Presentation is loading. Please wait.

Presentation is loading. Please wait.

Second-Order Circuits

Similar presentations


Presentation on theme: "Second-Order Circuits"— Presentation transcript:

1 Second-Order Circuits
Instructor: Chia-Ming Tsai Electronics Engineering National Chiao Tung University Hsinchu, Taiwan, R.O.C.

2 Contents Introduction Finding Initial and Final Values
The Source-Free Series RLC Circuit The Source-Free Parallel RLC Circuit Step Response of a Series RLC Circuit Step Response of a Parallel RLC Circuit General Second-Order Circuits Duality Applications

3 Introduction A second-order circuit is characterized by a second-order differential equation It consists of resistors and the equivalent of two energy storage elements

4 Finding Initial and Final Values
v and i are defined according to the passive sign convention Continuity properties Capacitor voltage Inductor current v i + _

5 Example

6 Example (Cont’d)

7 Example (Cont’d)

8 The Source-Free Series RLC Circuit

9 Cont’d Natural frequencies Damping factor Resonant frequency
Characteristic equation

10 Summary Three cases discussed Overdamped case :  > 0
Critically damped case :  = 0 Underdamped case :  < 0

11 Overdamped Case ( > 0)
i(t)

12 Critically damped Case ( = 0)

13 Critically damped Case (Cont’d)

14 Underdamped Case ( < 0)

15 Underdamped Case (Cont’d)
i(t)

16 Finding The Constants A1,2

17 Conclusions The concept of damping Oscillatory response is possible
The gradual loss of the initial stored energy Due to the resistance R Oscillatory response is possible The energy is transferred between L and C Ringing denotes the damped oscillation in the underdamped case With the same initial conditions, the overdamped case has the longest settling time. The critically damped case has the fastest decay.

18 Example Find i(t). t < 0 t > 0

19 Example (Cont’d) t < 0 t > 0

20 The Source-Free Parallel RLC Circuit

21 Summary Overdamped case :  > 0 Critically damped case :  = 0
Underdamped case :  < 0

22 Finding The Constants A1,2

23 Comparisons Series RLC Circuit Parallel RLC Circuit

24 Example 1 Find v(t) for t > 0. v(0) = 5 V, i(0) = 0
Consider three cases: R =  R = 5  R =6.25 

25 Example 1 (Cont’d)

26 Example 1 (Cont’d)

27 Example 2 Find v(t). Get x(0). Get x(), dx(0)/dt, s1,2, A1,2.

28 Example 2 (Cont’d) t > 0 t < 0

29 Step Response of A Series RLC Circuit

30 Characteristic Equation

31 Summary (Overdamped) (Critically damped) (Underdamped)

32 Example Find v(t), i(t) for t > 0. Consider three cases: R = 5 
Get x(0). Get x(), dx(0)/dt, s1,2, A1,2. t < 0 t > 0

33 Case 1: R = 5 

34 Case 2: R = 4 

35 Case 3: R = 1 

36 Example (Cont’d)

37 Step Response of A Parallel RLC Circuit

38 Characteristic Equation

39 Summary (Overdamped) (Critically damped) (Underdamped)

40 General Second-Order Circuits
Steps required to determine the step response Determine x(0), dx(0)/dt, and x() Find the transient response xt(t) Apply KCL and KVL to obtain the differential equation Determine the characteristic roots (s1,2) Obtain xt(t) with two unknown constants (A1,2) Obtain the steady-state response xss(t) = x() Use x(t) = xt(t) + xss(t) to determine A1,2 from the two initial conditions x(0) and dx(0)/dt

41 Example Find v, i for t > 0. Get x(0).
Get x(), dx(0)/dt, s1,2, A1,2. t < 0 t > 0

42 Example (Cont’d) t < 0 t > 0

43 Example (Cont’d) t > 0

44 Duality Duality means the same characterizing equations with dual quantities interchanged. Table for dual pairs Resistance R Conductance G Inductance L Capacitance C Voltage v Current i Voltage source Current source Node Mesh Series path Parallel path Open circuit Short circuit KVL KCL Thevenin Norton

45 Example 1 Series RLC Circuit Parallel RLC Circuit

46 Example 2

47 Application: Smoothing Circuits
Output from a D/A vs v0


Download ppt "Second-Order Circuits"

Similar presentations


Ads by Google