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154 CHAPTER 2 TIME-DOMAIN ANALYSIS OF CONTINUOUS-TIME SYSTEMS

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154 CHAPTER 2 TIME-DOMAIN ANALYSIS OF CONTINUOUS-TIME SYSTEMS

In this case the root Ξ» repeats twice. Observe that the characteristic modes in this case are eΞ»*t* and teΞ»*t* . Continuing this pattern, we can show that for the differential equation

(Dβˆ’Ξ»)ry0(t)=0(D - \lambda)^r y_0(t) = 0

the characteristic modes are eΞ»*t* , teΞ»*t* , t 2eΞ»*t* , …, t rβˆ’1eΞ»*t* , and that the solution is

y0(t)=(c1+c2t+β‹―+crtrβˆ’1)eΞ»ty_0(t) = (c_1 + c_2t + \dots + c_rt^{r-1})e^{\lambda t}

Consequently, for a system with the characteristic polynomial

Q(Ξ»)=(Ξ»βˆ’Ξ»1)r(Ξ»βˆ’Ξ»r+1)β‹―(Ξ»βˆ’Ξ»N)Q(\lambda) = (\lambda - \lambda_1)^r (\lambda - \lambda_{r+1}) \cdots (\lambda - \lambda_N)

the characteristic modes are eΞ»1*t* , teΞ»1*t* , …, t rβˆ’1eΞ»1*t* , eΞ»r+1*t* , …, eΞ»Nt and the solution is

y0(t)=(c1+c2t+β‹―+crtrβˆ’1)eΞ»1t+cr+1eΞ»r+1t+β‹―+cNeΞ»Nty_0(t) = (c_1 + c_2t + \dots + c_rt^{r-1})e^{\lambda_1 t} + c_{r+1}e^{\lambda_{r+1} t} + \dots + c_N e^{\lambda_N t}

COMPLEX ROOTS

The procedure for handling complex roots is the same as that for real roots. For complex roots, the usual procedure leads to complex characteristic modes and the complex form of solution. However, it is possible to avoid the complex form altogether by selecting a real-form of solution, as described next.

For a real system, complex roots must occur in pairs of conjugates if the coefficients of the characteristic polynomial Q(Ξ») are to be real. Therefore, if Ξ± + jΞ² is a characteristic root, Ξ± βˆ’ jΞ² must also be a characteristic root. The zero-input response corresponding to this pair of complex conjugate roots is

y0(t)=c1e(Ξ±+jΞ²)t+c2e(Ξ±βˆ’jΞ²)ty_0(t) = c_1 e^{(\alpha + j\beta)t} + c_2 e^{(\alpha - j\beta)t}

\n(2.7)

For a real system, the response y0(t) must also be real. This is possible only if c1 and c2 are conjugates. Let

c1=c2ejΞΈandc2=c2eβˆ’jΞΈc_1 = \frac{c}{2}e^{j\theta} \qquad \text{and} \qquad c_2 = \frac{c}{2}e^{-j\theta}

This yields

y0(t)=c2eiΞΈe(Ξ±+jΞ²)t+c2eβˆ’jΞΈe(Ξ±βˆ’jΞ²)ty_0(t) = \frac{c}{2}e^{i\theta}e^{(\alpha+j\beta)t} + \frac{c}{2}e^{-j\theta}e^{(\alpha-j\beta)t}

=

c2eΞ±t[ei(Ξ²t+ΞΈ)+eβˆ’j(Ξ²t+ΞΈ)]\frac{c}{2}e^{\alpha t}[e^{i(\beta t + \theta)} + e^{-j(\beta t + \theta)}]

=

ceαtcos⁑(βt+θ)ce^{\alpha t}\cos(\beta t + \theta)

(2.8)

Therefore, the zero-input response corresponding to complex conjugate roots Ξ± Β± jΞ² can be expressed in a complex form [Eq. (2.7)] or a real form [Eq. (2.8)].

