a) TO solve the problem we need to apply the conservation of angular momentum,
[tex]mR^{2}\omega_b + I\omega_t=0,[/tex]
where,
I is the moment of inertia for the turntable, which is
m= the mass of the beetle
M= mass of the turntable
clearing [tex]\omega_t[/tex],
[tex]\omega_t=-\frac{mR^2w_b}{I}[/tex]
We know that [tex]I= 1/2MR^2[/tex]. So,
Making a reference and asking where is the beetle we can see that it is on the turntale.
Therefore [tex]\omega = 0.0700 - 0.02210 = + 0.0579rad/s[/tex]
b) As we have seen in part a, it is [tex]-0.02210rad/s[/tex]
c) The angular velocity of the beetle is RELATIVE TO THE TURNTABLE, That is
[tex]T=\frac{2\pi}{\omega}=\frac{2\pi}{0.7}= 89.76s[/tex]