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ThetransferfunctionofalinearsystemisPracticeProblem16.7 The transfer function of a linear system is Practice Problem 16.7

H(s) = \frac{2s}{s+6}

Find the output *y*(*t*) due to the input 45*e* βˆ’3*t u*(*t*) and its impulse response. **Answer:** βˆ’90*e*<sup>βˆ’</sup>3*<sup>t</sup>* + 180*e*<sup>βˆ’</sup>6*<sup>t</sup>* , *t* β‰₯ 0, 2*Ξ΄*(*t*) βˆ’ 12*e*<sup>βˆ’</sup>6*<sup>t</sup> u*(*t*). The unit impulse response is the output response of a circuit when the input is a unit impulse. I 1 Example 16.8 Determine the transfer function *H*(*s*) = *Vo*(*s*)βˆ•*Io*(*s*) of the circuit in Fig. 16.18. # **Solution:** β–  **METHOD 1** By current division,

I_2 = \frac{(s+4)I_o}{s+4+2+1/2s}

But+β€’Vo2Ξ©4Ξ©s But + β€’ Vo 2 Ξ© 4 Ξ© s

V_o = 2I_2 = \frac{2(s+4)I_o}{s+6+1/2s}

Hence, Hence,

H(s) = \frac{V_o(s)}{I_o(s)} = \frac{4s(s+4)}{2s^2 + 12s + 1}

β– βˆ—βˆ—METHOD2βˆ—βˆ—Wecanapplytheladdermethod.Weletβˆ—Voβˆ—=1V.ByOhmβ€²slaw,βˆ—Iβˆ—2=βˆ—Voβˆ—βˆ•2=1βˆ•2A.Thevoltageacrossthe(2+1βˆ•2βˆ—sβˆ—)impedanceis β–  **METHOD 2** We can apply the ladder method. We let *Vo* = 1 V. By Ohm's law, *I*2 = *Vo*βˆ•2 = 1βˆ•2 A. The voltage across the (2 + 1βˆ•2*s*) impedance is

V_1 = I_2 \left( 2 + \frac{1}{2s} \right) = 1 + \frac{1}{4s} = \frac{4s + 1}{4s}

Thisisthesameasthevoltageacrossthe(βˆ—sβˆ—+4)impedance.Hence, This is the same as the voltage across the (*s* + 4) impedance. Hence,

I_1 = \frac{V_1}{s+4} = \frac{4s+1}{4s(s+4)}

ApplyingKCLatthetopnodeyields Applying KCL at the top node yields

I_o = I_1 + I_2 = \frac{4s + 1}{4s(s + 4)} + \frac{1}{2} = \frac{2s^2 + 12s + 1}{4s(s + 4)}

Hence, Hence,

H(s) = \frac{V_o}{I_o} = \frac{1}{I_o} = \frac{4s(s+4)}{2s^2 + 12s + 1}

asbefore.PracticeProblem16.8Findthetransferfunctionβˆ—Hβˆ—(βˆ—sβˆ—)=βˆ—Iβˆ—1(βˆ—sβˆ—)βˆ•βˆ—Ioβˆ—(βˆ—sβˆ—)inthecircuitofFig.16.18.Answer: as before. Practice Problem 16.8 Find the transfer function *H*(*s*) = *I*1(*s*)βˆ•*Io*(*s*) in the circuit of Fig. 16.18. Answer:

\frac{4s+1}{2s^2+12s+1}

. V(s) + β€’ **Figure 16.18** For Example 16.8. # **Solution:** (a) Using voltage division,

V_o = \frac{1}{s+1} V_{ab}

(16.9.1)But (16.9.1) But

V_{ab} = \frac{1|| (s+1)}{1+1|| (s+1)} V_i = \frac{(s+1)/(s+2)}{1+(s+1)/(s+2)} V_i

or or

V_{ab} = \frac{s+1}{2s+3} V_i

(16.9.2)SubstitutingEq.(16.9.2)intoEq.(16.9.1)resultsin (16.9.2) Substituting Eq. (16.9.2) into Eq. (16.9.1) results in

V_o = \frac{V_i}{2s + 3}

Thus,thetransferfunctionis Thus, the transfer function is

H(s) = \frac{V_o}{V_i} = \frac{1}{2s + 3}

(b)Wemaywriteβˆ—Hβˆ—(βˆ—sβˆ—)as (b) We may write *H*(*s*) as

H(s) = \frac{1}{2} \frac{1}{s + \frac{3}{2}}

ItsinverseLaplacetransformistherequiredimpulseresponse: Its inverse Laplace transform is the required impulse response:

h(t) = \frac{1}{2}e^{-3t/2}u(t)

