To solve this problem we will apply the kinematic equations of the simple harmonic movement, for which the angular velocity is expressed as a function of the square root of the spring constant and the mass. From the angular velocity it will be possible to find the frequency and finally the period - which is the inverse of the latter.
Mathematically the expression of angular movement for a spring satisfies equality:
[tex]\omega = \sqrt{\frac{k}{m}}[/tex]
Where,
k = Spring constant
m = Mass
Then the angular frequency is
[tex]\omega = \sqrt{\frac{65}{0.680}}[/tex]
[tex]\omega = 9.7769rad/s[/tex]
Now the frequency is defined as the ratio of change between the angular frequency and the constant 2π, that is
[tex]f = \frac{\omega}{2\pi}[/tex]
[tex]f = \frac{9.7769}{2\pi}[/tex]
[tex]f = 1.55604 Hz[/tex]
The period is the inverse of the frequency, therefore
[tex]T = \frac{1}{f}[/tex]
[tex]T = \frac{1}{1.55604}[/tex]
[tex]T= 0.6426s[/tex]