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Chapter 4 – Electric Power Definitions Under Probability Conditions: The Radomness Power Alexander E. Emanuel 5.1 - Introduction Let’s assume an observation time T , hours or days, divided in equal observation time intervals T such that T T . For each interval i , 1 i , a measuring instrument V / I / records voltage and current harmonic phasors hi hi and hi hi , ( h 1, 2, 3, where h is the harmonic order), The rms voltage and current, Vi and I i , as well as symmetrical components may be also computed and recorded. The intervals T are small enough to consider these quantities as cyclic within each time interval or to assume the interval as a period of a recurrent set of signals. This approach enables, for each interval i , the computation and recording of apparent S i , active Pi , and different nonactive powers N i , Qi , D Ii , DVi (for the definitions of these powers see ref. [1]). Evidently each electrical quantity will be characterized by a certain probability distribution for the observation time T. The main issue to be clarified on this approach is the formulation of correct definitions that characterize the flow of electric energy for the entire duration T. As it will be explained, the mean value is the representative quantity for each of the total apparent components, regardless of the type of probability distribution. However, this is not true for the total apparent power. A most significant fact is that if such probabilistic methods are used there is necessary to include a new type of nonactive power, the randomness power DR . 5.2- Single-Phase Sinusoidal Case. This is the simplest case and it will help prove the existence of the randomness power. For each interval i there are the active and reactive powers Pi Vi Ii cos(i ) (1) Qi Vi Ii sin( i ) (2) For the total observation time T the rms values of the voltage and current are V 1 2 1 2 Vi T Vi T i 1 i 1 I 1 2 1 2 Ii T Ii T i 1 i 1 (3) (4) yielding a total apparent power S V I (5) The total active or real power for the duration T is P 1 1 Pi T Pi P T i 1 i 1 (6) i.e. the mean of all the measured active powers Pi . The reactive power can be defined starting from the total lost energy W in the supply line. Assuming the resistance of the line that supplies the monitored load to be r , the total lost energy is Pi 2 Qi2 (7) W r T Vi 2 i 1 an has two distinct terms: one proportional with the squared active power and the other proportional with the reactive powers squared. A power factor compensating capacitor meant to minimize W will “deliver” the reactive power QC . The optimum value of QC can be found by minimizing the function F (QC ) i 1 (Qi QC ) 2 Vi 2 (8) which leads to Qi V 2 1 (9) Q Q 1 i 1 i 2 i 1 Vi This result helps define for the total reactive power when the powers are monitored as QC i 1 i statistics and holds true for any type of probability distribution. A simple numerical example will help shade light on this approach. A random load has its voltage, current and power recorded for five equal intervals, (Table I). This hypothetical load is assumed to be a resistance that varies randomly. The total rms voltage and current (3) and (4) are V 99.92 V and I 124.90 A giving an apparent power S 12,480.0 VA. The active power (6) is P 11,579.6 W leading to a power factor PF P / S 0. 