# Module P5.4 AC circuits and electrical oscillations

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1 F L E X I B L E L E A R N I N G A P P R O A C H T O P H Y S I C S Module P5.4 Opening items. Module introduction.2 Fast track questions.3 Ready to study? 2 AC circuits 2. Describing alternating currents 2.2 AC power and rms current 2.3 AC in resistors, capacitors and inductors 2.4 Resistance, reactance and impedance 2.5 The series LCR circuit 2.6 The parallel LCR circuit 2.7 Combining series and parallel circuits 2.8 Filter circuits 3 Oscillations in electrical circuits 3. Transient currents in an RC circuit 3.2 Transient currents in an LR circuit 3.3 Oscillations in LC circuits 3.4 Damped oscillations in LCR circuits 3.5 Driven oscillations in LCR circuits 4 Closing items 4. Module summary 4.2 Achievements 4.3 Exit test Exit module

2 Opening items. Module introduction Perhaps before reading this module you should do a small electrical audit. Spend a minute or two wandering around your home looking at the electrical appliances which you find there. Most of them will have a small plate or sticker attached which tells you something about their electrical specifications. My toaster, which is quite a simple model, just says 240V 000W 50Hz. Whilst the back of my microwave which incidentally was made in France bears the more complicated legend 240V ~ 50Hz fréq.: 2450MHz MW 500W/6,5A A good deal of this information concerns the sort of power supply that the appliance requires. In both the cases quoted the appliance requires a supply of alternating current (a.c.), with a root-mean-square voltage of 240 volts and a frequency of 50 hertz. Alternating currents are the central theme of this module. It seems clear that we must know something about them if we are to understand even the most basic information written on electrical appliances. (From 995 the UK electricity supply is 230 volts.)

3 Section 2 begins by showing a mathematical way of describing alternating currents, and investigating their behaviour in various electronic circuit components. This involves building mathematical models of physical situations, a process that some students find daunting. To avoid confusion everything has been made as explicit as possible, so you may find some of the steps spelled out in rather a lot of detail. Other topics covered in Section 2 include impedance (the a.c. equivalent of resistance), and the construction of simple filter circuits that can be used to block signals in certain frequency ranges. Phasor methods are introduced and used in this discussion to determine the impedances (and other properties) of a variety of simple circuits. Section 3 uses the results and concepts introduced in Section 2 to study the behaviour of charge, current and voltage in a variety of simple circuits. The circuits studied can exhibit various kinds of short-lived transient behaviour and, in some cases, sustained oscillations in which charges and currents flow back and forth repeatedly between different circuit components. In the most complicated cases this can even result in resonance when an alternating electrical supply excites an unusually large response from an appropriately designed circuit. This discussion of transients and oscillations also introduces the idea of a differential equation and some of the general principles that surround the use of such equations in particular physical contexts. However, no attempt is made to teach the mathematical techniques that are required to solve such equations in general. Although most people have some understanding of direct current, it is alternating current which in many ways has the greatest bearing upon our lives. That is one of the reasons why this module is important since it deals with an aspect of electricity which impinges directly upon our everyday lives.

4 Study comment Having read the introduction you may feel that you are already familiar with the material covered by this module and that you do not need to study it. If so, try the Fast track questions given in Subsection.2. If not, proceed directly to Ready to study? in Subsection.3.

5 .2 Fast track questions Study comment Can you answer the following Fast track questions?. If you answer the questions successfully you need only glance through the module before looking at the Module summary (Subsection 5.) and the Achievements listed in Subsection 5.2. If you are sure that you can meet each of these achievements, try the Exit test in Subsection 5.3. If you have difficulty with only one or two of the questions you should follow the guidance given in the answers and read the relevant parts of the module. However, if you have difficulty with more than two of the Exit questions you are strongly advised to study the whole module. Question F An inductor L of value 0.50H, a resistor R of value 0Ω and a capacitance C of value 5.07µF are connected in series (an LCR circuit) to an alternating supply of frequency 00Hz. What is the total impedance due to the three components? If the rms value of the supply voltage is 20V calculate the peak value of the resulting current. What is the phase relationship between the current and the voltage?

6 Question F2 Starting from an appropriate condition concerning the total voltage drop around a circuit, show that the current I(t) in a series LCR circuit that contains an external voltage supply V0 sin(ω t) must satisfy an equation of the form: d2i di I(t) L 2 +R + = V 0 Ω cos ( Ω t) dt dt C Describe the eventual behaviour of the general solution to this equation, after any transients have decayed.

7 Study comment Having seen the Fast track questions you may feel that it would be wiser to follow the normal route through the module and to proceed directly to Ready to study? in Subsection.3. Alternatively, you may still be sufficiently comfortable with the material covered by the module to proceed directly to the Closing items.

8 .3 Ready to study? Study comment In order to study this module you will need to be familiar with the following terms: amplitude, capacitance, charge, current, frequency, Kirchhoff s laws, parallel circuit, period, power, Ohm s law, oscillation, radians, resistance, series circuit, simple harmonic motion, vector (and vector addition ) and voltage. Mathematically, you should be familiar with the trigonometric functions sin (θ ) and cos(θ ) (including their graphs) and the use of the inverse trigonometric function arctan (x) to solve equations of the form tan(θ ) = x. You will also need to know Pythagoras s theorem and to be familiar with trigonometric identities, including the following results: π π sin 2 ( θ ) + cos 2 ( θ ) =,4 sin ( θ ) = cos θ,4 cos ( θ ) = sin θ +, 2 2 π and4 cos ( θ ) = sin θ 2 You do not need to be fully conversant with differentiation in order to study this module, but you should be familiar with the calculus notation dx/dt used to represent the rate of change of x with respect to t. If you are uncertain about any of these definitions then you can review them now by reference to the Glossary, which will also indicate where in FLAP they are developed. In addition, you will need to be familiar with SI units. The following Ready to study questions will allow you to establish whether you need to review some of the topics before embarking on this module.