(c)Whenβˆ—viβˆ—(βˆ—tβˆ—)=βˆ—uβˆ—(βˆ—tβˆ—),βˆ—Viβˆ—(βˆ—sβˆ—)=1βˆ•βˆ—sβˆ—,and (c) When *vi*(*t*) = *u*(*t*), *Vi*(*s*) = 1βˆ•*s*, and

V_o(s) = H(s)V_i(s) = \frac{1}{2s(s + \frac{3}{2})} = \frac{A}{s} + \frac{B}{s + \frac{3}{2}}

where where

A = sV_o(s)|{s=0} = \frac{1}{2(s + \frac{3}{2})}|{s=0} = \frac{1}{3}

B = \left(s + \frac{3}{2}\right) V_o(s)|{s=-3/2} = \frac{1}{2s}|{s=-3/2} = -\frac{1}{3}

Hence,forβˆ—viβˆ—(βˆ—tβˆ—)=βˆ—uβˆ—(βˆ—tβˆ—), Hence, for *vi*(*t*) = *u*(*t*),

V_o(s) = \frac{1}{3} \left( \frac{1}{s} - \frac{1}{s + \frac{3}{2}} \right)

anditsinverseLaplacetransformis and its inverse Laplace transform is

v_o(t) = \frac{1}{3}(1 - e^{-3t/2})u(t) \text{ V}

ForExample16.9.<spanid="pageβˆ’750βˆ’0"></span>(d)When For Example 16.9. <span id="page-750-0"></span>(d) When

v_i(t) = 8 \cos 2t

, then $V_i(s) = \frac{8s}{s^2 + 4}$ , and \n

V_o(s) = H(s)V_i(s) = \frac{4s}{(s + \frac{3}{2})(s^2 + 4)}

\n\n

= \frac{A}{s + \frac{3}{2}} + \frac{Bs + C}{s^2 + 4}

\n(16.9.3)where\n(16.9.3) where

A = \left(s + \frac{3}{2}\right) V_o(s) \Big|{s = -3/2} = \frac{4s}{s^2 + 4} \Big|{s = -3/2} = -\frac{24}{25}

Togetβˆ—Bβˆ—andβˆ—Cβˆ—,wemultiplyEq.(16.9.3)by(βˆ—sβˆ—+3βˆ•2)(βˆ—sβˆ—2+4).Weget To get *B* and *C*, we multiply Eq. (16.9.3) by (*s* + 3βˆ•2)(*s* 2 + 4). We get

4s = A(s^{2} + 4) + B(s^{2} + \frac{3}{2}s) + C(s + \frac{3}{2})

Equatingcoefficients,Constant: Equating coefficients, Constant:

0 = 4A + \frac{3}{2}C

$\Rightarrow$ $C = -\frac{8}{3}A$ \ns: $4 = \frac{3}{2}B + C$ \ns<sup>2</sup>: $0 = A + B$ $\Rightarrow$ $B = -A$ Solving these gives *A* = βˆ’24βˆ•25, *B* = 24βˆ•25, *C* = 64βˆ•25. Hence, for *vi*(*t*) = 8 cos 2*t* V,

V_o(s) = \frac{-\frac{24}{25}}{s + \frac{3}{2}} + \frac{24}{25} \frac{s}{s^2 + 4} + \frac{32}{25} \frac{2}{s^2 + 4}

anditsinverseis and its inverse is

v_o(t) = \frac{24}{25} \left( -e^{-3t/2} + \cos 2t + \frac{4}{3} \sin 2t \right) u(t) \text{ V}

βˆ—βˆ—Figure16.20βˆ—βˆ—βˆ—βˆ—Figure16.21βˆ—βˆ—Alinearsystemwithβˆ—mβˆ—inputsandβˆ—pβˆ—outputs.PracticeProblem16.9ReworkExample16.9forthecircuitshowninFig.16.20.βˆ—βˆ—Answer:βˆ—βˆ—(a) **Figure 16.20** **Figure 16.21** A linear system with *m* inputs and *p* outputs. Practice Problem 16.9 Rework Example 16.9 for the circuit shown in Fig. 16.20. **Answer:** (a)

2/(s + 4)

, (b) $2e^{-4t}u(t)$ , (c) $\frac{1}{2}(1 - e^{-4t})u(t)$ V, (d) $3.2(-e^{-4t} + \cos 2t + \frac{1}{2} \sin 2t)u(t)$ V.