EXAMPLE 2.1 Finding the Zero-Input Response

Find y0(t), the zero-input response of the response for an LTIC system described by

  • (a) the simple-root system (D2 + 3D + 2)y(t) = Dx(t) with initial conditions y0(0) = 0 and yΛ™0(0) = βˆ’5.
  • (b) the repeated-root system (D2 + 6D + 9)y(t) = (3D + 5)x(t) with initial conditions y0(0) = 3 and yΛ™0(0) = βˆ’7.
  • (c) the complex-root system (D2 + 4D + 40)y(t) = (D + 2)x(t) with initial conditions y0(0) = 2 and yΛ™0(0) = 16.78.

(a) Note that y0(t), being the zero-input response (x(t) = 0), is the solution of (D2 +3D+ 2)y0(t) = 0. The characteristic polynomial of the system is Ξ»2 + 3Ξ» + 2. The characteristic equation of the system is therefore Ξ»2 + 3Ξ» + 2 = (Ξ» + 1)(Ξ» + 2) = 0. The characteristic roots of the system are Ξ»1 = βˆ’1 and Ξ»2 = βˆ’2, and the characteristic modes of the system are eβˆ’t and eβˆ’2*t* . Consequently, the zero-input response is

y0(t)=c1eβˆ’t+c2eβˆ’2ty_0(t) = c_1 e^{-t} + c_2 e^{-2t}

Differentiating this expression, we obtain

yΛ™0(t)=βˆ’c1eβˆ’tβˆ’2c2eβˆ’2t\dot{y}_0(t) = -c_1 e^{-t} - 2c_2 e^{-2t}

To determine the constants c1 and c2, we set t = 0 in the equations for y0(t) and yΛ™0(t) and substitute the initial conditions y0(0) = 0 and yΛ™0(0) = βˆ’5, yielding

0=c1+c20 = c_1 + c_2 βˆ’5=βˆ’c1βˆ’2c2-5 = -c_1 - 2c_2

Solving these two simultaneous equations in two unknowns for c1 and c2 yields

c1=βˆ’5andc2=5c_1 = -5 \qquad \text{and} \qquad c_2 = 5

Therefore,

y0(t)=βˆ’5eβˆ’t+5eβˆ’2ty_0(t) = -5e^{-t} + 5e^{-2t}

(2.9)

This is the zero-input response of y(t). Because y0(t) is present at t = 0βˆ’, we are justified in assuming that it exists for t β‰₯ 0.†

(b) The characteristic polynomial is Ξ»2 + 6Ξ» + 9 = (Ξ» + 3)2, and its characteristic roots are Ξ»1 = βˆ’3, Ξ»2 = βˆ’3 (repeated roots). Consequently, the characteristic modes of the system are eβˆ’3*t* and teβˆ’3*t* . The zero-input response, being a linear combination of the characteristic modes, is given by

y0(t)=(c1+c2t)eβˆ’3ty_0(t) = (c_1 + c_2 t)e^{-3t}

† *y*0(t) may be present even before t = 0βˆ’. However, we can be sure of its presence only from t = 0βˆ’ onward.

We can find the arbitrary constants c1 and c2 from the initial conditions y0(0) = 3 and yΛ™0(0) = βˆ’7 following the procedure in part (a). The reader can show that c1 = 3 and c2 = 2. Hence,

y0(t)=(3+2t)eβˆ’3ttβ‰₯0y_0(t) = (3+2t)e^{-3t} \qquad t \ge 0

(c) The characteristic polynomial is Ξ»2 + 4Ξ» + 40 = (Ξ» + 2 βˆ’ j6)(Ξ» + 2 + j6). The characteristic roots are βˆ’2 Β± j6.† The solution can be written either in the complex form [Eq. (2.7)] or in the real form [Eq. (2.8)]. The complex form is y0(t) = c1eΞ»1*t* + c2eΞ»2*t* , where Ξ»1 = βˆ’2+j6 and Ξ»2 = βˆ’2βˆ’j6. Since Ξ± = βˆ’2 and Ξ² =6, the real-form solution is [see Eq. (2.8)]

y0(t)=ceβˆ’2tcos⁑(6t+ΞΈ)y_0(t) = ce^{-2t}\cos(6t+\theta)