9 Question R A 50Ω resistor is connected to a 20V d.c. supply. Calculate the current flowing in this resistor and hence the energy dissipated as heat in 5min. Question R2 A 00µF capacitor is connected to a 6V d.c. supply until it is fully charged. Calculate the maximum charge on the capacitor. If this capacitor is then discharged through a 0Ω resistor, calculate the maximum current which will flow.

10 Question R3 A resistor and a capacitor are connected in series to a d.c. supply. Draw a diagram representing this electrical circuit. The two components are now re-connected in parallel with the same d.c. supply. Draw a diagram representing this new circuit. Question R4 The displacement of a sinusoidal oscillation is described by the expression y = Asin(2πft), where A = 0cm and f = 2Hz. Calculate the displacement y when t = 0.25, 0.30 and 0.70s, respectively. What is the period of this oscillation?

11 2 AC circuits 2. Describing alternating currents and voltages You should already be familiar with the properties of a simple d.c. circuit of the kind shown in Figure. The box symbol represents a resistor, and the battery symbol represents a source of voltage (i.e. potential difference). The current I in the circuit will be such that the voltage drop V across the resistance R is equal to the voltage supplied by the battery. The voltage drop across the resistor can be measured using a voltmeter connected in parallel whilst the current flowing through the resistor can be measured using an ammeter connected in series. The resistance R can then be determined using Ohm s law V R= () I A I R V V Figure 4A simple d.c. circuit showing the measurement of potential difference and current using a voltmeter and ammeter, respectively. The arrow associated with the (conventional) current I indicates the direction in which positive charges would flow. The arrow associated with the voltage drop across the resistor points from low to high voltage and opposes the current direction. Negative values for I or V indicate currents and voltage drops that oppose the respective arrows.

12 In analysing a d.c. circuit such as that of Figure we generally think of the battery as a source of constant voltage, so that the current in any part of the circuit is a steady flow of electric charge in a single direction; that, after all, is the meaning of d.c. direct current. However, not all voltage sources are constant and neither are all currents direct. For example, the mains voltage supplied by standard wall sockets in the UK varies rapidly with time, the potential difference between the live and neutral terminals changing not just in magnitude but even in sign 50 times a second. Not surprisingly, the currents that such varying voltages produce in circuits will also vary with time, generally altering both their magnitude and direction in response to the variations in the voltage. A current that periodically reverses its direction in this way is called an alternating current (a.c.). A I R V V Figure 4A simple d.c. circuit showing the measurement of potential difference and current using a voltmeter and ammeter, respectively. The arrow associated with the (conventional) current I indicates the direction in which positive charges would flow. The arrow associated with the voltage drop across the resistor points from low to high voltage and opposes the current direction. Negative values for I or V indicate currents and voltage drops that oppose the respective arrows.

13 The simplest kind of alternating current is represented in Figure 2. The current changes smoothly and regularly with time in a manner that may be described by a sinusoidal function (i.e. a sine or a cosine function), just like a simple harmonic oscillator. Its peak value (or amplitude) is I 0, and the period over which it goes through one complete oscillatory cycle is T. In drawing Figure 2 we have chosen the time t = 0 to be a moment at which the current is zero, consequently, it is marginally easier to represent this particular current by means of a sine function rather than a cosine function so we can write 2πt I(t) = I0 sin T (2) I I0 0 T 2 T 3T 2 2T t I0 Figure 24Two cycles of an alternating current with peak value I0 and period T. Such a current may be represented by the function Note that we have chosen to represent the current by I(t) in order to emphasize that the value of I is changing with time and will generally depend on the value of t at which we choose to measure it. Equation 2 is very similar in form to the equation used to describe the displacement of a simple harmonic oscillator from its equilibrium position. The quantity 2πt/T, is called the phase of the oscillator, and increases by 2π each time t increases by an amount T.

14 Since an increase of phase by 2π corresponds to a complete oscillation, the phase has many of the characteristics of an angle measured in radians and some authors prefer to treat it as an angle, in which case it may be called the phase angle. It is possible to write the phase in Equation 2 2πt I(t) = I0 sin T (2) in a couple of other ways. The frequency f of an oscillation is related to the period by f = /T, so it is always possible to replace 2πt/T by 2πf t. More usefully we can introduce a related quantity called the angular frequency which is defined by ω = 2π/T so that the phase 2πt/T may be simply written as ωt.

15 In terms of frequency and angular frequency, the alternating current described by Equation 2 2πt (Eqn 2) I(t) = I0 sin T may therefore be written in the following equivalent ways. I(t) = I 0 sin(2πft) (3a) I(t) = I 0 sin(ωt) (3b) where f = /T and ω = 2π/T Frequency and angular frequency are defined in such a way that either quantity may be measured in units of s, thus the SI unit of each quantity is the hertz (Hz) since Hz = s.

16 So far, our mathematical descriptions of alternating currents have all been limited to the case where I = 0 when t = 0. Obviously this need not be the case; it is quite possible for an alternating current to have any one of its allowed values at t = 0. Figure 3 indicates the general situation that can arise. The current I is of the kind we have already discussed and is described by: I(t) = I0sin(ωt) (4a) but the current I2, which has the same angular frequency and amplitude as I, has some other value at t = 0. This more general current may be represented by the expression I2(t) = I0sin(ωt + φ) (4b) I I0 I0 sin φ I0 sin (ω t) 0 I0 T 2T t I0 sin (ω t + φ) Figure 34Sketch graph showing I = I0 sin(ωt) and I2 = I0 sin(ωt + φ), in which I2 leads I by a phase constant φ. where the constant φ is called the phase constant. The phase constant is the value of the phase at t = 0 and determines the current at that time since I2 (0) = I 0 sinφ.

