To solve this problem it is necessary to apply the concepts related to the elastic potential energy from the simple harmonic movement.
Said mechanical energy can be expressed as
![E = (1)/(2) kA^2](https://img.qammunity.org/2020/formulas/physics/college/18med01pcitertt8hqhffa9mn43t3128zp.png)
Where,
k = Spring Constant
A = Cross-sectional Area
From the angular movement we can relate the angular velocity as a function of the spring constant and the mass in order to find this variable:
![\omega^2 = (k)/(m)](https://img.qammunity.org/2020/formulas/physics/high-school/k55focw3mh8g37v4dhbsfiq6gdbb1fwchv.png)
for f equal to the frequency.
![k = 1.53(2\pi 1.95)^2](https://img.qammunity.org/2020/formulas/physics/college/e3zp0zcpc8m3lrvjkk1igyxgf5e4u9x6c9.png)
![k = 229.44](https://img.qammunity.org/2020/formulas/physics/college/tpj8gu2j9onoz6fdgexqi3dmyaw3137ecf.png)
Finally the energy released would be
![E = (1)/(2) (229.44)(0.075)^2](https://img.qammunity.org/2020/formulas/physics/college/x4k94wuotmfba9geivx82jurfb42crfku1.png)
![E = 0.6453J \approx 0.646J](https://img.qammunity.org/2020/formulas/physics/college/5psypljar7p9wq5d54k56a78za1ola848f.png)
Therefore the correct answer is B.