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Contents Introduction 2 Resistance in ac circuits 3 Inductance in ac circuits 7 Inductors in parallel 11 Inductors in series 13 Inductors in power circuits and systems 15 Ballasts in fluorescent light fittings 15 Fault current limiters 15 Capacitive VAR reduction 15 Inductors in electronic circuits 16 Capacitance in ac circuits 24 Capacitive reactance 26 Factors affecting capacitive reactance 27 Comparing capacitors in ac and dc circuits 31 Capacitors in series and in parallel 32 Capacitors in power circuits and systems 34 Power factor correction 34 Motors 35 Electronics 35 Summary 36 Answers 44 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 1 Introduction In this section you will learn how voltage is related to current in ac circuits, for the resistor, the capacitor and the inductor. The total opposition to current is affected by all of the circuit components and is called the impedance (Z). You will see that the current through a resistor is in phase with the voltage, but that the capacitor and inductor cause phase shifts between the applied voltage and the resulting current. Resistors continue to obey Ohm’s Law in an ac circuit, where voltages and currents are expressed as rms values. Capacitors and inductors are a little more complex, but we can still use equations very similar to Ohm’s Law for these components. There is a quantity called the reactance of capacitors and inductors that can be used instead of the resistance in Ohm’s Law. At the end of this section you should be able to: 2 Determine the voltage, current and resistance from measured or given values of any two of these quantities. Show the relationship between voltage drops and current in a resistive ac circuit. List applications of resistive ac circuits. Define 'inductive reactance' and ‘capacitive reactance’ Calculate the inductive reactance of a given inductor and show the relationship between inductive reactance and frequency. Determine voltage, current or inductive reactance in a purely inductive a.c. circuit given any two of these quantities. List applications of inductive ac circuits Calculate the capacitive reactance of a given capacitor and show the relationship between capacitive reactance and frequency. Determine voltage, current or capacitive reactance in a purely capacitive ac circuit given any two of these quantities. List applications of capacitive a.c. circuits. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Resistance in ac circuits You will remember that the two effects that are always present when an electric current flows are the heating effect and the magnetic effect. The heating effect is due to current flow and resistance. We can then say that any type of load that produces heat in the circuit is a resistive load. Some typical loads of this type are water heaters, electric ranges, toasters, radiators and incandescent lights. Remember that power P = VI in dc circuits and this also applies to purely resistive ac circuits. All materials exhibit some resistance, and we may have to consider the resistance of the circuit wiring. Sometimes we may neglect the resistance as other circuit properties may be so large as to make the resistance insignificant. In a purely resistive circuit, the impedance is equal to the circuit resistance. As Z = R, the circuit current may be calculated: I V R Example The hot resistance of a 60 W incandescent lamp is 960 Ω. Determine the current if the lamp is rated at 240 V. Solution Given R = 960 Ω and V = 240 V, find I. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 3 V Z but Z R so V I R 240 960 0.25 A I Example A water heater is rated at 3.6 kW on a 240 V 50 Hz supply. Determine the current drawn from the supply and the resistance of the element. Solution Given V = 240 V and P = 3.6 kW, find I and R. To determine the current we need to recall that the power P = VI in purely resistive ac circuits. (a) P V 3600 240 15 A I (b) V I 240 15 16 R In a purely resistive ac circuit the voltage and current will be in phase with each other. This condition is shown in Figure 1 in both the wave diagram and the phasor diagram. 4 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 = 0 = 0 Figure 1: Voltage and current in phase in resistive AC circuit The wave diagram shows instantaneous values from zero to maximum, whereas the phasor diagram is usually drawn to represent rms values. The rms values, as you know, are the values indicated by voltmeters and ammeters. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 5 Check your progress 1 Part A In questions 1–2, place the letter matching your answer in the brackets provided. 1 In a purely resistive circuit, the current and voltage: (a) are in phase (b) have a phase difference of 90° (c) are directly opposite with respect to phase angle (d) change with respect to phase angle when resistance increases 2 ( ) ( ) Impedance of a series ac circuit is: (a) resistance plus reactance (b) resistance squared plus reactance squared (c) square root of resistance squared plus reactance squared (d) root mean squared of resistance squared and reactance squared. Part B 1 Draw the phasor diagram for a single resistor connected to a 100 V supply and drawing 50 A. Use a scale of 1 mm per volt and 1 mm per ampere. Answers to Check your progress are at the end of the section. 