Chapter 5 AC electricity

While direct current (DC) refers to the flow of electrical charge carriers in a continuous direction, alternating current (or AC) refers to a periodic reversal of charge flow direction1 . As a mode of transferring electrical power, AC is tremendously useful because it allows us to use transformers to easily and efficiently step voltage up or down at will. If an electro-physical sensor senses a physical quantity that oscillates, the electric signal it produces will oscillate (AC) as well. For both these reasons, an instrument technician needs to be aware of how AC circuits work, and how to understand them mathematically.

5.1 RMS quantities

It is often useful to express the amplitude of an alternating quantity such as voltage or current in terms that are equivalent to direct current (DC). Doing so provides an “apples-to-apples” comparison between AC and DC quantities that makes comparative circuit analysis much easier.

The most popular standard of equivalence is based on work and power, and we call this the root-mean-square value of an AC waveform, or RMS for short. For example, an AC voltage of 120 volts “RMS” means that this AC voltage is capable of delivering the exact same amount of power (in Watts) at an electrical load as a 120 volt DC source powering the exact same load.

The problem is exactly how to calculate this “RMS” value if all we know about the AC waveform is its peak value. If we compare a sine wave and a DC “wave” side by side, it is clear that the sine wave must peak at a greater value than the constant DC level in order to be equivalent in terms of doing the same work in the same amount of time:

At first, it might seem like the correct approach would be to use calculus to integrate (determine the area enclosed by) the sine wave over one-half of a cycle: from 0 to π radians. This is close, but not fully correct. The ability of an electrical voltage to dissipate power at a resistor is not directly proportional to the magnitude of that voltage, but rather proportional to the square of the magnitude of that voltage! In mathematical terms, resistive power dissipation is predicted by the following equation:

P = V2-

If we double the amount of voltage applied to a resistor, the power increases four-fold. If we triple the voltage, the power goes up by a factor of nine. If we are to calculate the “RMS” equivalent value of a sine wave, we must take this nonlinearity into consideration.

First let us begin with a mathematical equivalence between the DC and AC cases. For DC, the amount of work done is equal to the constant power of that circuit multiplied by time. The unit of measurement for power is the Watt, which is defined as 1 Joule of work per second. So, multiplying the steady power rate in a DC circuit by the time we keep it powered will result in an answer of joules (total energy dissipated by the resistor):

       (  2 )
Work =   V-- t

Showing this equivalence by dimensional analysis:

         (       )
[Joules] =   [s]   [s]

We cannot calculate the work done by the AC voltage source quite so easily, because the power dissipation varies over time as the instantaneous voltage rises and falls. Work is still the product of power and time, but we cannot simply multiply one by the other because the voltage in this case is a function of time ((t)). Instead, we must use integration to calculate the product of power and time, and sum those work quantities into a total work value.

Since we know the voltage provided by the AC source takes the form of a sine wave ((t) = sinif we assume a sine wave with a peak value of 1 volt), we may write the formula for instantaneous AC power as follows:

             2      2
Power = (V-(t))-= sin-t
           R       R

To calculate the work done by this sinusoidal voltage on the resistor, we will integrate this instantaneous power with respect to time, between the intervals of = 0 and π (one half-cycle of the sine wave):

       ∫ π sin2-t
Work =  0  R   dt

In order to solve for the amount of DC voltage equivalent (from the perspective of resistive power dissipation) to a one-volt AC sine wave, we will set the DC work and AC work equations equal to each other, making sure the DC side of the equation has π for the amount of time (being the same time interval as the AC side):

(  2)     ∫ π   2
  V-- π =    sin-tdt
  R        0   R

Our goal is to solve for on the left-hand side of this equation.

First, we know that is a constant value, and so we may move it out of the integrand:

(    )      ∫ π
  V-2 π = 1-    sin2tdt
  R       R  0

Multiplying both sides of the equation by eliminates it completely. This should make intuitive sense, as our RMS equivalent value for an AC voltage is defined strictly by the ability to produce the same amount of power as the same value of DC voltage for any resistance value. Therefore the actual value of resistance (R) should not matter, and it should come as no surprise that it cancels:

      ∫ π
V 2π =    sin2tdt

Now, we may simplify the integrand by substituting the half-angle equivalence for the sin2t function

V 2π =  π 1−-cos2tdt
       0     2

Factoring one-half out of the integrand and moving it outside (because it’s a constant):

       ∫ π
V2π = 1    1− cos2tdt
      2 0

We may write this as the difference between two integrals, treating each term in the integrand as its own integration problem:

 2    1( ∫ π     ∫ π       )
V π = 2     1dt−     cos2t dt
          0       0

The second integral may be solved simply by using substitution, with = 2tdu = 2 dt, and dt du 2 :

