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R-H root distribution of s⁶+2s⁵+8s⁴+12s³+20s²+16s+16

Short answer

Routh array shows no sign changes, so zero roots in RHP. An all-zero s³ row gives an auxiliary equation whose solution yields four jω-axis roots (±j1.414, ±j2). Factoring out leaves s²+2s+2 giving two LHP roots at −1±j1. Thus, RHP=0, LHP=2, jω axis=4.

Using R-H criteria, tell how many roots of polynomial are in right half s-plane, in left half s-plane and on jω axis. s⁶ + 2s⁵ + 8s⁴ + 12s³ + 20s² + 16s + 16 = 0

Result: RHP = 0, LHP = 2, jωj\omega axis = 4. The system is marginally stable.

By the Routh–Hurwitz criterion, the number of sign changes in the first column equals the number of RHP roots. A zero row shows roots symmetric about the origin, which are found from the auxiliary equation.

s6+2s5+8s4+12s3+20s2+16s+16=0s^6 + 2s^5 + 8s^4 + 12s^3 + 20s^2 + 16s + 16 = 0

Routh array

RowCol 1Col 2Col 3Col 4
s6s^6182016
s5s^5212160
s4s^42(8)−1(12)2=2\frac{2(8)-1(12)}{2}=22(20)−1(16)2=12\frac{2(20)-1(16)}{2}=1216
s3s^32(12)−2(12)2=0\frac{2(12)-2(12)}{2}=02(16)−2(16)2=0\frac{2(16)-2(16)}{2}=0

The s3s^3 row is all zeros, so there are roots placed symmetrically about the origin. Auxiliary equation from the s4s^4 row:

A(s)=2s4+12s2+16,dAds=8s3+24sA(s) = 2s^4 + 12s^2 + 16, \qquad \frac{dA}{ds} = 8s^3 + 24s
RowCol 1Col 2
s3s^3824
s2s^28(12)−2(24)8=6\frac{8(12)-2(24)}{8}=68(16)−08=16\frac{8(16)-0}{8}=16
s1s^16(24)−8(16)6=2.67\frac{6(24)-8(16)}{6}=2.670
s0s^016

First column: 1, 2, 2, 8, 6, 2.67, 161,\ 2,\ 2,\ 8,\ 6,\ 2.67,\ 16. No sign change, so no root is in the RHP.

Roots of the auxiliary equation

2s4+12s2+16=2(s2+2)(s2+4)=0s=±j1.414, ±j2\begin{aligned} 2s^4+12s^2+16 &= 2(s^2+2)(s^2+4) = 0 \\ s &= \pm j1.414,\ \pm j2 \end{aligned}

These four roots lie on the jωj\omega axis and are not repeated. The other factor is

s6+2s5+8s4+12s3+20s2+16s+16(s2+2)(s2+4)=s2+2s+2  ⇒  s=−1±j1\frac{s^6+2s^5+8s^4+12s^3+20s^2+16s+16}{(s^2+2)(s^2+4)} = s^2+2s+2 \;\Rightarrow\; s = -1\pm j1
RegionNumberRoots
Right half plane0none
jωj\omega axis4±j1.414\pm j1.414, ±j2\pm j2
Left half plane2−1±j1-1\pm j1

The jωj\omega-axis roots are simple, so the system is marginally stable: it oscillates at 1.414 rad/s and 2 rad/s.

✓ Answer checked by Claude Opus 5.5 (high effort)

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