6 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Inductance in ac circuits The nature of an alternating current is that of a continual change in magnitude and direction. The magnetic effect of the current then produces a magnetic field that is also changing in the same manner as the current that gave rise to it. The field flux produced by an alternating current induces an emf in the conductor that opposes the applied emf. This emf of self-induction is equal to and directly opposite to the applied emf. In Figure 2 the two waveforms are shown changing. Figure 2: Voltages in an inductive ac circuit It is this induced emf opposing the circuit current that produces inductive reactance. Inductive reactance is the circuit property that opposes circuit current. The symbol for inductive reactance is XL and the unit is the ohm because XL allows us to continue to use relations similar to Ohms-law in ac circuits In an inductive ac circuit there is a phase shift between the applied emf and the circuit current. The phase shift is such as to cause the circuit current to lag the applied emf by 90°. The wave diagram and phasor diagram for this condition are shown in Figure 3. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 7 Figure 3: V and I relationship for a ‘pure’ inductive circuit To explain the phase shift consider the induced emf V’. This emf is due to the changing current in the inductor. Recall that in a coil, v N t where: v instantaneous induced emf rate of change of flux t N number of turns Note: the negative sign indicates opposition (Lenz's law) The rate of change of flux is directly due to the rate of change of the current ie, the magnitude of the emf is dependent on the rate of change of the current. v L i t where: v instantaneous induced emf i rate of change of current t L inductance At 0° the value of V is zero thus the rate of change of the current must be zero so the current is at a maximum value. Between 0° and 90° the induced emf is equal to and opposite to the applied emf. For this to occur the change in current must be from a maximum value negative toward zero as the induced emf opposes the current that causes it. 8 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 The induced emf rises from zero to maximum negative as the current falls from maximum negative to zero. At 90° the induced emf is maximum and negative requiring current to be at its maximum rate of change going positive (that is, passing through zero). The current then follows a sine wave pattern and when plotted on the wave diagram is seen to be lagging the applied emf by 90°. To calculate circuit current in an inductive circuit the total impedance is inductive reactance. Substituting XL for Z we use: I V XL Example What current will flow in a 240 volt, 50 hertz circuit which has an inductive reactance of 60 ohm? Solution Given: V = 240 V, 50 Hz XL = 60 Find I I V XL 240 60 4A Inductive reactance depends on the inductance and the frequency of the supply voltage. The equation to calculate this value is: X L 2 fL where: X L inductive reactance in ohm f supply frequency in hertz L inductance in henry Inductive reactance is directly proportional to both the supply frequency and the inductance. Circuit current will be affected by a change in either. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 9 When there is an increase in frequency, XL will increase, causing the circuit current to decrease. When there is a decrease in frequency, XL will decrease, causing the circuit current to increase. Where there is an increase in inductance, XL will increase, causing the circuit current to decrease. When there is a decrease in inductance, XL will decrease, causing the circuit current to increase. Example 1 Calculate the inductive reactance of a coil which, when connected to a 240 V, 50 Hz supply draws a current of 0.5 A . 2 What will the value of inductive reactance be if the coil is reconnected to a 100 V 60 Hz supply? Solution Given: I = 0.5A V = 250 V 50 Hz Find XL. First we must calculate inductive reactance of the contactor coil. V I 240 0.5 480 XL Now we can determine the value of inductance: XL = 480 f = 50 Hz Find L X L 2 fL L XL 2 f 480 314 1.53 henry 10 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Check your progress 2 1 What is the current phase relationship to the applied voltage in a purely inductive circuit? _____________________________________________________________________ _____________________________________________________________________ _____________________________________________________________________ 2 Calculate the inductive reactance of a 0.5 henry inductor on a 50 Hz supply. _____________________________________________________________________ _____________________________________________________________________ _____________________________________________________________________ Check your answers with those given at the end of the section. Inductors in parallel If inductors are connected in parallel as shown in Figure 4 the total inductance or equivalent inductance is given as: LT 1 1 1 1 ....... L1 L2 L3 which is similar to calculating equivalent resistance of parallel resistors. From which the equivalent reactance may be calculated as follows: X L 2 fLT EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 11 Figure 4: Inductors in parallel Alternatively the reactance of each inductor can be calculated using the general equation: X L 2 fL and since in a purely inductive circuit the impedance consists of reactance only we may determine the equivalent impedance as follows: ZT 1 1 1 1 ........ Z1 Z 2 Z 3 Note: this can only be used for pure inductors. To find the total current IT use the following relationship: IT V ZT Example For the circuit in Figure 5 calculate: (a) LT (b) ZT (c) IT Figure 5 12 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Solution 1 1 1 1 2 3 4 0.92 H LT (a) (b) (c) ZT XL 2 50 0.92 289 240 289 0.83 IT Inductors in series If inductors are connected in series as shown in Figure 6 the total inductance or equivalent inductance is given as: LT L1 L2 L3 ... similar to calculating equivalent resistance of series resistors. From which the equivalent reactance may be calculated as follows: X L 2 fLT Figure 6: Inductors in series Alternatively the impedance of each inductor can be calculated using the general equation: X L 2 fL and again we can calculate the equivalent impedance given that impedance is due only to the reactance follows: ZT Z1 Z 2 Z3 ... To find the total current IT use the following relationship: EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 13 IT V ZT Example For the circuit in Figure 7 calculate: (a) LT (b) ZT (c) IT Figure 7 Solution (a) (b) (c) 14 LT 2 3 4 9H X L 2 50 9 2827 240 IT 2827 0.085 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Inductors in power circuits and systems Inductors are widely used in electrical and electronic circuits. They can be used to: store energy oppose change in current flow limit AC current with little loss of power. Some particular applications are given below. Ballasts in fluorescent light fittings Fluorescent lamps, because they work on a principle of electrical current flow through a gas do not have any built-in current limiting feature such as incandescent lamps do. A resistor could be used for this purpose but it would prove to be very inefficient due to heat generated in the resistor. A better method is to use an inductor (ballast or choke) to limit the current, and this is done with very little loss. Fault current limiters In high voltage systems inductors are often used in series with high voltage lines to limit current flow in the event of a fault. Capacitive VAR reduction When high voltage systems are lightly loaded, the line-to-line and line-toground capacitance can cause voltages in excess of nominal system voltage to be induced. Inductors are usually automatically brought into line to cancel this effect. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 15 Inductors in electronic circuits In electronics, inductors are used for: Tuning circuits—radio and television recievers employ a circuit containing a capacitor and an inductor that allows signals of one frequency only to pass through. By making the capacitor adjustable via a knob, the user can select what frequency the radio receives. Filter circuits—work in a similar way to the tuning circuits. By careful choice of inductors and/or capacitors, a circuit can be made to block or accept a range of frequencies. Used often to filter out unwanted noise from electronic circuits, especially the 50 Hz mains induced noise. Check your progress 3 For the circuit in Figure 8 calculate: (a) LT ______________________________________________________________________ ______________________________________________________________________ (b) XL ______________________________________________________________________ ______________________________________________________________________ (c) IT ______________________________________________________________________ ______________________________________________________________________ Figure 8 Check your answers with those given at the end of the section. 16 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Check your progress 4 Part A In questions 1-12, place the letter matching your answer in the brackets provided. 1 In a purely resistive ac circuit, the current: (a) lags the emf by 90° (b) leads the emf by 90° (c) is in phase with the emf (d) has a phase angle of between 0° and 90° 2 ( ) ( ) The inductive reactance of a coil is directly proportional to the: (a) circuit current (b) applied voltage (c) supply frequency (d) circuit impedance 3 The angle of phase difference between the applied voltage and the current in a purely inductive circuit is: (a) 0° (b) 45° (c) 90° (d) 180° 4 ( ) ( ) ( ) Inductive reactance is measured in ohm because it: (a) absorbs power (b) it is the true resistance of an ac circuit (c) is the equivalent resistance of an ac circuit (d) is the ratio of the emf of self induction to the current, in an ac circuit 5 The opposition to current flow in a purely inductive ac circuit is termed: (a) inductance (b) resistance (c) inductive reactance (d) impedance reactance EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 17 6 The inductance of a coil will: (a) increase with frequency (b) reduce with frequency (c) reduce with applied voltage (d) will not change with any of the above as it is a physical quantity 7 ( ) ( ) ( ) ( ) ( ) ( ) The emf of self induction is: (a) equal to and in phase with the applied emf (b) exactly opposite but less than the applied emf (c) equal to and in phase opposition to the applied emf (d) less than but directly in phase with the applied emf 8 Inductance may be defined as the circuit property which: (a) absorbs power (b) opposes any change in current (c) increases with increase in frequency (d) decreases