17 Given any two quantities that oscillate with the same angular frequency, such as I and I2, it is always possible to relate the oscillations of one to those of the other by describing the way in which the phase of one is related to that of the other. In the case of I and I2 we can describe this phase relationship by saying that I2 leads I by φ or that I lags I 2 by φ. Note that φ could have many values, though it is customary to limit it to the range π < φ +π since adding or subtracting an integer multiple of 2π to the phase makes no difference to the value of the current.

18 I π (a) Use the trigonometric identity sin (θ ) = cos θ to write down 2 an expression that represents the current I shown in Figure 2 in terms of a cosine function. I0 π (b) Use the trigonometric identity cos (θ ) = sin θ + to determine 2 the phase relationship between cos(ωt) and sin(ωt). I0 0 T 2 T 3T 2 2T t Figure 24Two cycles of an alternating current with peak value I0 and period T. Such a current may be represented by the function

19 The phasor representation Another way of representing the alternating current of Figure 2 is in terms of a rotating phasor, as shown in Figure 4. A phasor is rather like the hand on a clock, though the phasors we will consider will all rotate in the anticlockwise direction. A phasor has a magnitude A and rotates at a fixed angular speed ω, so that the angle θ from the x-axis to the phasor increases with time. The y-component of the phasor (i.e. its projection y = Asinθ on to the y-axis) varies sinusoidally with θ, as indicated in Figure 4. y A y ω A sin θ θ x θ π 2π θ/rad Figure 44The projection of a phasor on to the y-axis is a sinusoidal function of the angle θ.

20 It follows that a graph showing the variation of thisy-component with time will be identical to Figure 2 provided the following requirements are met: The magnitude A of the phasor is equal to the amplitude (or peak value) I0 of the current. 2 At any time t, the angle θ of the phasor is equal to the phase (generally, ωt + φ) of the current. I I0 0 T 2 T 3T 2 2T t I0 Question T Draw a diagram showing the phasors that represent the alternating currents I and I2 (defined in Equations 4a and 4b) at time t = 0. In what way would your answer have changed if you had been asked to draw the phasors a quarter of a period later, at t = T/4?4 Figure 24Two cycles of an alternating current with peak value I0 and period T. Such a current may be represented by the function The fact that oscillating systems, such as alternating currents, can be represented by phasors is interesting but little more than that at present. However, later in the module you will see that the phasor representation becomes very useful when we have to work out the combined effect of several alternating currents that differ in phase and amplitude.

21 2.2 AC power and rms current When dealing with direct current, the power dissipated by a current passing through a resistor may be calculated using the formula P = I2 R (5) Resistors can become hot as a result of this power dissipation when current passes through them. When dealing with alternating current the situation is not so simple, since the current changes continuously. If the current at any instant is given by I = I0 sin(ω t), then the instantaneous a.c. power dissipation is given by P = I 2 R = I02 R sin 2 (ω t)

22 This instantaneous power is shown in Figure 5. Though it is useful to know the expression for the instantaneous power it is not really of much direct relevance when dealing with everyday a.c. devices such as light bulbs and electric heaters. The frequency of the mains supply (50Hz in the UK) is such that the instantaneous power rises and falls 00 times every second, which is much too fast for any heating effect to be seen or felt. When dealing with such everyday devices it is more useful to have an expression for the average a.c. power dissipated over a time that is much larger than the oscillation period of the current. P instantaneous power P = I02R sin2 (ω t) I02R 0 I02R T 2 3T 2T t 2 I 2R average value = 0 2 T Figure 54The instantaneous power Over one complete period of oscillation T, the average value of an dissipation P = I 02 R sin 2 ( ω t). alternating current I = I 0 sin(ω t) will be zero since every positive contribution to the average current will be counterbalanced by a negative contribution of equal magnitude. Nonetheless, an alternating current really does cause power dissipation in a resistor you only have to switch on an electric fire to be sure of that. The reason for this is apparent from Equation 5; P = I2 R (Eqn 5) the instantaneous power is proportional to I02, so the instantaneous power is positive whenever I is non-zero, irrespective of its sign.

23 Thus, the average power P dissipated over one full period T will be equal to the mean of I02 over that period. We may indicate this by using angular brackets to denote the mean and writing P = I02 R sin 2 (ω t) = I02 R sin 2 (ω t) Now the mean square current on the right-hand side can be worked out straightforwardly using the techniques of integration developed elsewhere in FLAP, but there is a simpler method that uses the special properties of the function sin2(ω t). Since the angular brackets indicate an average over a full period of oscillation, the time at which we start timing is unimportant, so we could equally well write π P = I02 R sin 2 ω t + = I02 R cos 2 (ω t) 2 If we add the right-hand sides of these last two equations we find: 2 P = I02 R sin 2 (ω t) + I02 R cos 2 (ω t) = I02 R sin 2 (ω t) + cos 2 (ω t)

