RLC Circuits Natural Response Ch. 8 – RLC Circuits RLC Parallel 2 RLC Series Natural Response The circuit has been working for a long time and the energy of capacitor or inductor suddenly released to the resistive network. Step Response The response of a circuit to the sudden application of a DC voltage or current source ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 3 Natural Response of RLC Parallel Applying KCL: 0 iC iL iR C dv 1 t v vd I 0 dt L 0 R d 2v 1 1 dv C 2 v 0 dt L R dt This is a second order homogeneous DE with constant coefficients. It admits the solution of the form As 2 e st v(t ) Ae st d 2 v 1 dv 1 v0 dt 2 RC dt LC 1 1 1 1 Ase st Ae st 0 Ae st s 2 s 0 RC LC RC LC Characteristic Equation 1 1 s + s+ =0 RC LC 2 ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 4 2 The roots of characteristic equation are Simplify the notation as 1 and 0 2 RC 2 1 1 1 s2 2 RC 2 RC LC s1 2 0 2 1 LC s2 2 0 2 The second order differential equation can be rewritten using α and ω0 as d 2v dv 2 2 0v 0 2 dt dt 1 1 1 s1 2 RC 2 RC LC The characteristic equation can be rewritten using α and ω0 as s 2 2 s 0 0 ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 5 Characteristic Equation Terminology Parameter s1, s2 The characteristic roots can be Terminology Value in Natural Response Characteristic Roots s1 2 0 2 s2 2 0 2 Neper Frequency 1 2RC 0 Resonant Radian Frequency 0 1 LC Real numbers and (distinct) 2 02 0 Two identical real numbers 2 02 0 Complex numbers (complex conjugates) ELEC 250 – Summer 2015 2 02 0 Ch. 8 – RLC Circuits 6 Real distinct roots 2 02 0 The solution Note that the constants A1 and A2 are determined by initial conditions as When the roots are real and distinct, the voltage response of parallel RLC circuit is said to be over-damped v ( t ) = A1es1t + A2es2t ELEC 250 – Summer 2015 dv(0 ) v(0 ) and dt Ch. 8 – RLC Circuits 7 Solution strategy for real distinct roots Step (1) Find the roots of the characteristic equation. dv(0 ) Step (2) Find v(0 ) and using circuit analysis. dt s1 2 0 2 s2 2 0 2 Step (3) Find the values of A1 and A2 using the values at step 2 as v(0 ) A1 A2 dv(0 ) iC (0 ) s1 A1 s2 A2 dt C Step (4) Substitute values of s1, s2, A1 and A2 from step (1) and (3) to obtain the expression of solution as v ( t ) = A1es1t + A2es2t ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 8 Duplicate real roots 2 02 0 The solution v t D1tes1t D2es1t Note that the constants A1 and A2 are determined by initial conditions as When the roots are real and duplicate, the voltage response of parallel RLC circuit is said to be critically-damped ELEC 250 – Summer 2015 dv(0 ) v(0 ) and dt Ch. 8 – RLC Circuits 9 Solution strategy for duplicate real roots Step (1) Find the roots of the characteristic equation. s1 s1 dv(0 ) Step (2) Find v(0 ) and using circuit analysis. dt Step (3) Find the values of D1 and D2 using step the values at step 2 as v(0 ) D2 dv(0 ) iC (0 ) D1 D2 dt C Step (4) Substitute values of s1, D1 and D2 from step (1) and (3) to obtain the expression of solution as v t D1tes1t D2es1t ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 10 Complex (conjugate) roots 2 02 0 The solution v t e t B1 cos d t B2 sin d t where damped radian frequency Note that the constants B1 and B2 are determined by initial conditions as When the roots are complex conjugate, the voltage response of parallel RLC circuit is said to be under-damped ELEC 250 – Summer 2015 d 2 2 0 dv(0 ) v(0 ) and dt Ch. 8 – RLC Circuits 11 Solution strategy for complex conjugate roots Step (1) Find the roots of the characteristic equation. Step (2) Find v(0 ) and s1 jd s2 jd dv(0 ) using circuit analysis. dt Step (3) Find the values of A1 and A2 using step the values at step 2 as v(0 ) B1 dv(0 ) iC (0 ) B1 d B2 dt C Step (4) Substitute values of s1, s2, B1 and B2 from step (1) and (3) to obtain the expression of solution as v t e t B1 cos d t B2 sin d t ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 12 Example: The two switches in the circuit operate synchronously. When switch 1 is in position a, switch 2 is in position d. When switch 1 moves to position b, switch 2 moves to position c. Switch 1 has been in position a for a long time. At t = 0, the switches move to their alternate positions. Find 𝒗𝒐 (𝒕) for 𝒕 > 𝟎 ? ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 13 Solution: ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 14 ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 15 Natural Response of RLC Series Applying KVL: t di 1 VR VL VC 0 Ri L id V0 0 dt C 0 d 2i di i L 2 R 0 dt dt C d 2i R di i 0 This is a second order homogeneous DE with constant coefficients. dt 2 L dt LC The RLC series DE can be written as d 2i di 2 2 i0 0 2 dt dt R 2L 0 1 LC Neper Frequency Resonant Frequency ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 16 Natural Response of RLC Series The series RLC circuit is governed by the same second order DE with constant coefficients as the parallel RLC circuit It admits the same solutions Two real roots Over-damped i t A1es1t A2es2t Duplicate roots Critically-damped i t D1tes1t D2es1t Two complex roots Under-damped i t est B1 cos d t B2 sin d t ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 17 Comparison Parallel/Series RLC Parameter s1, s2 Terminology Characteristic Roots Neper Frequency 0 Resonant Radian Frequency Value in Natural Response PARALLEL Value in Natural Response SERIES s1 2 0 2 s1 2 0 2 s2 2 0 2 s2 2 0 2 1 2RC 0 1 LC ELEC 250 – Summer 2015 0 R 2L 1 LC Ch. 8 – RLC Circuits 18 Example: In the following circuit, the resistor is adjusted for critical damping. The initial capacitor voltage is 15 V, and the initial inductor current is 6 mA. a) Find the numerical value of R. 𝒅𝒊 b) Find the numerical values of 𝒊 𝒕 and immediately after the switch is closed. 𝒅𝒕 c) Find 𝒗𝒄 (𝒕) for 𝒕 > 𝟎 ? ELEC 250 – Summer 2015 Ch. 8 – RLC Circuits 19 Solution: ELEC 250 – Summer 2015