928. This result indicates that a certain type of nonactive power exists, otherwise the apparent and the active powers will be equal. Table I. i Vi (V) 1 100.0 2 99.5 3 99.8 4 100.1 5 100.2 I i (A) 100.0 180.0 160.0 80.0 60.0 Pi (W) 10,000.0 17,910.0 15,968.0 8,008.0 6,012 The nonactive power in question is the Randomness Power and in this example it has the value DR S 2 P2 4,654.5 var In the general case the substitution of (1), (2), (3) and (4) in (5) gives S 2 V 2I 2 1 1 2 1 2 2 2 2 2 Vi I i Vi [ I i cos(i )] Vi [ I i sin( i )] 2 2 2 i 1 i 1 i 1 i 1 i 1 i 1 (10) By applying Lagrange’s identity 2 2 2 1 ai bi aibi i 1 i 1 i 1 2 (ambn anbm ) m 1 n m 1 to the squared apparent power (10), one finds 2 1 1 S 2 Vi I i cos(i ) i 1 m 1 2 2 1 1 V I sin( ) i i i 2 i 1 m 1 2 P Q 2 V n m 1 m V n m 1 m I n cos( n ) Vn I m cos(m ) I n sin( n ) Vn I m sin( m ) (11) D R2 where DR 1 2 2 (Vm I n ) (Vn I m ) 2VmVn I m I n cos(m n ) m1 n m1 (12) is the expression of the randomness power (measured in var). In practical situations S is computed from (3), (4) and (5), P and Q are computed from (6) and (9) and DR from (11), i.e. from the basic formula Q DR S 2 P 2 2 This approach enables the incorporation in DR of the randomness reactive power, a minute component, otherwise neglected by the approximation (9). 5.3- Three-Phase, Sinusoidal and Unbalanced The IEEE Std. 1459 – 2000 [1] recommends the use of effective apparent power Se 3Ve I e (13) where Ve and I e are the effective voltage and current, respectively Ve2 (V ) 2 Vu2 (14) I e2 ( I ) 2 I u2 (15) with V , I the positive-sequence voltage and current and the residual voltage and current Vu , I u , caused by the load imbalance. According to IEEE Std. 1459 the imbalance components Vu , I u are function of the negative- and zero-sequence components, i.e. Vu2 (V ) 2 (V 0 ) 2 / 2 and I u2 ( I ) 2 4 ( I 0 ) 2 From (13), (14) and (15) is found that the effective apparent power (13), can be separated in two components: Se2 9Ve2 I e2 ( S ) 2 Su2 (16) where S is the positive-sequence apparent power, considered as the most important component. The positive-sequence active and reactive powers which are the useful and dominant terms, S ( P )2 (Q )2 ; P 3V I cos( ) Q 3V I sin( ) The second term is the unbalanced power (VA) Su (V Iu ) 2 (Vu I ) 2 (Vu Iu ) 2 (17) The unbalanced power has three sub-terms; the third term Vu Iu contains the active and nonactive powers associated with the negative- and the zero-sequence components that can be easily separated from S u . The case we are interested in is when the stored information recorded for the equal times intervals includes the voltages Vi , Vui , the currents Ii , Iui and the powers Pi and Qi . The effective voltage and current for the total duration of time T are 1 Ve [(V Ie 1 i 1 ) 2 Vui2 ] (18) ) 2 I ui2 ] (19) i [( I i 1 i thus, the total effective apparent power squared has four terms 2 2 2 2 Vi Ii Vi Iui 9 i 1 i 1 i 1 i 1 2 Se 9Ve I e 2 2 2 2 2 Vui I ui Vui I i i 1 i 1 i 1 i 1 (20) The first term is due to the positive-sequence components and just like in the previous case leads to three components: 9 2 (S ) 2 2 i 1 Ii i 1 2 2 Vi 2 P Q DR where P Q 1 (21) 2 ; Pi 3Vi I i cos(i ) (22) Qi ; Qi 3Vi I i sin( i ) (23) Pi i 1 1 2 2 1 9 Vi I i Vm I n Vn I m 2 m 1 n m 1 i 1 are the total positive-sequence active and reactive powers and DR 9 1 2 m 1 n m1 9 1 2 2 [Vm I n Vn I m ] 2 2 (Vm I n ) (Vn I m ) 2Vm Vn I m I n cos(m n ) m1 n m1 (24) is the positive-sequence randomness power The remaining three terms in (20), correspond to the three terms in (17), leading to the following expressions: 9 2 i 1 i 1 (Vi ) 2 ( I ui ) 2 S u' 2 ' DuR 2 with Su' 9 2 3 Vi I i 1 ui i 1 i 1 D (Vui ) 2 ( I i ) 2 S u'' 9 ' DuR and 2 2 1 m 1 n m 1 ( Vm I un Vn I um ) 2 '' 2 uR with S u' ' 3 Vui I i i 1 '' DuR and 9 2 1 m 1 n m 1 1 m 1 n m 1 ( Vum I n Vun I m ) 2 and 9 2 i 1 i 1 (Vui ) 2 ( I ui ) 2 S