24 However sin2 (ω t) + cos2(ω t) =, which is a constant, so its average value over a full period is the same as its instantaneous value, i.e.. Thus sin 2 (ω0t) + cos2 (ω0t) = 2 P = I02 R and P = I02 R (6) 2 This amounts to saying that sin 2 (ω0t) = /2, so the mean of I2 over a full period is I02 2. As you can see, when an alternating current of peak value I0 passes through a resistance R, the power dissipation is the same as that which would occur if a direct current of steady value I0 2 were to flow through the resistor. Because of the way it has been derived by taking the square root of the mean of I2 over a full period this effective average current is called the root-mean-square current or rms current. The root-mean-square current is usually denoted Irms so we can write: so, where 2 R P = I rms (7a) I rms = I0 (8a) 2 = I0

25 If we had started this investigation of the power dissipated by a resistor connected to an a.c. supply by considering an alternating voltage V = V 0sin(ω t) across the resistor rather than an alternating current through the resistor, we could have used the d.c. expression P = V02 /R to lead us to the a.c. results: P = where 2 V rms R V rms = V 0 (7b) 2 = V 0 (8b) In this case V rms is the root-mean-square voltage. Finally, note that by multiplying together the right-hand sides of Equations 7a 2 R P = I rms (Eqn 7a) and 7b, and then taking the square root, it can be seen that the average power dissipated by the resistor is also given by: P = VrmsIrms (7c)

26 Question T2 A 0Ω resistor is supplied using a 6V d.c. supply. Calculate the following quantities. (a) The current flowing through the resistor. (b) The energy dissipated every second in the resistor. (c) The rms current and rms voltage which would produce identical energy dissipation with the resistor connected to an alternating supply. (d) The corresponding peak values of alternating voltage and current.4

27 2.3 Alternating current in resistors, capacitors and inductors In the last subsection we examined the effect of an alternating current passing through a resistor. In this subsection we look at the origin of such a current. In particular we will answer the following question, If an alternating voltage is applied across a resistor, what current will it cause to flow through the resistor? As you will see, in the case of a resistor the relationship between the voltage and the current is quite straightforward, but we will also examine two other electronic components, a capacitor and an inductor, in which the relationship is not so simple.

28 I0 sin (ω t) Alternating current in resistors Figure 6a shows a simple a.c. circuit that supplies an alternating voltage V(t) = V0 sin(ω t) across a resistor. Since Ohm s law V = IR can be applied at any instant, we can expect that the varying voltage will produce a varying current given by I(t) = I V0 ~ V0 sin (ω t) ω I0 I0 V0 ωt R V (a) t time (b) Figure 64(a) A circuit supplying an alternating voltage (represented by the wavy line in a circle) across a resistor. The arrows shows the positive direction for the voltages, with an arrowhead at the positive end. (b) The current produced in the circuit is in phase with the voltage that causes it, as shown by the graph and the corresponding phasor diagram. V(t) V 0 = sin (ω t) R R

29 so, if we define V I0 = 0 R I0 sin (ω t) (9) I(t) = I 0 sin(ω t) I V0 then we can write (0) ~ V0 sin (ω t) ω I0 I0 V0 ωt R V t time A graph of this current, and the voltage that caused it, is shown in Figure 6b, along with the (a) (b) corresponding current and voltage phasors at an Figure 64(a) A circuit supplying an alternating voltage (represented by the wavy line in a arbitrary time t. The peak circle) across a resistor. The arrows shows the positive direction for the voltages, with an current I 0 has been arrowhead at the positive end. (b) The current produced in the circuit is in phase with the chosen for graphical voltage that causes it, as shown by the graph and the corresponding phasor diagram. convenience in Figure 6b; in practice it would be determined by the values of V 0 and R. The main point to notice about Figure 6b is that the current and the voltage rise and fall together, neither one leads or lags the other so there is no phase difference, and we can say that they are in phase. This is also clear from the phasors which rotate together, one on top of the other.

30 Alternating current in capacitors ω I I0 sin (ω t + π/2) I0 V0 sin (ω t) A capacitor acts to store charge, and may V0 generally be thought of ωt as a pair of parallel V C π 2π ~ t time ω ω conducting plates holding charges of equal magnitude but opposite sign. An alternating (a) (b) voltage V(t) = V0 sin(ω t) may be applied across a capacitor of fixed Figure 74(a) A circuit supplying an alternating voltage across a capacitor. (b) The current capacitance C by means produced in the circuit leads the voltage that causes it by π/2, as shown by the graph and the of a circuit like that corresponding phasor diagram. As in Figure 6, the inner circle in part (b) represents the peak shown in Figure 7a. voltage V0. No conduction current actually passes through the capacitor in such a circuit but there is an ebb and flow of charge from the capacitor as it is alternately charged and discharged; it is this flow that constitutes the current in the circuit.

31 Predicting this current is a slightly indirect process but the general approach is the same as before; we start with a result that can be expected to apply at any particular instant. In the case of a capacitor, the formula that we need is that which relates the charge q stored on the capacitor to the potential difference V across it: q = CV. Assuming this is true at every instant we can write q(t) = CV(t) = CV0 sin(ω t) ()

32 Note that our (arbitrary) choice of direction for the arrow indicating the positive sense of voltages across the capacitor in Figure 7a means that the stored charge q(t) must be interpreted as the charge on the upper plate of the capacitor. Whenever V ( t ) is negative (implying that the upper plate is at the lower potential), q(t) will also be negative. ω I0 sin (ω t + π/2) V0 sin (ω t) I0 I V0 ~ C (a) V ωt t π ω 2π ω time (b) Figure 74(a) A circuit supplying an alternating voltage across a capacitor. (b) The current produced in the circuit leads the voltage that causes it by π/2, as shown by the graph and the corresponding phasor diagram. As in Figure 6, the inner circle in part (b) represents the peak voltage V0. Now, the current at any point in a circuit is determined by the rate of flow of charge at that point in the circuit. In Figure 7a the positive direction assigned to the current is such that a positive current will cause q(t) to increase.