with increase in frequency 9 As current decreases in an inductive circuit there is: (a) an increase in magnetic flux (b) a decrease in self induced emf (c) an increase in self induced emf (d) a decrease in capacitive reactance 10 A ballast is used in a fluorescent lamp fitting to: (a) improve the power factor (b) improve the light colour (c) limit the current drawn by the lamp (d) fix the fitting to a vertical surface 11 Adding an inductor in series with an existing inductor will: (a) increase the impedance and decrease the inductance of the circuit (b) increase the impedance and increase the inductance of the circuit (c) decrease the impedance and decrease the inductance of the circuit (d) decrease the impedance and increase the inductance of the circuit 18 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 12 Adding an inductor in parallel with an existing inductor will: (a) increase the impedance and decrease the inductance of the circuit (b) increase the impedance and increase the inductance of the circuit (c) decrease the impedance and decrease the inductance of the circuit (d) decrease the impedance and increase the inductance of the circuit ( ) Part B 1 A coil of negligible resistance draws a current of 4 ampere when connected to a 240 volt, 50 hertz supply. Determine the: (a) reactance of the coil ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (b) inductance of the coil ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 2 A coil of negligible resistance draws a current of 10 ampere when connected to a 240 volt, 50 hertz supply. Determine the current the same coil would draw if connected to a 120 volt, 100 hertz supply. ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 19 3 Calculate the reactance of a 3 henry coil when the supply is 240 volt, 50 hertz. ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 4 Calculate the inductance of an inductor that will limit an ac circuit to a current of 5 ampere in a 115 volt, 60 hertz supply. ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 5 For the circuit in Figure 9, determine the inductance of an ideal coil which would have a current of 10 A through it. Figure 9 ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 20 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 6 For the circuit in Figure 10 calculate: Figure 10 (a) LT (equivalent inductance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (b) ZT (equivalent impedance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (c) IT (total current) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 7 For the circuit in Figure 11 calculate: Figure 11 (a) LT (equivalent inductance) ____________________________________________________________________ EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 21 ____________________________________________________________________ ____________________________________________________________________ (b) ZT (equivalent impedance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (c) IT (total current) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 8 For the circuit in Figure 12 calculate: Figure 12 (a) LT (equivalent inductance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (b) ZT (equivalent impedance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ 22 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 (c) IT (total current) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ Answers to check your progress are at the end of the section. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 23 Capacitance in ac circuits A capacitor has the ability to store an electric charge in the form of stress in the dielectric materials when there is an imbalance of electrons on the capacitor plates. Figure 13 shows the current in a purely capacitive circuit to which a sinusoidal voltage is applied. Figure 13: Voltage and current in a capacitive ac circuit You will see that I leads V by 90° when the ac circuit contains capacitance only. This is because the current will flow from the supply to the capacitor until the capacitor voltage equals the supply voltage and then stops. The value of the circuit current is dependent on the difference in the voltage of the source from the voltage across the capacitor - the greater the difference, the greater the rate of current flow. Current only flows in the conductors external to the capacitor while electrons are moving from one plate of the capacitor to the other. In Figure 13 (b) the voltage is from an ac source and is continually changing in magnitude and direction. The rate of charge flow is related to current and time. I 24 Q ampere t EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 The circuit current will be at a maximum when the applied voltage is changing at its maximum rate, and zero when the voltage is not changing. At which part of the cycle do these two changes occur? We will reconsider a single cycle of the voltage sine wave of an ac source in Figure 14. Figure 14: Single wave of ac voltage The maximum rate of change in voltage occurs as the wave is passing through zero volts. This is because the greater rise in value of voltage level is happening in a lesser time than it does as the wave reaches a maximum. The rate of change at various points can be easily determined as shown in the following example. Each period of time was over a 5° section of the wave cycle. The greater rate is found to be at the points 1 and 3 in Figure 14. At points 2 and 4 the rate of change is zero. The rate of change is maximum at the instant the voltage changes direction at points 1 and 3. We can now plot the information for current flow in a capacitive circuit as shown in Figure 15 and you will see that the relationship is that of Figure 13. Figure 15: Current voltage relationship in a purely capacitive circuit At point 1 the rate of change in voltage is maximum going positive; thus current is maximum positive. