Alternating Current. Asist. Prof. Dr. Aytaç Gören Asist. Prof. Dr. Levent Çetin
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1 Asist. Prof. Dr. Aytaç Gören Asist. Prof. Dr. Levent Çetin
2 Contents Alternating Voltage Phase Phasor Representation of AC Behaviors of Basic Circuit Components under AC Resistance, Reactance and Impedance Power in AC Circuits 2
3 Capacitor Capacitors react different due to the voltage level applied to them under alternating current. If the voltage level applied is greater than the voltage on a capacitor, the source charges the capacitor; in opposite case, capacitor behaves like a source. The current equation for a capacitor is: i( t) C dv( t) dt 3
4 4
5 The phase difference between voltage and current is 90 degrees on a capacitor or in other words, current leads voltage 90 degrees. This case results with negative electrical power which means that capacitor transfers power to the circuit (i.e. Capacitor discharges its electrical charge). The resistance of the capacitors change due to the frequency of the alternating voltage. The higher frequency of the AC signal, the more easily that signal will pass through the capacitor. Thus, this is called as capacitive reactance, X c. 1 X c wc 1 X C 2 fc 5
6 Let us examine the behavior of the capacitor in the circuit mathematically. The current can be found using the capacitive reactance equation and the implementation of Ohm s Law to AC easily. 6
7 The current of the AC source leads the voltage of the source 90 degrees. The resistance effect of the capacitor to AC source is calculated considering this. 7
8 Adding a 5 [Ohm] resistor to this circuit, let us calculate the total effect of the resistor and the capacitor. The total resistance in this circuit is found as: X c j R 5 0j Z R X c j
9 Implementing the Ohm s Law to the circuit, the current is calculated. In this analysis, the phase of the source is always zero (0). As it can be considered easily, the phase shift is degrees in this circuit whereas in the circuit that has only one capacitor it was 90 degrees. 9
10 Using phasor diagrams, Let us examine the last table carefully. The current and the voltage on the resistor is on the same phase as it is mentioned. However, the current on a capacitor leads voltage by 90 degrees. 10
11 Parallel Resistor Capacitor Circuit 11
12 12
13 Resistor, Reactance and Impedance The resistance against the current can be in three types: 1. Resistor: It is the friction of electrons during motion. Its symbol is R and unit is [ ] (i.e. [Ohm]). It does not form any phase shift. 2. Reactance: It is the inertia of electrons. It occurs if there is a change in voltage or current values (if an electric or magnetic field occurs). The capacitor and inductor are the main circuit components which this influence is highly distinct. If there is a reactance effect in a circuit, there is also phase shift. If the component is a capacitor, the current leads voltage by 90 degrees whereas if it is an inductance, the current lags voltage by 90 degrees. 13
14 3. The impedance, is the strain against the current in an electrical circuit. In aother words, it is the resistance against the motion of electrons. Impedance is the total resistance and reactance effects of all components. The resistance in DC circuits is the impedance in AC s. The AC implemented Ohm s Law can be seen as below. Please consider that all the quantities are in complex number form in the equation below : Z V I Like Ohm s Law, other laws (Kirrschoff s, grid theorems, etc.) used in circuit analysis can be also implemented in AC in condition of using complex numbers. It is the power calculations that the AC and DC calculations differes. The next subject will be about this case. 14
15 Resistor (R) Coil (L) (Inductor) Capacitor(C) (Condenser) 15
16 Serial R-L-C Circuits 16
17 17
18 18
19 It should be considered that the amplitude of the voltage on the capacitor is greater than the voltage supplied to the circuit. The reason is that the influence of the reactance of the coil effects just the opposite according to the influence of the reactance of the coil to the circuit. The influence of the impedance in the whole circuit is smaller than the influence of impedance of any single component. This case causes higher voltages on single components. However, this does not change the Kirchhoff s Law about the the total voltages in a circuit (0+0j). 19
20 Parallel R-L-C Circuit 20
21 21
22 22
23 Serial and Parallel Circuits 23
24 The calculation of impedance in this circuit should be completed step by step. First, serial connection branch of C 2 and L, afterwards the parallel branch of resistor and last the serial capacitor effects should be calculated. 24
25 25
26 26
27 27
28 Power in AC Circuits Since it was mentioned, there is a phase shift between current and voltage in AC circuits. The reason is the impedance as it was stated. There are three definitions in AC circuits which are related with power. These are: True power (active power), Reactive power, Apparent power. 28
29 Power in AC Circuits The reactive power that is referring to the influence of reactance is: The apparent power is the power related with the impedance: 29
30 Power in AC Circuits The power quantities are scalar quantities. It is a prependicular triangle that we get if we draw the calculated values, considering the 90 degrees of direction angle between the resistor and the reactance and phase shift in the circuit. This triangle is called as Power Triangle. As it is seen in this triangle, a part of the power is lost in an AC circuit. The generated effective power is just as the true power. Power factor is the cosine of the angle between the true and apparent powers (cos ). This value is equal to 1 in only circuits those have just resistors. But if there is a reactance, then the value is between 0 and 1. 30
31 Power in AC Circuits To examine the effect of the reactance, let us calculate the P, Q and S powers in this circuit. The power factor of this circuit may be found using the definition below. 31
32 Power in AC Circuits The power factor value shows that the 70.5 % of the power used from the grid is served for the purpose. This situation is not wanted. So, in circuit design stage, it must be noted that the power factor is approximately equal to 1. For this reason, the capacitive and inductive ractance values should be equal to each other. If this is not possible, a capacitor or an inductor should be externally added to the circuit. This improvement is called as compensation. Now, let us calculate the reactance of the same circuit. 32
33 Power in AC Circuits The ractance in this circuit is inductive. In othe words, the coil is the reason of ractance. To compensate this, let us add a capacitor to the circuit. Using the calculations below, the capacitor value that can form a capacitive ractance to generate the same inductive ractance value but in opposite direction might be found. 33
34 Power in AC Circuits The capacitor value found is not a standart value for capacitors, so the closest standart value shold be chosen (22 µf) and connected in parallel with the circuit. Now let us examine this case: The new impedance value is: 34
35 Power in AC Circuits And the new power factor is: As seen above, this improvement made the power factor closer to 1. Besides, the current is decreased. These two results indicate that the circuit is improved in means of efficiency and economic. 35
36
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