33 So, using the derivative notation of differential calculus, we find dq(t) dt and combining Equations I(t) = (2) q(t) = CV(t) = CV0 sin(ω t) (Eqn ) and 2 gives us I(t) = d[cv 0 sin(ω t)] dt This derivative can be easily evaluated by using the techniques of differentiation (or laboriously evaluated by drawing a graph of sin(ω t) and evaluating its gradient at many values of t). Using either method, the result will be I(t) = ωcv0 cos(ω t) so if we define I0 = ωcv0 (3) then we can write I(t) = I 0 cos(ω t) (4)

34 which can be rewritten in terms of a sine function as π I(t) = I0 sin ω t + 2 (5) ω I0 sin (ω t + π/2) V0 sin (ω t) I0 I V0 ~ C V ωt t π ω 2π ω time Having expressed the current in terms of a sine (b) function it is easy to see (a) that in a circuit containing just a Figure 74(a) A circuit supplying an alternating voltage across a capacitor. (b) The current capacitor the current and produced in the circuit leads the voltage that causes it by π/2, as shown by the graph and the the voltage are n o t in corresponding phasor diagram. As in Figure 6, the inner circle in part (b) represents the peak phase. The current leads voltage V. 0 the voltage by π/2. Figure 7b shows this relationship in graphical form, along with the associated phasors. As you can see the current phasor and the voltage phasor rotate at the same rate, but the current phasor is 90 ahead of the voltage phasor.

35 Alternating current in inductors An inductor is essentially a coil of wire. When a current is made to flow through an inductor a magnetic field is produced in the coil. When the current is changed, the changing magnetic flux in the coil causes an induced voltage in the coil (Faraday s law) and the polarity of this voltage acts to oppose any change in the current. ω I0 I0 sin (ω t π/2) I ωt L V (a) V0 sin (ω t) V0 ~ π ω 2π ω time (b) Figure 84(a) A circuit supplying an alternating voltage across an inductor. (b) The current produced in the circuit lags the voltage that causes it by π/2, as shown by the graph and the corresponding phasor diagram. Figure 8a shows a simple circuit that applies an alternating voltage V(t) = V 0sin(ω t) across an ideal inductor.

36 As the voltage changes the current will also tend to change. If the derivative di/dt represents the rate of change of the current I(t) passing through the inductor then the size of the voltage drop across the inductor at any instant will be di V(t) = L (6) dt where the constant L is called the inductance of the inductor. You should be able to see from Equation 6 that the inductance can be expressed in units of VsA ; such a unit is called a henry (H), so H = VsA. Widely used inductances vary from a few microhenry to hundreds of henry. Since V(t) = V0 sin(ω0t) Equation 6 gives di V 0 = sin (ω t) L dt (7)

37 Aside Because inductors act to oppose changes in the current they are often said to be a source of back voltage which counters any change in the voltage supplied. Since the total voltage around a closed circuit must be zero (Kirchhoff s law) it follows that supply voltage + back voltage = 0 If the supply voltage is given by V(t), it follows from Equation 6 that the back voltage is induced voltage = L di 4 dt

38 di V 0 = sin (ω t) L dt (Eqn 7) Equation 7 is an example of a differential equation since it involves the derivative di/dt of the quantity that interests us, the varying current I(t). The techniques needed to solve such equations are taught elsewhere in FLAP but you are not required to know them in order to study this module. Whenever such equations arise in this module we will simply quote their solutions and leave it to you to check by substitution that they are correct, should you wish to do so. The solution to Equation 7, subject to the condition that there is no source of steady current in the circuit, is V I(t) = 0 cos (ω t) ωl V so, if we define I0 = 0 (8) ωl then we can write I(t) = I0cos(ω t) which we can rewrite in terms of a sine function as π I(t) = I0 sin ω t 2 (9)

39 π I(t) = I0 sin ω t 2 Having expressed the current in terms of a sine function we can again determine its phase relationship to the applied voltage V(t). In this case the current lags the voltage by π/2. Figure 8b shows this relationship in graphical form, along with the associated phasors The current phasor is 90 behind the voltage phasor. (Eqn 9) ω I0 I0 sin (ω t π/2) I ωt L V (a) V0 sin (ω t) V0 ~ π ω 2π ω (b) Figure 84(a) A circuit supplying an alternating voltage across an inductor. (b) The current produced in the circuit lags the voltage that causes it by π/2, as shown by the graph and the corresponding phasor diagram. time

40 Summing-up As the above investigations show, when an alternating voltage V(t) is applied across a resistor, a capacitor or an inductor the resulting current has the same frequency as the applied voltage but is not necessarily in phase with it. In the case of the resistor the phases do coincide, but in the capacitor the current leads the voltage by π/2, and in the inductor the current lags the voltage by π/2. The peak value of the current, I 0, depends on the resistance, capacitance or inductance in each respective case, but in addition, it also depends on the frequency of the supply in the case of a capacitor or an inductor. We will say more about this relationship in the next subsection. In each of the cases considered above we defined a quantity I0 which was interpreted as the peak current: I0 = V0 /R, I0 = V0 ωc and I0 = V0 /(ω L). Confirm that the quantity on the right-hand side of each definition can be expressed in units of ampere (A).

