Three capacitors with values of 10 μF, 30 μF, and 15 μF are connected in series to a 480-V, 60-Hz line (Figure 21–11). Find the following circuit values:
X_{C1}—capacitive reactance of the first capacitor
X_{C2}—capacitive reactance of the second capacitor
X_{C3}—capacitive reactance of the third capacitor
X_{CT}—total capacitive reactance for the circuit
C_T—total capacitance for the circuit
I_T—total circuit current
E_{C1}—voltage drop across the first capacitor
VARs_{C1}—reactive power of the first capacitor
E_{C2}—voltage drop across the second capacitor
VARs_{C2}—reactive power of the second capacitor
E_{C3}—voltage drop across the third capacitor
VARs_{C3}—reactive power of the third capacitor
VARs_{CT}—total reactive power for the circuit
Since the frequency and the capacitance of each capacitor are known, the capacitive reactance for each capacitor can be found using the formula
X_C=\frac{1}{2πfC}
Recall that the value for C in the formula is in farads and the capacitors in this problem are rated in microfarads.
X_{C1}=\frac{1}{2πfC}
X_{C1}=\frac{1}{377×0.000010}
X_{C1}=265.252\ Ω
X_{C2}=\frac{1}{2πfC}
X_{C2}=\frac{1}{377×0.000030}
X_{C2}=88.417\ Ω
X_{C3}=\frac{1}{2πfC}
X_{C3}=\frac{1}{377×0.000015}
X_{C3}=176.835\ Ω
Since there is no phase angle shift between any of the three capacitive reactances, the total capacitive reactance is the sum of the three reactances (Figure 21–12):
X_{CT}=X_{C1}+X_{C2}+X_{C3}
X_{CT}=265.252\ Ω+88.417\ Ω+176.835\ Ω
X_{CT}=530.504\ Ω
The total capacitance of a series circuit can be computed in a manner similar to that used for computing parallel resistance. Refer to the Pure Capacitive Circuits Formula section of Appendix D. Total capacitance in this circuit is computed using the formula
C_T=\frac{1}{\frac{1}{C_1}+\frac{1}{C_2}+\frac{1}{C_3}}
C_T=\frac{1}{\frac{1}{10\ μF}+\frac{1}{30\ μF}+\frac{1}{15\ μF}}
C_T=\frac{1}{0.2\frac{1}{μF}}
C_T=5\ μF
The total current can be found by using the total capacitive reactance to substitute for R in an Ohm’s law formula:
I_T=\frac{E_{CT}}{X_{CT}}
I_T=\frac{480\ V}{530.504\ Ω}
I_T=0.905\ A
Since the current is the same at any point in a series circuit, the voltage drop across each capacitor can now be computed using the capacitive reactance of each capacitor and the current flowing through it.
E_{C1}=I_{C1}×X_{C1}
E_{C1}=0.905×265.25
E_{C1}=240.051\ V
E_{C2}=I_{C2}×X_{C2}
E_{C2}=0.905×88.417
E_{C2}=80.017\ V
E_{C3}=I_{C3}×X_{C3}
E_{C3}=0.905×176.83
E_{C3}=160.031\ V
Now that the voltage drops of the capacitors are known, the reactive power of each capacitor can be found.
\text{VARs}_{C1}=E_{C1}×I_{C1}
\text{VARs}_{C1}=240.051×0.905
\text{VARs}_{C1}=217.246
\text{VARs}_{C2}=E_{C2}×I_{C2}
\text{VARs}_{C2}=80.017×0.905
\text{VARs}_{C2}=72.415
\text{VARs}_{C3}=E_{C3}×I_{C3}
\text{VARs}_{C3}=160.031×0.905
\text{VARs}_{C3}=144.828
Power, whether true power, apparent power, or reactive will add in any type of circuit. The total reactive power in this circuit can be found by taking the sum of all the VARs for the capacitors or by using total values of voltage and current and Ohm’s law:
\text{VARs}_{CT}=\text{VARs}_{C1}+\text{VARs}_{C2}+\text{VARs}_{C3}
\text{VARs}_{CT}=217.248+72.415+144.828
\text{VARs}_{CT}=434.491
The circuit with all computed values is shown in Figure 21–13.
