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Circuits in the Frequency Domain

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Presentation on theme: "Circuits in the Frequency Domain"— Presentation transcript:

1 Circuits in the Frequency Domain
Topic 18 Circuits in the Frequency Domain ( )

2 Summary P P-1 Transforms Impedances Approach
1. Transform all voltages and currents to phasors 2. Solve the circuit 3. Transform the phasors back to the time domain Polar →Rectangular co-ordinates Special cases a b j A θ Rectangular → Polar co-ordinates 5/3/2019 Frequency Domain

3 Assessment 9.6 32mH 90Ω C vs i (a) Find the value of C that yields a steady-state output current i with a phase angle of -105° Basically What we want is for the phase angle of I to be -105° So what the problem really wants is 45° real and imaginary parts must be the same R 5/3/2019 Frequency Domain R

4 (b) Find the magnitude of the steady state output current
Assessment 9.6 32mH 90Ω C vs i (b) Find the magnitude of the steady state output current & we just set this one =R 5/3/2019 Frequency Domain

5 (a) Calculate the impedance at frequencies of 2 krad/s
Assessment 9.7 20Ω 5mH 25µF (a) Calculate the impedance at frequencies of 2 krad/s ZN (b) 8 krad/s is similar 5/3/2019 Frequency Domain

6 Standard trick to make denominator real
Assessment 9.7 20Ω 5mH 25µF (c) At what finite frequency does the impedance become purely resistive Standard trick to make denominator real ZN Need this to go to 0 (d) so so 5/3/2019 Frequency Domain

7 What is the maximum amplitude of the current in the inductor?
Assessment 9.9 20Ω 5mH 25µF it What is the maximum amplitude of the current in the inductor? iL Given what we know already about this problem, how can we write down an expression for iL by inspection? 150 cos4000t v We know ZN so we can easily compute the total current So Also 7.07 mS iL 45° .393 1.18 2.75 -.393 f=ω/2π T=1/f=2π/ω T=3.14 mS A Thus 5/3/2019 Frequency Domain

8 Assessment 9.11 ½Vx 10Ix Vx Voc Find the Thevenin equivalent wrt a-b
20 Ω j10 Ω 10Ix 10 Ω -j10 Ω Ix a b ½Vx Vx 10Ix Voc Find the Thevenin equivalent wrt a-b Find voc Node voltages appears a useful approach Note so Not as in text Right node Left node so 5/3/2019 Frequency Domain

9 Assessment 9.11 It 10Ix Vx Find the Thevenin equivalent wrt a-b Vt
j10 Ω Vx 10Ix 10 Ω a Find the Thevenin equivalent wrt a-b Vt 10Ix 245° A -j10 Ω Ix 20 Ω Find ZTh Turn off independent sources & apply a (phasor) test voltage at a-b b Find the current drawn from the test source The only solution is Ix=0 To find Ix we note so 5/3/2019 Frequency Domain

10 Problem 9.16 Find the steady state expression for io in the circuit if
vs 240mH 2.5mF io Find the steady state expression for io in the circuit if The total impedance seen by the voltage source is 4 In polar form So And 5/3/2019 Frequency Domain

11 Find and plot Vo/Vs as a function of ω (with ω on a log scale) if
Problem vs 5kΩ vo 10µF + - Find and plot Vo/Vs as a function of ω (with ω on a log scale) if Low Pass Filter Pass region Reject region 5/3/2019 Frequency Domain

12 Repeat the plot with the capacitor and resistor exchanged
Problem part b vs 5kΩ vo 10µF + - Repeat the plot with the capacitor and resistor exchanged High Pass Filter Reject region Pass region 5/3/2019 Frequency Domain

13 Problem 9.57 Use the node-voltage method to find Vo and Io
8 250° mA 40 Ω j20 Ω Vo 8 Io 16 Io 50 Ω -j25 Ω - + Vx Vo Use the node-voltage method to find Vo and Io Label the essential nodes Please note there is no current flowing between the two halves of the circuit because there’s no way for it to get back i.e. this current is 0 Sum the currents at the essential nodes 2 1 3 5/3/2019 Frequency Domain

14 Problem 9.57 1 2 3 2 into 3 4 Now put 4 into 1 Vo Vx j20 Ω 8 Vo Vo Io
250° mA 40 Ω j20 Ω Vo 8 Io 16 Io 50 Ω -j25 Ω - + Vx Vo 1 2 3 2 into 3 4 Now put 4 into 1 5/3/2019 Frequency Domain

15 Problem 9.62 100° 50° 10° -j1Ω j1Ω Use mesh-current method to find the branch currents Ia, Ib, Ic & Id. 1 Ia Ib Ic Id I2 Mark in the mesh currents I3 I4 1 + j2 5 1 6 2 3 2 + 3 4 5/3/2019 Frequency Domain

16 Problem 9.12 A 1000 Hz sinusoidal voltage with a maximum amplitude of 200 volts at t=0 is applied across the terminals of an inductor. The maximum amplitude of the steady-state current in the inductor is 25 A. (a) What is the frequency of the inductor current? L The same as the voltage Hz (b) What is the phase angle of the voltage? 2000° Max amplitude at t=0 means it’s a cosine wave: phase angle 0° magnitude (c) What is the phase angle of the current? -90° (d) What is the inductive reactance of the inductor? phase Reactance is the imaginary part of the imedance - i.e. ωL 5/3/2019 Frequency Domain

17 5/3/2019 Frequency Domain

18 End of this lecture 5/3/2019 Frequency Domain

19 Can this really be the end?
Ohh… Momma! Can this really be the end? 5/3/2019 Frequency Domain

20 To quote Jim Morrison Yeah, Bob, This… is... the... end. 5/3/2019
Frequency Domain


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