41 2.4 Resistance, reactance and impedance The discussion of alternating currents in resistors in the last subsection shows no real surprises. In particular, if we measure the peak value V0 of the voltage across a resistor and the peak value I0 of the current that it causes to flow through the resistor (or the corresponding rms values), then we can easily determine the resistance R. It is given by V V R = 0 = rms I0 I rms This resistance does not depend on the frequency of the a.c. supply and does not give rise to any phase difference between the voltage and the current. In a similar way, we can use the quantity V0 /I0 to define a sort of effective a.c. resistance for capacitors and inductors. However, for these components the value of V0 /I0 does depend on the frequency of the supply and there will be a phase difference between the voltage and the current. Since the response of capacitors and inductors depends on the nature of the supply they are said to be reactive components, and V0 /I0 is called the reactance of a capacitor or an inductor, rather than its resistance. Nonetheless, the unit of reactance, like that of resistance, is still the ohm (Ω).

42 Using the symbols XC and XL to represent, respectively, the reactance of a capacitor and an inductor we see from Equations 3 and 8 I0 = ωcv0 V I0 = 0 ωl (Eqn 3) (Eqn 8) (together with the relation ω = 2πf0) that and V XC = 0 = I0 cap ω C (20) V XL = 0 = ω L I0 ind (2)

43 These results, along with the relevant phase relationships, are summarized in Table. R, X XC Table 4Resistance/reactance of various circuit components, together with the phase relationship they produce between voltage and current. Component Resistance/reactance Phase relationship resistor R = V 0 /I0 (constant) V and I in phase capacitor XC = /( ω C) I leads V by π/2 inductor XL = ω L I lags V by π/2 Graphs showing how resistance and reactance vary with angular frequency are shown in Figure 9. XL R ω Figure 94Graphs of R, XC and XL plotted as a function of angular frequency ω. Figure 9 indicates that the value of R is greater than the common reactance at which XL = XR. Must this always be the case, or does it depend on the particular resistors, capacitors and inductors we choose to consider?

44 We can summarize this in words by saying that the frequency does not affect the conduction through a resistor but the conduction through a capacitor increases with frequency while that through an inductor decreases with frequency. For direct current the reactance of a capacitor becomes infinite while that for an inductor falls to zero. At very high frequencies the inductor reactance rises without limit while that for the capacitor falls to zero. Inductors tend to block high frequency currents while capacitors block d.c. currents. Resistance and reactance are both I I special cases of a more general a.c. phenomenon known as impedance. network of If, as in Figure 0, an alternating resistors, voltage V(t) = V0 sin(ω t) impedence Z ~ V ~ V = capacitors and is supplied to some general inductors network of resistors, capacitors and inductors then the current I(t) that the network draws from the Figure 04When a network of resistors, capacitors and inductors (with two supply will have the general form external connections) is attached to a source of alternating voltage the effect is I(t) = I 0 sin(ω t + φ), where I0 represents the peak value equivalent to that of a load of impedance Z which causes the current to lead the of the current and φ determines the voltage by a fixed phase difference φ. phase relationship between the voltage and the current.

45 The values of I0 and φ in I(t) = I 0 sin(ω t + φ), will depend on the resistances and reactances of the various components of the network, but in general terms we say that the impedance Z of the network is Z= V 0 V rms = I0 I rms (22) If the network consisted of a single resistor, its impedance would simply be the resistance of that resistor and φ would be zero. Similarly, if the network consisted of a single capacitor or inductor then its impedance would equal the reactance of that capacitor or inductor and the value of φ would be +π/2 or π/2, respectively. In the next two subsections we will investigate the impedances and phase relationships that arise from more complicated networks.

46 It is important to note that the instantaneous power supplied to the network in Figure 0 is given by P(t) = V(t)I(t) = V0 sin(ω t)i0sin(ω t + φ) In the case of a resistor (or even a network of resistors), where the phase difference φ = 0, we have already seen that the average a.c. power over a full period I ~ V (T = 2π/ω) is I network of resistors, capacitors and inductors = ~ Z V impedence P = V0 I0/2 = V rms Irms. However, for a network containing capacitors and inductors φ will not generally be zero and it may be shown that Figure 04When a network of resistors, capacitors and inductors (with two external connections) is attached to a source of alternating voltage the effect is equivalent to that of a load of impedance Z which causes the current to lead the voltage by a fixed phase difference φ. P = Vrms Irmscosφ (23)

47 P = Vrms Irmscosφ (Eqn 23) It follows that both the instantaneous and average power dissipated when the network consists of a single capacitor or a single inductor is zero since φ = π/2 in these cases, and cos(π/2) = 0. Express P for a network in terms of the impedance Z and the peak current I 0, and hence show that 2 Z cos φ. P = I rms It is also true that for any network consisting only of pure inductors and capacitors, there is no power dissipation, since in each component the current and voltage are 90 out of phase. Power dissipation requires the presence of resistance in the circuit.

48 2.5 The series LCR circuit Combining C and R ~ I0 R I0 R + = V Figure shows a φ I capacitor and a resistor C R V0 connected in series. I0 XC I0 XC When circuit components are connected in this way VR VC the same current I(t) (a) (b) flows through each of them, but the total instantaneous voltage V(t) Figure 4A capacitor and resistor in a series a.c. circuit (an RC circuit). The voltage phasors at t = 0 are shown, as is their sum which represents the total voltage that must be across them is the sum of supplied at t = 0. the instantaneous voltages VR(t) and VC(t) across the individual components. (To this extent they behave like d.c. circuits.) Since the voltage across the resistor is in phase with the current while that across the capacitor is not, it follows that the voltage across the capacitor cannot be in phase with the voltage across the resistor. This means that the total voltage across the resistor and capacitor, which is just the applied voltage V(t), will not be in phase with the voltage across either component. Nor therefore can the applied voltage be in phase with the current in the circuit.

