Correct Answer - Option 2 : ω = 3 rad/sec
\(\;\sin \omega t \to \boxed{G\left( s \right)} \to Y\left( s \right) = \left| {G\left( s \right)} \right| \cdot \sin \left( {\omega t + \angle G\left( s \right)} \right)\)
Output will be zero when
|G(s)| = 0
Put s = jω
\(\left| {\frac{{\left( { - {\omega ^2} + 9} \right)\left( {j\omega + 2} \right)}}{{\left( {j\omega + 1} \right)\left( {j\omega + 3} \right)\left( {j\omega + 4} \right)}}} \right| = 0\)
at ω = 3 , |G(jω)| = 0