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 25 At points 2 and 4 the rate of change of voltage is zero and current is therefore zero. At point 3 the rate of change of voltage is maximum going negative so current is maximum negative. The current wave will also be sinusoidal and, plotted to the given points, will be seen to be leading the voltage by 90°. In a purely capacitive circuit the current leads the voltage by 90 degrees. Capacitive reactance The property of a capacitor that limits current in ac circuits is known as capacitive reactance. The symbol is XC and the unit is the ohm. If the only component in an ac circuit is a capacitor, then the total impedance of the circuit is equal to the capacitive reactance. To calculate circuit current in a capacitive circuit we can use the following relationship: I V ampere XC where V and I are rms values of voltage and current respectively. Example A capacitor having a capacitive reactance of 80 ohm is connected to a 240 V 50 Hz supply. Determine the circuit current. Solution Given: V = 240 volt, 50 Hz XC = 80 Find I 26 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 I V XC 240 80 3A Example Determine the capacitive reactance required to limit current to 0.25 A on a 240 V, 50 Hz supply. Solution Given V = 240 volt 50 Hz I = 0.25 A Find XC. V I 240 0.25 960 XC As with resistance only, capacitive reactance is used with the basic Ohm’s law equation to solve circuit problems. Values of circuit voltage and current are rms values. Factors affecting capacitive reactance The factors that affect the value of the reactance of a capacitor are the frequency of the supply and the capacitance of the capacitor. To calculate the capacitive reactance given capacitance and supply frequency we use: XC 1 2 fC where: X C = capacitive reactance in ohm f = supply frequency in hertz C = capacitance in farad EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 27 Capacitive reactance is inversely proportional to both frequency and capacitance. That is, if either one is increased capacitive reactance decreases. Example Consider a capacitive circuit on an ac supply which has a 5 A current. What will be the circuit current if the frequency is doubled? Solution As the reactance is inversely proportional to the frequency, that is: X C1 1 f the new reactance will be half, as frequency is multiplied by two. New reactance: 1 X C 2 X C1 2 The new circuit current then must be doubled and becomes 10 amps. Similarly, reactance is inversely proportional to capacitance and the changes to reactance and circuit current for a change in capacitance follow those for changes in frequency. increase f → decrease XC → increase I decrease f → increase XC → decrease I increase C → decrease XC → increase I decrease C → increase XC → decrease I Examples Calculate the capacitive reactance of a 60 microfarad capacitor on a 240 V, 50 Hz supply. Solution Given C = 60 F (60 × 10-6 farad) F = 50 Hz 28 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Find XC XC 1 2 fC 1 _ 2 3.141 50 60 10 6 53 An alternative is to have 106 or 1 000 000 on the top line and the capacitance in micro-farad on the bottom line. 106 ohm 2 fC 1 000 000 314 60 53 XC How much current will flow in a 240 V, 50 Hz circuit if the circuit has an 8 F capacitor as its only load? Solution Given V = 240 volt 50 Hz C = 8 F Find I V Z Z XC I I XC V XC 106 2 fC 1 000 000 314 8 398 240 398 0.603 A I EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 29 Check your progress 5 1 What is the capacitive reactance of a 100 f capacitor on a 50 Hz supply? ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 2 Calculate the current if a 16 F capacitor is connected to a 240 V, 50 Hz supply. ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ Check your answers with those given at the end of the section. 30 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Comparing capacitors in ac and dc circuits When a capacitor is connected to a source of dc there will be a movement of electrons to the uncharged plates. As the plates become charged the electron movement will cease. When fully charged, the capacitor voltage is the same as the supply, and there is no potential difference between the supply and the capacitor. A charged capacitor will therefore block dc. On an ac source, a capacitor is continually charging and discharging. No electrons pass through the capacitor even though there is an ac current through the circuit. Figure 16: A capacitor passing ac current There will be a continual flow of AC in the lamp filament causing a continual glow. Therefore a capacitor will allow a flow of ac in the external circuit, even though no electrons actually cross the dielectric! EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 31 Capacitors in series and in parallel From the expression CK A farad L it can be seen that if capacitors are connected in parallel the total capacitance will increase as this is similar to increasing the plate area, Figure 17 (a). Total capacitance in parallel is the sum of the individual capacitances. Figure 17: Capacitor connections In series, capacitors will appear to have the distance between plates increased as seen in Figure 5(b) which will decrease the total capacitance. Total capacitance for a series connection is calculated as follows: CT 1 farad 1 1 1 C1 C2 C3 You will recognise the basic expressions and note that the change is opposite to finding total resistance for series and parallel resistors. 