49 In what follows we are going to determine the relationship between the applied voltage and the current in this circuit, which will involve finding expressions for the ratio of their peaks Z = V0 /I0 and for the phase difference φ between them. ~ I0 R V + I0 R φ = I C R VC VR I0 XC (a) I0 XC V0 (b) Figure 4A capacitor and resistor in a series a.c. circuit (an RC circuit). The voltage phasors at t = 0 are shown, as is their sum which represents the total voltage that must be supplied at t = 0. The easiest way to find the relationship between the peak voltages (and this is the key to finding the impedance) is to use phasor diagrams of the kind introduced in Subsection 2.. Those needed in this case are also shown in Figure b. If the current is assumed to be of the form I(t) = I 0 sin(ω t), then at t = 0 it can be represented by a horizontal phasor. The voltage across the resistor VR(t) is in phase with this current so it too can be represented by a horizontal phasor at t = 0. This voltage phasor is shown in Figure b, it has amplitude I0R.

50 Now, remembering that ~ I0 R I0 R the voltage across a + = V φ capacitor lags the current I C through it by π /2 (since R V0 I0 XC I0 XC the current leads the voltage by π/2) we see VR VC that at t = 0, the voltage (a) (b) across the capacitor is represented by a phasor that points vertically Figure 4A capacitor and resistor in a series a.c. circuit (an RC circuit). The voltage downwards. This phasor phasors at t = 0 are shown, as is their sum which represents the total voltage that must be supplied at t = 0. is also shown in Figure b, and has amplitude I0 XC, where XC is the reactance of the capacitor. The phasor representing the total voltage across the resistor and capacitor at t = 0 is obtained by adding the other two phasors together as though they were vectors. Using Pythagoras s theorem, the amplitude V0 of this resultant phasor, which represents the total voltage across the circuit, is given by V 02 = I02 R 2 + I02 XC2 so i.e. V 02 = I02 ( R 2 + XC2 ) V 0 = I0 R 2 + XC2

51 ~ It follows that the impedance Z = V 0 /I 0 of the series combination of a resistor and a capacitor is given by Z= R 2 + XC2 (24) It can also be seen from Figure that the total voltage lags the voltage in the resistor by φ. I0 R V + I0 R φ = I C R VC VR I0 XC (a) I0 XC V0 (b) Figure 4A capacitor and resistor in a series a.c. circuit (an RC circuit). The voltage phasors at t = 0 are shown, as is their sum which represents the total voltage that must be supplied at t = 0. If we take the current phase as our reference zero then the voltage phase lag φ is given by X tan φ = C R X (25) so φ = arctan C R

52 Since the voltage in the resistor is in phase with the current in the circuit, and since we chose to represent the current by I(t) = I0sin(ω t), it follows that we can represent the total voltage by V(t) = V0 sin(ω t + φ). So, in a series RC circuit, the impedance is R 2 + XC2, and the current leads the applied voltage by X arctan C, since φ is a negative quantity in this case. R

53 Combining L and R ~ The same thing can be V0 I0 XL I0 XL done for a series V I0 R φ I combination of an + = I0 R R inductor and a resistor which is actually how a real inductor would VR VL behave. (a) (b) The relevant circuit is shown in Figure 2. Once again it will be Figure 24A resistor and an inductor in a series a.c. circuit (an LR circuit). The voltage assumed that the current phasors at t = 0 are shown, as is their sum which represents the total voltage that must be supplied at t = 0. is of the form I(t) = I 0 sin(ω t) and as before we will write the applied voltage as V(t) = V0 sin(ω t φ). The challenge is to find the ratio V0/I0 and the value of φ that are appropriate to this case. Of course, V 0 /I0 can always be written as Z, so the first problem is to find the impedance Z of the series combination. We will use the voltage phasors at t = 0 to help solve this problem.

54 The current in each series component is the same, and the voltage across the resistor is in phase with that current, so at t = 0 the phasor for the voltage across the resistor is horizontal and points to the right. The voltage across an inductor leads the current through it, so the phasor for the voltage across the inductor points vertically upwards in this case. The phasor representing the total voltage is the (phasor) sum of these two, as indicated in Figure 2. ~ V I0 R I R VR I0 XL I0 XL + = φ I0 R VL (a) (b) Figure 24A resistor and an inductor in a series a.c. circuit (an LR circuit). The voltage phasors at t = 0 are shown, as is their sum which represents the total voltage that must be supplied at t = 0. V0

55 Following a similar argument to that used earlier, the impedance of the LR combination will be Z= R 2 + X L2 (26) In this case the current (which is in phase with the resistor voltage) lags the total voltage. So V(t) = V0 sin(ω0t + φ) where in this case φ must be a positive quantity. X tan φ = L R X (27) or equivalently φ = arctan L R So, in a series LR circuit, the impedance is R 2 + X L2 and the current lags the applied voltage.

56 Combining L, C and R Figure 3 shows a resistor, a capacitor and an inductor combined in ~ I0 XL I0 R I0 R a series a.c. circuit. V = The current in each φ I C V0 R component is the same L I0 (XC XL ) I0 XC and so has the same phase. It is sensible to VR VC VL take this current as (a) (b) defining our phase zero, with the voltages across each component having Figure 34A series LCR a.c. circuit with the relevant phasor diagram showing how the phase angles with respect individual voltages are combined. (In this case XC > XL0). to the current phase. This time we must add together three voltage phasors at t = 0. Fortunately two of them point in opposite directions along the same line, so their resultant is easy to determine, and this can be combined with the third phasor in the usual way.

