Waste of energy

Many household electric appliances, for example transformers or motors, have inductive components. The electric utility company does not like to have an inductive load on its distribution network and it requires that a capacitor should be applied so that the inductive component is "compensated". Read more about this issue by searching for "power factor" or "cos phi factor".

To illustrate the advantage of having a compensating capacitor, consider the two electric circuits shown in the Figure. The resistor r = 1 Ω r=1\Omega represents the resistance of the distribution network that is driven by an ideal AC voltage source of voltage V = 110 V V=110V . The inductor L L and the resistor R R represent the appliance, with a capacitor C C added for compensation.

We will select numbers corresponding to a situation when the appliance does not use much power. The inductive impedance will be ω L = X L = 250 Ω \omega L = X_L=250\Omega and the load resistance is R = 25 Ω R=25\Omega . The capacitance, if present, will be selected so that the impedance of the whole L , R , C L,R,C circuit is purely resistive (does not have a phase shift between the voltage and the current).

Calculate P 1 P_1 , the power lost in the transmission network for the circuit without the capacitor, and P 2 P_2 , the power lost in the transmission network when the compensating capacitor is present. What is the ratio P 2 / P 1 P_2/P_1 , expressed in percentage? (Pick the number closest to your answer.)

(Inspired by Steven Chase's problem . )

1 % 0.1 % 0.01 % 10 % 100 %

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1 solution

Laszlo Mihaly
Jan 29, 2018

We are using complex values, with j = 1 j=\sqrt{-1} .

For the first circuit the impedance is Z = R + j ω L = R + j X L Z=R+j\omega L=R+jX_L (a resitor and inductor in series). The current is I = V r + R + j X L I=\frac{V}{r+R+j X_L} and the power loss is

P 1 = I 2 r = V 2 r ( r + R ) 2 + X L 2 P_1=|I|^2 r =V ^2 \frac{r}{(r+R)^2+ X_L^2} .

In the second circuit the impedance is

1 1 / ( R + j X L ) + j X C = 1 R / ( R 2 + X L 2 ) j X L / ( R 2 + X L 2 ) + j X C \frac{1}{1/(R+jX_L)+jX_C}= \frac{1}{R/(R^2+X_L^2)-jX_L/(R^2+X_L^2)+jX_C} ,

where X C X_C is the impedance of the capacitor. This quantity is real if j X L / ( R 2 + X L 2 ) 2 + j X C = 0 -jX_L/(R^2+X_L^2)^2+jX_C =0 and then the impedance is a real number, ( R 2 + X L 2 ) / R = R + X L 2 / R (R^2+X_L^2)/R=R+X_L^2/R . The current is I = V r + R + X L 2 / R I=\frac{V}{r+R+ X_L^2/R} and the power loss is

P 2 = I 2 r = V 2 r ( r + R + X L 2 / R ) 2 P_2=|I|^2 r =V ^2 \frac{r}{(r+R + X_L^2/R)^2} .

The ratio is P 2 / P 1 = ( r + R ) 2 + X L 2 ( r + R + X L 2 / R ) 2 = 0.00990 1 % P_2/P_1=\frac{(r+R)^2+ X_L^2}{(r+R + X_L^2/R)^2}=0.00990\approx 1\% . In fact, with the numbers we have, we can take the limit of r < < X L r<<X_L and R < < X L R<<X_L and this quantity is P 2 / P 1 R 2 X L 2 = 0.01 P_2/P_1\approx \frac{R^2}{X_L^2}=0.01 .

With the numbers we have the appliance consumes about 5W of power. Without the capacitor the loss in the network is 0.2W. Although this is not much, with many households the losses add up to a substantial energy waste. The saving is very significant.

Could one add the capacitor in series with the inductance (and resistor) in the second circuit, as an alternative?

Peter Baumgart - 3 years, 2 months ago

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If they are in series, the current in the motor will be very small. That is not good for the operation of the motor. When the capacitor is in parallel large current can flow back and forth between the motor and the capacitor.

Laszlo Mihaly - 3 years, 2 months ago

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I C. Thanks... (Of course for the AC situation, a large current could flow through a capacitor in series, but the capacitance would have to be large, at least for modest omega (like 60 Hz) and the device possibly too bulky, correct?)

Peter Baumgart - 3 years, 2 months ago

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