New Formula to Determine the Minimum Capacitance Required for Self-Excited Induction Generator Ali Mohamed Ahmed El-Tamaly Electrical Engineering Department, Faculty of Engineering Elminia University, Elminia, Egypt Self Excited Induction Generator Equipped with SCR Rectifier / LCI Inverter Io Rectifier UG VI VR IG LCI 100 80 60 40 20 0 0 i (t ) = 0.5k 1.0k 1.5k 2.0k 2.5k 5 7 11 13 I o cos (ωt ) − cos (5ωt ) − cos (7ωt ) + cos (5ωt ) + cos (13ωt ) ...... 2 3 1 1 1 1 π Utility interfacing of SCIG via diode rectifier and PWM inverter Rectifier PWM VR Electric Utility VI IG Induction Generator Equipped with PWM Rectifier / LCI Inverter Variable frequency PWM Converter S1 Ia S3 a IG S2 Ib b S4 DC Link S5 Ic S6 C LCI Inverter Electric Utility Most of previous work uses numerical iterative method to determine this minimum capacitor. But the numerical iteration takes long time and divergence may be occurs. For this reason it cannot be used online. A new simple formula for the minimum self-excited capacitor required for induction generator is presented here. By using this formula there is no need for iteration and it can be used to obtain the minimum capacitor required online. Complete mathematical analysis for induction generator to drive this new formula is presented. The result from this new formula is typical as the results from iterative processes The IEEE recommended equivalent circuit of three-phase induction generator. Vt RL -jXc jXr jXs Rs Is Rr s jXm jXL Where the slip S is shown in equation (1) N sa − N a a − b = S= N sa a a: a is Pu frequency fa/fr and speed Na/Nsr. b is Pu The loop equation for IS of Fig.2 can be written as :- IS Z = 0 (3) Where Z is the loop impedance seen by the current, IS and can be obtained as in (4) Z=Zm+ZLC+Zs (4) Zm = ( Xm ) Rr a −b - jX C RL Z LC = 2 + jX L a a Rs Zs = + jX S a In steady state operation IS ≠ 0 otherwise there is no generated voltage , Then Z=Zm+ZLC+Zs =0 (4) By equating both the real and imaginary parts of (3) by zero we get two nonlinear equations ((5) and (6)) in function of Xm and a. Solving (5) and (6) together yields the values of Xm and a. P ( X m , a ) = ( A1 X m + A2 ) a 3 + ( A3 X m + A4 ) a 2 + ( A5 X m + A6 ) a + ( A7 X m + A8 ) = 0 Q( Xm , a) = (B1 Xm + B2 )a4 + (B3 Xm + B4 ) a3 + (B5 Xm + B6 ) a2 + (B7 Xm + B8 ) a + B9 = 0 it is possible to compute Cmin by using the following iterative procedure If we use the value of Xm in the calculation of Cmin then we can modifie (5) and (6) to be as shown in (7) and (8) are function in a and XC. − a1a3 + a2 a2 + (a3 X C + a4 )a − a5 X C = 0 (7) − b1a 4 + b2 a 3 + (b3 X C + b4 )a 2 (8) + (b5 X C + b6 )a − b7 X C = 0 Then by separation of XC in (7) and (8) a1a 3 − a2 a 2 − a4 a XC = a3 a − a5 b1a 4 − b2 a 3 − b4 a 2 − b6 a XC = b3 a 2 − b5 a − b7 (9) (10) By equating the right hand sides in (9) and (10) then we have the following equation:- (a1 b3 − a3 b1 ) a 4 − (a2 b3 + a1 b5 − a3 b2 − a5 b1 ) a 3 (12) + (a 2 b5 + a3 b4 − a 4 b3 − a1 b7 − a5 b2 ) a 2 − (a3 b6 + a5 b4 − a 4 b5 − a 2 b7 ) a + (a5 b6 + a 4 b7 ) = 0 From (12) the frequency can be calculated and then substitute this frequency in (9) or (10) to calculate XC and Cmin. NEW FORMULA TO CALCULATE CMIN BY USING NODAL ANALYSIS YL YC Rs a Vt/a RL a Yin JXc a2 Xr Xs Is Xm JXL Vt Yt = 0 a Where Yt =Yin +YL +YC (13) Rr a-b C4 = X L2 Rr (L2 L3 − L1 ) + X L2 RS L22 + RL L12 C3 = X L2 Rr v (L1 − L2 L3 ) − 2v( X L2 RS L22 + R L L12 ) ( C2 = RL2 (Rr L22 − Rr L1 + Rr L2L3 + XL2Rs Rr2 + L22v2 ) + 2 * RL Rr Rs (L2 L3 − L1 ) + RL (L12v2 + Rr2L3 + Rs2L22 C1 = RL2 Rr v (L1 − L2 L3 ) − 2v RL Rs L22 (RS + RL ) ( ) C0 = Rr2 + L22 v2 RL Rs (RL + Rs ) 1From the imaginary part we can drive a simple formula for the minimum value of terminal capacitor as shown in (17). M4 1 XLa Cmin = + 2 2 2π M3 M1 + M2 M 1 = Rs Rr − f ( f − v) L1 M2 = Rr f L3 + Rs ( f −v) L2 M3 = R + X f 2 L 2 L 2 M4 =Rr *M2 − L2 f ( f −v)M1 100 80 60 40 20 0 C min 50 100 150 %speed 200 Variation of Cmin with rotational speed at RL=1pu and unity power factor. 100 80 60 40 20 0 50 100 150 %speed 200 Variation of Cmin with rotational speed at no load. CONCLUSIONS In this paper a new formula for the minimum capacitance required for selfexcited induction generator is presented. This new formula is simple and it does not need numerical iteration. For this reason this new formula helps to determine the minimum capacitance required for self excited induction generator on line. The new formula gives typical results as the results obtained from iterative technique without any iteration or divergence problem.
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