\(G\left( s \right) = \frac{1}{{\left( {s + 1} \right)\left( {s + 2} \right)}}\)
\(H\left( s \right) = \frac{{s + \alpha }}{s}\)
1 + G(s) H(s) = 0
\(\Rightarrow 1 + \frac{1}{{\left( {s + 1} \right)\left( {s + 2} \right)}}.\frac{{s + \alpha }}{s} = 0\)
⇒ s3 + 3s2 + 2s + s + α = 0
⇒ s3 + 3s2 + 3s + α = 0
\(\begin{array}{*{20}{c}} {{s^3}}\\ {{s^2}}\\ {\begin{array}{*{20}{c}} {{s^1}}\\ {s^\circ } \end{array}} \end{array}\begin{array}{*{20}{c}} 1&3&0\\ 3&\alpha &0\\ {\begin{array}{*{20}{c}} {\frac{{9 - \alpha }}{3}}\\ \alpha \end{array}}&{\begin{array}{*{20}{c}} 0\\ 0 \end{array}}&{\begin{array}{*{20}{c}} 0\\ 0 \end{array}} \end{array}\)
Closed loop poles will be on the imaginary axis if any row in Routh’s array became zero.
for \(\frac{{9 - \alpha }}{3} = 0\), the s1 row will become zero.
⇒ 9 – α = 0 ⇒ α = 9.