Differentiating this expression, we obtain

yΛ™0(t)=βˆ’2ceβˆ’2tcos⁑(6t+ΞΈ)βˆ’6ceβˆ’2tsin⁑(6t+ΞΈ)\dot{y}_0(t) = -2ce^{-2t}\cos{(6t + \theta)} - 6ce^{-2t}\sin{(6t + \theta)}

To determine the constants c and ΞΈ, we set t = 0 in the equations for y0(t) and yΛ™0(t) and substitute the initial conditions y0(0) = 2 and yΛ™0(0) = 16.78, yielding

2=ccos⁑θ2 = c \cos \theta

16.78 = βˆ’2ccosβ‘ΞΈβˆ’6csin⁑θ-2c \cos \theta - 6c \sin \theta

Solution of these two simultaneous equations in two unknowns ccos ΞΈ and csinΞΈ yields

ccos ΞΈ = 2 and csinΞΈ = βˆ’3.463

Squaring and then adding these two equations yield

c2=(2)2+(βˆ’3.464)2=16⟹c=4c^{2} = (2)^{2} + (-3.464)^{2} = 16 \Longrightarrow c = 4

Next, dividing csinΞΈ = βˆ’3.463 by ccos ΞΈ = 2 yields

tan⁑θ=βˆ’3.4632\tan \theta = \frac{-3.463}{2}

and

ΞΈ=tanβ‘βˆ’1(βˆ’3.4632)=βˆ’Ο€3\theta = \tan^{-1} \left( \frac{-3.463}{2} \right) = -\frac{\pi}{3}

Therefore,

y0(t)=4eβˆ’2tcos⁑(6tβˆ’Ο€3)y_0(t) = 4e^{-2t}\cos\left(6t - \frac{\pi}{3}\right)

For the plot of y0(t), refer again to Fig. B.11c.

Ξ»2+4Ξ»+40=(Ξ»2+4Ξ»+4)+36=(Ξ»+2)2+(6)2=(Ξ»+2βˆ’j6)(Ξ»+2+j6)\lambda^2 + 4\lambda + 40 = (\lambda^2 + 4\lambda + 4) + 36 = (\lambda + 2)^2 + (6)^2 = (\lambda + 2 - j6)(\lambda + 2 + j6)

† The complex conjugate roots of a second-order polynomial can be determined by using the formula in Sec. B.8-10 or by expressing the polynomial as a sum of two squares. The latter can be accomplished by completing the square with the first two terms, as follows:

EXAMPLE 2.2 Using MATLAB to Find Polynomial Roots

Find the roots Ξ»1 and Ξ»2 of the polynomial Ξ»2 + 4Ξ» + k for three values of k: (a) k = 3, (b) k = 4, and (c) k = 40.

(a) >> r = roots([1 4 3]).’ r = -3 -1 For k = 3, the polynomial roots are therefore Ξ»1 = βˆ’3 and Ξ»2 = βˆ’1. (b) >> r = roots([1 4 4]).’ r = -2 -2 For k = 4, the polynomial roots are therefore Ξ»1 = Ξ»2 = βˆ’2. (c) >> r = roots([1 4 40]).’ r = -2.00+6.00i -2.00-6.00i For k = 40, the polynomial roots are therefore Ξ»1 = βˆ’2+j6 and Ξ»2 = βˆ’2βˆ’j6.

EXAMPLE 2.3 Using MATLAB to Find the Zero-Input Response

Consider an LTIC system specified by the differential equation

(D2+4D+k)y(t)=(3D+5)x(t)(D^2 + 4D + k)y(t) = (3D + 5)x(t)

Using initial conditions y0(0) = 3 and yΛ™0(0) = βˆ’7, apply MATLAB’s dsolve command to determine the zero-input response when: (a) k = 3, (b) k = 4, and (c) k = 40.