To solve this problem we will use the kinematic equations of angular motion, starting from the definition of angular velocity in terms of frequency, to verify the angular displacement and its respective derivative, let's start:
[tex]\omega = 2\pi f[/tex]
[tex]\omega = 2\pi (2.5)[/tex]
[tex]\omega = 5\pi rad/s[/tex]
The angular displacement is given as the form:
[tex]\theta (t) = \theta_0 cos(\omega t)[/tex]
In the equlibrium we have to [tex]t=0, \theta(t) = \theta_0[/tex] and in the given position we have to
[tex]\theta(t) = \theta_0 cos(5\pi t)[/tex]
Derived the expression we will have the equivalent to angular velocity
[tex]\frac{d\theta}{dt} = 2.7rad/s[/tex]
Replacing,
[tex]\theta_0(sin(5\pi t))5\pi = 2.7[/tex]
Finally
[tex]\theta_0 = \frac{2.7}{5\pi}rad = 9.848\°[/tex]
Therefore the maximum angular displacement is 9.848°