u''' 2 ''' DuR 2 with S u' ' ' 3 Vui I ui i 1 ''' DuR and 9 2 ( Vum I n Vun I m ) 2 Thus the final expression of the total effective apparent power for the duration T T is S e2 where 2 2 2 P Q S u DR2 (25) S S S S 2 ' u u 2 '' u 2 ''' u 2 and 2 DuR' 2 DR'' 2 DuR''' 2 DR2 DR 5.4- Three-Phase Systems with Nonsinusoidal and Unbalanced Conditions This is the general case. For each time interval i, the effective voltage and current are recorded, moreover the fundamental component is separated from the total harmonics component, i.e. 2 Vei2 Ve21i VeHi 2 2 I ei I e21i I eHi and where Ve1 and I e1 are the effective fundamental voltage and current and VeHi and I eHi are given by the expressions VeHi 2 Vehi I eHi and h 1 The total effective apparent power squared is Ve1i 2 2 9 9 i 1 Se2 9Ve I e Vei I ei 2 2 i 1 i 1 2 I ehi h 1 2 2 I eHi i 1 i 1 (26) 2 2 2 2 VeHi I e1i VeHi I eHi i 1 i 1 i 1 i 1 2 I e1i i 1 2 Ve1i The first term is due to the contributions of the fundamental voltage and current and has exactly the same terms as (25), 2 i1Ie1i 2 i 1 9 Ve1i 2 2 2 2 P1 Q1 S1u D12R The second term is due to the interaction between the fundamental voltages and the harmonic currents 2 2 2 2 I eHi DI DIR 2 i 1 i 1 9 Ve1i with DI 1 3Ve1i I eHi and i 1 D IR 3 1 V m 1 n m 1 I e1m eHn Ve1n I eHm 2 being the current distortion power and the randomness current distortion power, respectively. The third term is due to the interaction between the harmonic voltages and the fundamental currents 9 2 VeHi2 i 1 I i 1 2 e1i DV 2 2 DVR with DV 1 3VeHi I e1i and DVR 3 1 V I VeHn I e1m I VeHn I eHm 2 i 1 m 1 n m 1 being the voltage distortion power and the randomness voltage distortion. The fourth term is due to the interaction between the harmonic voltages and the harmonic currents 9 2 VeHi2 i 1 I i 1 2 eHi SH 2 eHm e1n 2 D HR with SH 1 3V i 1 eHi I eHi and DHR 3 1 V m 1 n m 1 eHm eHn 2 The total harmonic apparent power S H can be further separated in the harmonic active power PH and the nonactive harmonic power N H . Finally, for the general case the apparent power squared can be resolved using the expression Se2 2 2 2 2 S1 S1u DI DV 2 S H DR2 where 2 2 2 DR D12R DIR DVR DHR is the total randomness power. (27) 5.5- Conclusions It is common practice to observe electrical quantities by means of statistics. A large time interval is divided in a finite number of small observation times and for each observation time the electrical quantities of interest are measured and recorded thus leading to probability densities for each one of the monitored quantities. The present study proves that for the active and nonactive powers the equivalent value for the large time interval is always the mean value. For the apparent power however, this property does not apply. The apparent power is determined from the product of the equivalent or effective rms voltages and currents. Under these circumstances the apparent power resolution has to include a new type of nonactive power, named randomness power. The randomness power is to be considered only when the apparent power is an equivalent value for a load or a cluster of load that are monitored using a statistical approach. Whenever randomness is present the subharmonics can be detected. If the subharmonics and their associated powers are included, i.e. if the approach to the measurement for the total duration T is deterministic, then the randomness power is nil. 5.6- References [1] IEEE Std. 1459 – 2000, “Definitions for the Measurement of Electric Power Quantities Under Sinusoidal, Nonsinusoidal Balanced or Unbalanced Conditions,” Trial-Use June 2000, Full-Use August 2002.