        ( ∫       ∫         )
V 2π = 1   π 1dt−   π cos-udu
       2   0       0   2

Moving the one-half outside the second integrand:

        (∫ π       ∫ π       )
V2π = 1     1 dt− 1    cosu du
      2   0       2 0

Finally we are at a point where we may perform the integrations:

        (∫         ∫         )
V2π = 1    π1 dt− 1  π cosu du
      2   0       2 0
        (              )
V 2π = 1 [t]π0 − 1[sin2t]π0
      2        2
  2    1(         1           )
V  π = 2 [π − 0]− 2[sin2π− sin0]
      1(         1     )
V2π = -  [π − 0]− -[0 − 0]
      2          2
  2    1
V  π = 2(π− 0)
V2π = -π

We can see that π cancels out of both sides:

V2 = 1

Taking the square root of both sides, we arrive at our final answer for the equivalent DC voltage value:

V = √2

So, for a sinusoidal voltage with a peak value of 1 volt, the DC equivalent or “RMS” voltage value would be approximately 0.707 volts. In other words, a sinusoidal voltage of 1 volt peak will produce just as much power dissipation at a resistor as a steady DC voltage of 0.7071 volts applied to that same resistor. Therefore, this 1 volt peak sine wave may be properly called a 0.7071 volt RMS sine wave, or a 0.7071 volt “DC equivalent” sine wave.

This factor for sinusoidal voltages is quite useful in electrical power system calculations, where the wave-shape of the voltage is nearly always sinusoidal (or very close). In your home, for example, the voltage available at any wall receptacle is 120 volts RMS, which translates to 169.7 volts peak.

5.2 Resistance, Reactance, and Impedance

Resistance (R) is the dissipative opposition to an electric current, analogous to friction encountered by a moving object. In any example of electrical resistance, the electrical energy is converted into some other form of energy that cannot (or does not) return back to the circuit. Resistance may take the form of an actual resistor, in which case the electrical energy is converted into heat. Resistance may also take the form of an electric motor, an electric light, or an electrochemical cell where the electrical energy is converted into mechanical work, photons, or enables an endothermic chemical reaction, respectively.

Reactance (X) is the opposition to an electric current resulting from energy storage and release between certain components and the rest of the circuit, analogous to inertia of a moving object. Capacitors and inductors are classic examples of “reactive” electrical components, behaving either as electrical loads or as electrical sources depending on whether the applied electrical signal is increasing or decreasing in intensity at that instant in time. When a purely reactive component is subjected to a sinusoidal signal, it will spend exactly half the time behaving as a load (absorbing energy from the circuit) and half the time behaving as a source (returning energy to the circuit). Thus, a purely reactive component neither contributes nor dissipates any net energy in the circuit, but merely exchanges2 energy back and forth. Even though the fundamental mechanism of reactance (energy storage and release) is different from the fundamental mechanism of resistance (energy conversion and dissipation), reactance and resistance are both expressed in the same unit of measurement: the ohm (Ω).

Impedance (Z) is the combined total opposition to an electric current, usually some combination of electrical resistance (energy dissipation) and electrical reactance (energy storage and release). It is also expressed in the unit of the ohm. In order to represent how much of a particular impedance is due to resistance and how much is due to reactance, the value of an impedance may be expressed as a complex number with a “real” part (representing resistance) and an “imaginary” part (representing reactance). This concept will be explored in much more detail later in this chapter.

The amount of electrical reactance offered by a capacitor or an inductor depends on the frequency of the applied signal. The faster the rate at which an AC signal oscillates back and forth, the more a reactive component tends to react to that signal. The formulae for capacitive reactance (XC) and inductive reactance (XL) are as follows:

XC  = 2πfC-         XL = 2πf L

Just as conductance (G) is the reciprocal of resistance (1 ∕ R), a quantity called susceptance (B) is the reciprocal of reactance (1 ∕ X). Susceptance is useful when analyzing parallel-connected reactive components while reactance is useful for analyzing series-connected reactive components, in much the same way that conductance and resistance are useful when analyzing parallel-connected and series-connected resistors, respectively.

Impedance (Z) also has a reciprocal counterpart known as admittance ().

5.3 Series and parallel circuits

Impedance in a series circuit is the orthogonal sum of resistance and reactance:

    ∘ ---------------
Z =   R2 + (X2  − X2 )
             L    C

Equivalent series and parallel circuits are circuits that have the exact same total impedance as one another, one with series-connected resistance and reactance, and the other with parallel-connected resistance and reactance. The resistance and reactance values of equivalent series and parallel circuits may be expressed in terms of those circuits’ total impedance:

If the total impedance of one circuit (either series or parallel) is known, the component values of the equivalent circuit may be found by algebraically manipulating these equations and solving for the desired R and values:

Z2 = RseriesRparallel                  Z2 = XseriesXparallel

Back to Main Index of Book