The half-life (\(t_{1/2}\)) of a radioactive nuclide is related to the decay constant (\(\lambda\)) by the following formula:
\[ t_{1/2} = \frac{\ln(2)}{\lambda} \]
Where:
Given that the decay constant \( \lambda = 6.93 \, \text{s}^{-1} \), we can substitute this value into the formula:
\[ t_{1/2} = \frac{0.693}{6.93} \]
Now, performing the division:
\[ t_{1/2} \approx 0.1 \, \text{seconds} \]
The half-life of the nuclide is approximately \( \boxed{0.1} \) seconds.
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: