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# Elektronika (12)

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### Elektronika (12)

1. 1. Elektronika<br />AgusSetyo Budi, Dr. M.Sc<br />Sesion #12<br />JurusanFisika<br />FakultasMatematikadanIlmuPengetahuanAlam<br />
2. 2. Outline <br />20-1: How XL Reduces the Amount of I<br />20-2: XL = 2πfL<br />20-3: Series or Parallel Inductive Reactances<br />20-4: Ohm's Law Applied to XL<br />20-5: Applications of XLfor Different Frequencies<br />20-6: Waveshape of vLInduced by Sine-Wave Current<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />2<br />07/01/2011<br />
3. 3. Inductive Reactance<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />3<br />
4. 4. 20-1: How XL Reduces the Amount of I<br />An inductance can have appreciable XL in ac circuits to reduce the amount of current. <br />The higher the frequency of ac, and the greater the L, the higher the XL.<br />There is no XL for steady direct current. In this case, the coil is a resistance equal to the resistance of the wire.<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />4<br />
5. 5. 20-1: How XL Reduces the Amount of I<br /><ul><li>In Fig. 20-1 (a), there is no inductance, and the ac voltage source causes the bulb to light with full brilliance.
6. 6. In Fig. 20-1 (b), a coil is connected in series with the bulb.
7. 7. The coil has a negligible dc resistance of 1 Ω, but a reactance of 1000 Ω.
8. 8. Now, I is 120 V / 1000 Ω, approximately 0.12 A. This is not enough to light the bulb.
9. 9. In Fig. 20-1 (c), the coil is also in series with the bulb, but the battery voltage produces a steady dc.
10. 10. Without any current variations, there is no XLand the bulb lights with full brilliance.</li></ul>07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />5<br />
11. 11. 20-2: XL = 2πfL<br />The formula XL = 2πfL includes the effects of frequency and inductance for calculating the inductive reactance.<br />The frequency is in hertz, and L is in henrys for an XL in ohms.<br />The constant factor 2π is always 2 x 3.14 = 6.28.<br />The frequency f is a time element.<br />The inductance L indicates the physical factors of the coil.<br />Inductive reactance XL is in ohms, corresponding to a VL/IL ratio for sine-wave ac circuits.<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />6<br />
12. 12. 20-3: Series or Parallel Inductive Reactances<br /><ul><li>Since reactance is an opposition in ohms, the values XL in series or in parallel are combined the same way as ohms of resistance.
13. 13. With series reactances, the total is the sum of the individual values as shown in Fig. 20-5 (a).
14. 14. The combined reactance of parallel reactances is calculated by the reciprocal formula.</li></ul>Fig. 20-5<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />7<br />
15. 15. 20-4: Ohm's Law Applied to XL<br />The amount of current in an ac circuit with only inductive reactance is equal to the applied voltage divided by XL.<br />I = V/XL = 1 A<br />I = V/XLT = 0.5 A<br />I1 = V/XL1 = 1 A<br />I2 = V/XL2 = 1 A<br />IT = I1 + I2 = 2 A<br />Fig. 20-6: <br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />8<br />
16. 16. 20-5: Applications of XLfor Different Frequencies<br />The general use of inductance is to provide minimum reactance for relatively low frequencies but more for higher frequencies.<br />If 1000 Ω is taken as a suitable value of XL for many applications, typical inductances can be calculated for different frequencies. Some are as follows:<br />2.65 H 60 Hz Power-line frequency<br />160 mH 10,000 Hz Medium audio frequency<br />16 mH 10,000 Hz High audio frequency<br />1.6 μH 100 MHz In FM broadcast band <br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />9<br />
17. 17. 20-6: Waveshape of vLInduced by Sine-Wave Current<br />Induced voltage depends on rate of change of current rather than on the absolute value if i.<br />A vL curve that is 90° out of phase is a cosine wave of voltage for the sine wave of current iL.<br />The frequency of VL is 1/T.<br />The ratio of vL/iL specifies the inductive reactance in ohms.<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />10<br />
18. 18. 20-6: Waveshape of vLInduced by Sine-Wave Current<br />di/dt<br />di/dt for Sinusoidal Current is a Cosine Wave <br />di<br />L<br />vL =<br />dt<br />0<br /><br />Current<br />Sinusoidal Current<br />Iinst. = Imax× cos <br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />11<br />
19. 19. 20-6: Waveshape of vLInduced by Sine-Wave Current<br />V<br />Amplitude<br />0<br />Time<br />Θ = -90<br />I<br />V<br />I<br />Inductor Voltage and Current<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />12<br />
20. 20. 20-6: Waveshape of vLInduced by Sine-Wave Current<br />Application of the 90° phase angle in a circuit<br />The phase angle of 90° between VL and I will always apply for any L with sine wave current.<br />The specific comparison is only between the induced voltage across any one coil and the current flowing in its turns.<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />13<br />
21. 21. 20-6: Waveshape of vLInduced by Sine-Wave Current<br /><ul><li> Current I1 lags VL1 by 90°.
22. 22. Current I2 lags VL2 by 90°.
23. 23. Current I3 lags VL3 by 90°.</li></ul>NOTE: I3 is also IT for the series-parallel circuit.<br />Fig. 20-8<br />07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />14<br />
24. 24. 07/01/2011<br />© 2010 Universitas Negeri Jakarta | www.unj.ac.id |<br />15<br />TerimaKasih<br />