Appendix D
Metal | Sym. | Spec. grav. | Melt Point °C °F |
Elec. Cond. % copper |
Lb/in.3 | |
Aluminum | Al | 2.710 | 660 | 1220 | 64.9 | 0.0978 |
Antimony | Sb | 6.620 | 631 | 1167 | 4.42 | 0.2390 |
Arsenic | As | 5.730 | 4.90 | 0.2070 | ||
Beryllium | Be | 1.830 | 1287 | 2336 | 9.32 | 0.0660 |
Bismuth | Bi | 9.800 | 271 | 512 | 1.50 | 0.3540 |
Brass (70–30) | 8.510 | 900 | 1652 | 28.0 | 0.3070 | |
Bronze (5% Sn) | 8.870 | 1000 | 1382 | 18.0 | 0.3200 | |
Cadmium | Cd | 8.650 | 321 | 610 | 22.7 | 0.3120 |
Calcium | Ca | 1.550 | 842 | 1562 | 50.1 | 0.0560 |
Cobalt | Co | 8.900 | 1495 | 2723 | 17.8 | 0.3210 |
Copper | Cu | 8.900 | 1085 | 1981 | 100.0 | 0.3210 |
Gold | Au | 19.30 | 1064 | 1945 | 71.2 | 0.6970 |
Graphite | 2.250 | 3500 | 6332 | 0.001 | 0.0812 | |
Indium | In | 7.300 | 156 | 311 | 20.6 | 0.2640 |
Iridium | Ir | 22.40 | 2446 | 4442 | 32.5 | 0.8090 |
Iron | Fe | 7.200 | 1400 to 1500 |
2552 to 2732 |
17.6 | 0.2600 |
Malleable | 7.200 | 1600 to 1500 |
2912 to 2732 |
10.0 | 0.2600 | |
Wrought | 7.700 | 1600 | 2912 | 10.0 | 0.2780 | |
Lead | Pb | 11.40 | 327 | 621 | 8.35 | 0.4120 |
Magnesium | Mg | 1.740 | 650 | 1204 | 38.7 | 0.0628 |
Manganese | Mn | 7.200 | 1246 | 2273 | 0.90 | 0.2600 |
Mercury | Hg | 13.65 | —38.8 | —37.7 | 1.80 | 0.4930 |
Molybdenum | Mo | 10.20 | 2623 | 4748 | 36.1 | 0.3680 |
Monel (63–37) | 8.870 | 1300 | 2372 | 3.00 | 0.3200 | |
Nickel | Ni | 8.90 | 1455 | 2646 | 25.0 | 0.3210 |
Phosphorus | P | 1.82 | 44.2 | 111.6 | 10^{-17} | 0.0657 |
Platinum | Pt | 21.46 | 1768 | 3214 | 17.5 | 0.0657 |
Metal | Sym. | Spec. grav. | Melt Point °C °F |
Elec. Cond. % copper |
Lb/in.3 | |
Potassium | K | 0.860 | 63.0 | 146.1 | 28.0 | 0.0310 |
Selenium | Se | 4.81 | 221 | 430 | 14.4 | 0.1740 |
Silicon | Si | 2.40 | 1414 | 2577 | 10^{-5} | 0.0866 |
Silver | Ag | 10.50 | 962 | 1764 | 106 | 0.3790 |
1330 | 2436 | |||||
Steel (carbon) | 7.84 | to 1380 | to 2516 | 10.0 | 0.2830 | |
Stainless | ||||||
(18–8) | 7.92 | 1500 | 2732 | 2.50 | 0.2860 | |
(13–Cr) | 7.78 | 1520 | 2768 | 3.50 | 0.2810 | |
(18–Cr) | 7.73 | 1500 | 2732 | 3.00 | 0.2790 | |
Tantalum | Ta | 16.6 | 3017 | 5462 | 13.9 | 0.5990 |
Tellurium | Te | 6.20 | 450 | 846 | 10^{-5} | 0.2240 |
Thorium | Th | 11.7 | 1750 | 3182 | 9.10 | 0.4220 |
Tin | Sn | 7.30 | 232 | 449 | 15.0 | 0.2640 |
Titanium | Ti | 4.50 | 1668 | 3034 | 2.10 | 0.1620 |
Tungsten | W | 19.3 | 3422 | 6181 | 31.5 | 0.6970 |
Uranium | U | 18.7 | 1135 | 2075 | 2.80 | 0.6750 |
Vanadium | V | 5.96 | 1910 | 3470 | 6.63 | 0.2150 |
Zinc | Zn | 7.14 | 420 | 788 | 29.1 | 0.2580 |
Zirconium | Zr | 6.40 | 1855 | 3371 | 4.20 | 0.2310 |