From the graph, we can see that at \( t = 10 \times 10^3 \) s, the natural logarithm of the activity \( \ln R \) decreases from 2 to 1, which means the activity halves. This suggests the activity follows an exponential decay law of the form: \[ R = R_0 e^{-t/\tau} \] At \( t = 0 \), \( R_0 = N_0 \), which is the number of undecayed nuclei. From the graph, we are given that \( \ln R = 2 \) at \( t = 0 \), and \( \ln R = 1 \) at \( t = 10 \times 10^3 \) s. This gives us the relation: \[ \ln \left( \frac{R_0}{2} \right) = 1 \] Therefore, \[ \ln R_0 = 1 + \ln 2 \] Using \( \ln 2 \approx 0.693 \), we get: \[ \ln R_0 = 1.693 \] Exponentiating both sides: \[ R_0 = e^{1.693} = 75,000 \] Thus, \( N_0 = 75,000 \).
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is:
The velocity-time graph of an object moving along a straight line is shown in the figure. What is the distance covered by the object between \( t = 0 \) to \( t = 4s \)?