32 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Check your progress 6 For the circuit in Figure 6 calculate: (a) CT (equivalent capacitance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (b) ZT (equivalent impedance) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ (c) IT (total current) ____________________________________________________________________ ____________________________________________________________________ ____________________________________________________________________ Figure 18 Check your answers with those given at the end of the section. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 33 Capacitors in power circuits and systems Capacitors are widely used in electrical and electronic circuits. The features of capacitors are their ability to: store energy oppose change in voltage pass ac while blocking dc current. Some particular applications follow. Power factor correction Some installations have loads with a large inductive component. Because the current through these loads is not in phase with the voltage, these installations draw more current that is necessary. This condition causes what is known as a low power factor. Power utilities place limits on the power factor presented by each premises, which should ideally be unity (ie 1). Power factor correction using capacitors is done at all stages of a power distribution system. At the transmission stage, large high voltage capacitors are placed in circuit when the system power factor drops below a predetermined level. This is often done automatically. At the distribution and at high voltage customer premises, power factor capacitors are connected to 11 kV supply lines and switched in banks to compensate for low power factor. At the 415/240 V level individual items of equipment sometimes incorporate power factor correction capacitors. An example is fluorescent light fittings which can be ordered as either HPF (high power factor) or LPF (low power factor). The HPF fittings have a capacitor fitted. 34 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Motors Capacitors are used in single phase motors to enable the motor to start unaided. This is done by using the capacitor to alter the phase angle between two windings in the motor thereby producing a rotating magnetic field. Electronics Capacitors find use in ac circuits associated with the electronics industry. Some examples are: Power supplies—capacitors are used to smooth out (or filter) the output of dc power supplies to remove ripple and make the waveform as ‘flat’ as possible. Oscillator circuits—used to produce an alternating output signal. Blocking of dc—capacitors are used in circuits designed to allow ac to pass but block dc. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 35 Summary Pythagoras’s theorem may be expressed as: Z2 = R2 + X2 where Z = impedance R = resistance X = reactance and derived from this: Z R2 X 2 Ohms law still holds for an ac circuit, with V and I as rms values. Inductance is a physical circuit property. Inductance is that circuit property that opposes a change in current. When the magnetic flux surrounding an inductor changes in strength, an emf is induced in the conductors in such a direction as to oppose the change in current. An increase in current will induce the emf in a direction to try to stop the current increasing. A decrease in current induces the emf in a direction that will tend to keep the current up. The property of inductive reactance is that property that opposes circuit current. The symbol for inductive reactance is XL and is expressed in ohms. Inductive reactance may be calculated given the inductance of the coil and the supply frequency using the expression: XL = 2fL ohm 36 In a purely inductive circuit the current lags the applied voltage by 90°. For an increase in frequency or inductance or both these, XL will increase and circuit current will decrease. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 For a decrease in frequency, inductance or both of these, XL will decrease and circuit current will increase. Ohm’s law when applied to ac circuits uses values of impedance (Z), rms values of voltage (V) and rms values of current (I). Resistive loads generally are loads that produce heat. In purely resistive ac circuits the voltage and current are in phase with each other. In purely capacitive ac circuit the current leads the voltage by 90 degrees. Capacitive reactance is that property that limits circuit current in a capacitive circuit. The symbol is XC and the unit is the ohm. The equation to calculate XC, given C and f, is: XC 1 ohm 2fC where f is in hertz C is in farad XC is inversely-proportional to both f and C. increase f → decrease XC → increase I decrease f → increase XC → decrease I increase C → decrease XC → increase I decrease C → increase XC → decrease I A capacitor allows AC to flow and will block dc. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 37 Check your progress 7 Part A In questions 1–13, place the letter matching your answer in the brackets provided. 1 When there is an imbalance of electrons on the opposite plates of a capacitor, there is: (a) no charge on the capacitor (b) no voltage across the capacitor (c) a constant current flowing through the capacitor (d) a stress in the electron orbits of the dielectric 2 ( ) The ability of a capacitor to store a charge which will oppose a change in voltage in an ac circuit is called its: (a) reactance (b) resistance (c) capacitance (d) permissiveness 3 ( ) The relationship between voltage and current in a purely capacitive circuit, supplied by ac, is that current: (a) and voltage are in phase (b) lags voltage by 90° (c) leads voltage by 90° (d) and voltage are in phase opposition 4 ( ) ( ) The resultant of two or more voltages differing in phase may be determined by: (a) phasor addition (b) adding numerically (c) algebraic addition (d) averaging the values 38 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 5 An equation to determine capacitive reactance is: (a) X C V Z (b) X C R Z (c) X C 2 fC (d) X C 6 1 2 fC ( ) ( ) ( ) ( ) As applied frequency on a capacitor increases, the capacitive reactance: (a) reduces (b) increases (c) does not change (d) acts to change applied frequency 7 8 In a purely capacitive circuit with ac supply, the current is: (a) I V R (b) I V C (c) I V XC (d) I V 2 fC The angle of phase difference between voltage and current in a purely capacitive circuit is: (a) 0° (b) 45° (c) 90° (d) 180° EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 39 9 The equation to determine the total capacitance of three capacitors in parallel is: (a) CT (b) 1 C1 C2 C3 1 1 1 1 CT C1 C2 C3 (c) CT C1 C2 C2 C3 (d) CT C1 C2 C3 ( ) ( ) ( ) ( ) ( ) 10 For a purely capacitive circuit, impedance (Z) equals: (a) supply voltage (b) total capacitance (c) frequency of the supply (d) total capacitive reactance 11 A capacitor is used in a fluorescent lamp fitting to: (a) improve the power factor (b) improve the light colour (c) limit the current drawn by the lamp (d) fix the fitting to a vertical surface 12 Adding a capacitor in series with another capacitor will: (a) increase the impedance and decrease the capacitance of the circuit (b) increase the impedance and increase the capacitance of the circuit (c) decrease the impedance and decrease the capacitance of the circuit (d) decrease the impedance and increase the capacitance of the circuit 13 Adding a capacitor in parallel with another capacitor will: (a) increase the impedance and decrease the capacitance of the circuit (b) increase the impedance and increase the capacitance of the circuit (c) decrease the impedance and decrease the capacitance of the circuit (d) decrease the impedance and increase the capacitance of the circuit. 40 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Part B 1 Draw a neat wave and phasor diagram of the voltage and current for a capacitor on an ac supply. (No scale is required.) 2 Calculate the voltage required to cause a 5 A current in a circuit having a capacitive reactance of 40 Ω. ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 3 The current in a 240 V, 50 hertz capacitive circuit is 6 A. What current will flow if the frequency is increased to 60 Hz ? ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 4 Calculate the capacitive reactance of a 100 µF capacitor when it is connected to a 415 V, 50 Hz supply. ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 41 5 When connected to a 240 volt, 50 hertz supply a capacitor draws a current of 10 A. What current would be drawn if the size of the capacitor was doubled? ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 6 Two capacitors, each with a capacitance of 40 F are connected in series to a 240 volt, 50 hertz supply. ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 7 For the circuit in Figure 19 calculate: (a) CT (equivalent capacitance) ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ (a) ZT (equivalent impedance) ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ (a) IT (total current) ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________ 42 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Figure 19 Answers to Check your progress are at the end of the section. EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 43 Answers Check your progress 1 Part A 1 (a) 2 (c) Part B 1 Check your Progress 2 1 Current lags voltage by 90°. 2 157 Check your Progress 3 44 (a) 3.7 H (b) 1162 (c) 0.206 A EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 Check your progress 4 Part A 1 (c) 2 (c) 3 (c) 4 (d) 5 (c) 6 (d) 7 (b) 8 (b) 9 (c) 10 (c) 11 (b) 12 (c) Part B 1 (a) 60 Ω (b) 0.19 H 2 2.5 A 3 942 Ω 4 0.061 H 5 0.032 H 6 (a) 0.217 H (b) 81.8 Ω (c) 1.34 A 7 (a) 6 H (b) 1885 Ω EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 45 (c) 0.127 A 8 (a) 0.531 H (b) 167 Ω (c) 0.168 A Check your progress 5 1 2.895 ohm 2 1.206 mA Check your progress 6 1 (a) 9.9 F (b) 321 (c) 0.746 A Check your progress 7 Part A 1 (d) 2 (c) 3 (c) 4 (a) 5 (d) 6 (a) 7 (c) 8 (c) 9 (a) 10 (d) 11 (a) 46 EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 12 (a) 13 (d) Part B 1 2 200 V 3 7.2 A 4 31.8 Ω 5 20 A 6 1.5 A 7 (a) 650 F (b) 4.1 Ω (c) 27 A EGG202A: 3 Analyse single element ac circuits NSW DET 2017 2006/060/04/2017 LRR 3811 47