lateral. When load is uniformly distributed, its not necessary to model each load in order to determine the voltage drop from source end to the last load. In the case of a uniformly distributed load, load densityis given in (kva/km2) as well as the total area which the load is occupying MV radial-type primary feeder with uniformly distributed load Distribution transformer H.R.C.F Low-voltage feeders Tapped-off distribution transformer load In this case, the total load is represented by a single load at the mid distance

حساب تیار قصر الدارة Calculation: Short Circuit Current Short circuit current is the current flowing in an electrical circuit due to fault occurrence which is different than the normal current (could reach 10 times more than normal current) Short circuit could be : Symmetric (3phase), unsymmetrical (two phase, two phase to earth, single phase to earth) Most occurred one is single phase to earth and symmetric 3 phase fault. 6kW 4kW 2.5kW 1kW 20m 10m 10m 6m 2kW 1.5kW 1.5kW 1kW Calculate short circuit current if a single phase short circuit occurred between phase a and ground, occurring at entrance of load 2

حساب تیار قصر الدارة calculation: Short circuit Current 6kW=27 A 2kW =9 A 4kW 20m 10m 10m 6m 1.5kW =6.8A 2.5kW 1.5kW =6.8A 1kW 1kW =4.5A Assume rated voltage is 220V, single phase, resistive load, copper cables are used whose cross section area is 6 mm2 = =1.78 10 30 6 10 =0.089Ω = =. =2471.94

ApplicationExamples: Asquared-shaped service area (A=9 km 2 ) withauniformly distributed load density of 400kVA/km 2 atpeakloadingand125kva/km 2 atoff-peakloading.thelumpedloadof industrial plant working three shifts a day at constant loading of 2000 kva. Primary feeders use over-head four-wire grounded bare copper conductors with manufacturer data asgivenintable1. Determine for both peak and off-peak loadings: i) The percentage voltage drop from sub-station to taping-off point a, from taping a to b, from taping b to c, and from taping c to d on the main primary feeder. ii) The line-to-ground voltages at the tapings a, b, c, and d.

OHTL 400kVA/km 2 density load Residential load 9 km 2 Tapping here is done manually by introducing more number of turns thus OHTL raising the voltage level o a b c d 1.5km 3km 1.5km Industrial load 2000-kVA 3 shift load 11kV Substation: Nominal voltage ratio 66/11-kV V ss (atpeakloading)=1.025p.uof66kv V ss (atoff-peakloading)=1.0p.uof66kv Distribution transformer: Ratings:2000kVA&11kV/380V Low-voltage tapings at operation = +5% Transformer impedance, ZT =0.0+ j0.05 pu

Manufacturer data for hard-drawn copper type conductors OHTL section Conductor Size(mm 2 ) Outside diam (mm) GMR/R ratio Resistance at 50 Hz&50 o C (Ω/km) bc 25 6.606 0.7265 1.212 oa 120 14.57 0.7581 0.16 To calculate the TL inductance parameters for OHTL, we apply the following: =2 10 ln, GMR= 0.7788 times the actual radius(r) of conductor GMD = (D1D2D3) For a GMD of 1.0 m, then: 1.026 10 ( 25 ) =2 10 ln / Inductive reactance is obtained by: =2 π 1.04 10 ( 120 )

Conductor Size (mm 2 ) Parameters in Ω/km r x L K-factor %VD per kva.km 25 1.212 0.379 0.00104 120 0.16 0.3267 0.00024 K factor calculations based on 0.9 pf: K at0.9p.f = (r 0.9+x L 0.4358) ( 1 3 1000) 100 11000 2 3 %VD-calculations at peak hours loadings: o a b c d 5600 kva 5600 kva 2000 kva 2000 kva 2000 kva 1.5 1.5 1.5 3600 kva 1.5

%VD-calculations at peak hours loadings: o a b c d 5600 kva 5600 kva 2000 kva 2000 kva 2000 kva 1.5 1.5 1.5 1.5 %VD SS a =0.00024 (5600 1.5) =2.016% %VD a b =0.00024 (5600 1.5+2000 1.5) =2.736% %VD b c =0.00104 (2000 1.5) =3.12% %V drop =(102.5 2.016 2.736 3.12)=94.628% To determine the %VDin sections c-d, transformer load current need to be determined: I Load = 2000 kva 3 (0.94628 11 kv) 3600 kva 110.93 =110.93A A= 2000 3 11 pu current The percentage of voltage reaching to the transformer after the voltage drop on the way =1.056 pu

pu Z T =0.0+j0.05 Transformer impedance is usually given in puvalues puvd cd = I Load pu (R Tcosφ+X T sinφ) V base pu 0.05 Due to tapping, which is raised by 5% so the effect is such to make an opposite effect to voltage drop = 1.056 (0.0 0.9+0.05 0.4358) 0.05= 0.027 1.0 = 2.7 (i.e. voltage rise) %VD cd %VD SS a =0.00024 (5600 1.5)=2.016% To compensate for the drop that will occur in the industrial load %VD a b =0.00024 (5600 1.5+2000 1.5)=2.736% %VD b c =0.00104 (2000 1.5)=3.12% %VD c d = 2.7%

%VD-calculations at off-peak hours loadings: Line-to-neutral bus voltages calculations at peak hours loadings V a =puv a V base =pu(v o VD oa ) V base =(1.025 0.02016) 11 =1.00484 11 =6.3816kV 3 3 V b =puv b V base =pu(v a VD ab ) V base =(1.0048 0.02736) 11 =0.97748 11 =6.20783kV 3 3 V c =puv c V base =pu(v b VD bc ) V base =(0.97748 0.0312) 11 =0.94628 11 =6.00968 kv 3 3 V d =puv d V base =pu(v c VD cd ) V base =(0.94628+0.027) 220=0.9733 220=214.12 V

o a b c d 3125 kva 3125 kva 2000 kva 2000 kva 2000 kva 1.5 1.5 1.5 1.5 km 1125 kva %VD-calculations at off-peak hours loadings: V a =puv a V base =pu(v o VD oa ) V base =(1.0.01125) 11 =0.98875 11 =6.2974kV 3 3 V b =puv b V base =pu(v a VD ab ) V base =(0.98875 0.01845) 11 =0.9703 11 =6.1622kV 3 3 V c =puv c V base =pu(v b VD bc ) V base =(0.9703 0.0312) 11 =0.9391 11 =5.9641kV 3 3 V d =puv d V base =pu(v c VD cd ) V base =(0.9391+0.027) 220=0.9661 220=212.54 V