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M utual Inductance & Transformer

M utual Inductance & Transformer. Electric Circuit. Chairul Hudaya, M.Sc Electric Power and Energy Studies (EPES) Department of Electrical Engineering Universitas Indonesia http://www.ee.ui.ac.id/epes/hudaya. M. i 1. i 2. v 1. v 2. L 1. L 2. Coil 2. Coil 1.

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M utual Inductance & Transformer

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  1. Mutual Inductance & Transformer Electric Circuit Chairul Hudaya, M.Sc Electric Power and Energy Studies (EPES) Department of Electrical Engineering Universitas Indonesia http://www.ee.ui.ac.id/epes/hudaya

  2. M i1 i2 v1 v2 L1 L2 Coil 2 Coil 1 CIRCUIT WITH MUTUAL INDUCTANCE PASSIVE SIGN CONVENTION : Arrows for I1 and I2 point into plus end of V1 and V2 DOT CONVENTION : If both current reference arrows point into dotted ends or both into undotted ends of inductor, use plus sign for both mutual inductance, otherwise use the minus sign

  3. Dot Convention The dots are placed in such a manner that the currents entering (or leaving) both the dotted terminals will produce adding magnetic flux. In this case the mutual flux linkages will add to the self flux linkages.(Case I) Conversely, if current enters through one dotted terminal and leaves through the other, they produce opposing flux. In this case mutual flux linkages subtract from self linkages.(Case II)

  4. i1 i2 M L1 L2 Coil 2 Coil 1 Case I v1 v2

  5. Case 1: jM + + V1 I1 V2 I2 • • _ _ jL1 jL2 V1 = jL1I1 + jMI2 V2 = jL2I2 + jMI1

  6. i1 i2 M L1 L2 Coil 2 Coil 1 Case II v1 v2

  7. Case 2: jM _ + • I1 V1 V2 I2 • _ + jL2 jL1 V1 = jL1I1 + jMI2 V2 = jL2I2 + jMI1

  8. Circuits with Mutual Inductance

  9. Example 1: j8 -j4 6 2 • + + I1 I2 va(t) vb(t) j6 j10 _ _ • va(t) = 50cos(400t + 30) V vb = 80cos(400t – 40) V Va = 50300 V Vb = 80-400 V

  10. EXAMPLE 1: Continued j8 -j4 6  2  • + + I1 I2 j10  j6  80-40 V 5030V _ _ • Solve for I1 and I2 Mesh 1 (2 + j10)I1 + j8I2 = 5030 j8I1 + (j6 – j4 + 6)I2 = - 80-40 Mesh 2 (2+j10) j8 I1 5030 = Matrix Form j8 (6+j4) I2 -80-40

  11. Example 2: 8  -j4  j8  j10  • • j3  + j5  12  200 V I1 _ I2 6  Solve for I1 and I2

  12. Example 2: Continued 8  -j4  j8  j10  • • j3  + j5  12  200 V I1 _ I2 6  (8 + j10 + j5 + 6)I1 - (j5 + 6 + j3)I2 = 200 Mesh 1: Mesh 2 -(6 + j5 + j3)I1 + (6 + j5 + j8 – j4 + 12 + j3)I2 = 0 (14+j15) -(6+j8) I1 200 Matrix = -(6+j8) (18+j12) I2 0

  13. BASIC TRANSFORMER From figure V2=ZL.I2 so : Substitute I2 we have :

  14. Simplify Circuit – one loop circuit Reflected impedance ZR

  15. SECONDARY TO PRIMARY RATIO CURRENT RATIO VOLTAGE RATIO

  16. IDEAL TRANSFORMER

  17. n= N2/N1 called turn ratio of transformer Voltage Ratio Current Ratio

  18. IDEAL TRANSFORMER LAWS Define the primary variables (I1,V1) to satisfy and the secondary variable to violate the passive sign convention. Then if I1 or I2 point into dotted end while the other point into undotted end, use plus sign in both i-v laws, otherwise use minus sign

  19. EXAMPLE

  20. IMPEDANCE REFLECTED • REFLECTED LOAD INTO PRIMARY

  21. Contoh • Suatu generator menyuplai beban , spesifikasi rating generator tersebut adalah : • V rat = 500 volt S rat = 100 kVA

  22. SISTEM PER-UNIT Besaran yang dijadikan basis utama adalah Daya Semu (S) dan Tegangan (V)

  23. Ubah komponen dalam Unit

  24. Besarnya I sebenarnyauntuktiap area dapatdiperolehdenganmengalikannilaiI perunitdengannilai I basisnyadi area tersebut

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