a) TO solve the problem we need to apply the conservation of angular momentum,
![mR^(2)\omega_b + I\omega_t=0,](https://img.qammunity.org/2020/formulas/physics/college/rw4d0r88uokkhytyqfi42m8wpe7tg59f9l.png)
where,
I is the moment of inertia for the turntable, which is
m= the mass of the beetle
M= mass of the turntable
clearing
,
![\omega_t=-(mR^2w_b)/(I)](https://img.qammunity.org/2020/formulas/physics/college/44049hi4enq2jqbg99g7jxk01xkqz7dqxm.png)
We know that
. So,
Making a reference and asking where is the beetle we can see that it is on the turntale.
Therefore
![\omega = 0.0700 - 0.02210 = + 0.0579rad/s](https://img.qammunity.org/2020/formulas/physics/college/pyf6kjlfhawdu5zsbbggkjpep3fts4gxyo.png)
b) As we have seen in part a, it is
![-0.02210rad/s](https://img.qammunity.org/2020/formulas/physics/college/umj6yk8vfri4eyxbwocv74m7nittvi1usw.png)
c) The angular velocity of the beetle is RELATIVE TO THE TURNTABLE, That is
![T=(2\pi)/(\omega)=(2\pi)/(0.7)= 89.76s](https://img.qammunity.org/2020/formulas/physics/college/spq37cab2eaemak4s6avuijs7e623ym9h3.png)