57 Thus V 02 = I02 R 2 + I02 ( X L XC )2 i.e. V 02 = I02 [R 2 + ( X L XC )2 ] but the impedance Z is given by Z = V 0 /I0, hence the impedance of a series LCR circuit is given by Z= R 2 + ( X L XC ) 2 (28) Substituting for the reactances (XL = ω0l and XC = /(ωc0)) gives us Z= R2 + ω L ωc 2 (29) It is also true that Z2 = R2 + X2 where X is the total reactance of the circuit. So, for a series circuit (impedance)2 = (resistance)2 + (reactance)2

58 The constant φ that determines the phase relationship between the current in the circuit and the supply voltage can also be deduced from the final phasor diagram in Figure 3. ~ I0 XL V L C VL VC R I0 R = I I0 (XC XL ) I0 XC φ I0 R V0 VR (a) (b) The value of φ is given Figure 34A series LCR a.c. circuit with the relevant phasor diagram showing how the by individual voltages are combined. (In this case X > X 0). C φ = arctan X L XC R L (30)

59 φ = arctan X L XC R (Eqn 30) So, in a series LCR circuit, if X C is greater ~ than XL then φ will be I0 XL I0 R I0 R V negative and the current = φ I in the circuit will lead the C V0 R L I0 (XC XL ) total voltage (as shown I0 XC in Figure 3). However, if XC is less than X L, VR VC VL Equation 30 will yield a (a) (b) positive value for φ, this corresponds to the case Figure 34A series LCR a.c. circuit with the relevant phasor diagram showing how the in which the current lags individual voltages are combined. (In this case XC > XL0). the total voltage.

60 In this convention we are taking the conventional voltage in the resistor to define the zero phase condition, so I(t) = I 0 sin(ω t) and the voltage applied to the whole circuit is then V(t) = V 0 sin(ω t + φ ), where V0 = Z0I0 and φ is given by Equation 30. X XC (Eqn 30) φ = arctan L R Question T3 A series LCR circuit has a supply current I(t) = I 0 sin(2πft) where = 0.A and the supply frequency f = 50Hz. If the components have values R = 00Ω, C = 50µF (i.e F) and L = 0.5H, calculate the impedance of the circuit and hence obtain an expression for the supply voltage.4

61 2.6 The parallel LCR circuit V V0 /XC ~ The basic principle that I I IR IC I0 underlies the analysis of a V0 X X C L parallel LCR circuit, of the V0 /R φ = kind shown in Figure 4 is I IL V0 /R R IL that the instantaneous V0 /XL voltage V(t) is the same IC across each element but the current will generally differ (b) from one component to (a) another. When dealing with a series circuit, a phasor Figure 44A parallel LCR circuit, the current phasors at t = 0, and the resultant phasor diagram was used to that represents the current drawn from the supply. combine the voltages across each component, but with a parallel circuit, phasors must be used to combine the currents through each component. The total current being supplied to the combination of resistor, capacitor and inductor will therefore be the phasor sum of the individual currents in each component. The current in the resistor I R(t) is in phase with the supply voltage V(t); the current in the capacitor IC (t) leads V(t) by π/2, and the current in the inductor IL(t) lags V(t) by π/2.

62 Hence, if the supply voltage is given by V(t) = V 0 sin(ω t) the currents in the resistor, I capacitor and inductor at t = 0 can be represented by the phasors shown in Figure 4. These phasors may be added together (like vectors) giving a resultant phasor that represents the current I(t) (a) drawn from the supply. V V0 /XC ~ IR I IC V0 /R IL IL IR V0 XC XL = I0 φ V0 /R V0 /XL IC (b) Figure 44A parallel LCR circuit, the current phasors at t = 0, and the resultant phasor that represents the current drawn from the supply. In Figure 4 the amplitudes of the current phasors have been denoted by the constants V0/XC, V0 /R and V0 /XL. This looks rather clumsy but makes more sense than denoting them IC, IR and IL. Explain why.

63 If we use Pythagoras s theorem to evaluate the amplitude of the resultant phasor in Figure 4, we find that the peak value of the total current in the circuit is given by V V0 /XC ~ I IR I IC V0 /R IL IL = I0 φ V0 /R V0 /XL 2 I0 = IR V0 XC XL V R XC X L V 02 IC (a) (b) (3) Figure 44A parallel LCR circuit, the current phasors at t = 0, and the resultant phasor that represents the current drawn from the supply. so, 2 I0 = + 2 V0 R XC X L

64 but the impedance Z = V0 /I0. Hence; the impedance of a parallel LCR circuit is given by 2 = + 2 Z R XC X L (32) Substituting for the reactances (XC = /(ωc) and XL = ωl) we can rewrite this in the equivalent form 2 = ωc + 2 ω L Z R (33)

65 The constant φ that determines the phase relationship between the total current and the current through the resistor (and hence the voltage) may also be expressed in terms of the amplitudes of the three current phasors: V V φ = arctan 0 0 X C XL V0 R Dividing both the numerator (the top) and the denominator (the bottom) of this expression by V0 gives us φ = arctan X C X L R (34) So, in a parallel LCR circuit, if /XC is greater than /XL, then φ will be positive and the current will lead the voltage, but if /XC is less than /XL, φ will be negative and the current will lag the voltage. In other words, if the voltage in the circuit is V(t) = V 0 sin(ω t), the current will be given by I(t) = I 0 sin(ω t + φ), where I0 = V0 /Z and φ is given by Equation 34.

66 Question T4 A parallel LCR circuit has a supply voltage of the form V = V 0 sin(2πft), where V0 = 00V and the supply frequency f = 50Hz. If the components have values R = 00Ω, C = 50µF and L = 0.5H, calculate the impedance of the circuit and hence write an expression for the supply current.4

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