Step 1: Understanding the decay process. Radioactive decay follows the equation: \[ N = N_0 \times \left( \frac{1}{2} \right)^n \] Where \( N_0 \) is the initial number of nuclei, \( N \) is the number of nuclei left after \( n \) half-lives, and \( n \) is the number of half-lives elapsed. If \( \frac{7}{8} \) of the substance has disintegrated, then \( \frac{1}{8} \) of the substance remains. This means the number of remaining radioactive nuclei is \( \frac{N_0}{8} \).
Step 2: Finding the number of half-lives. Using the decay equation: \[ \frac{N_0}{2^n} = \frac{N_0}{8} \] Simplifying: \[ 2^n = 8 \] \[ n = 3 \] So, 3 half-lives have elapsed.
Step 3: Calculating the time. Since the half-life is \( T \), the time taken for the disintegration of \( \frac{7}{8} \) of the substance is: \[ \text{Time} = 3 \times T = 3T \]
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,



Find the value of m if \(M = 10\) \(kg\). All the surfaces are rough.
As per the given figure, a small ball $P$ slides down the quadrant of a circle and hits the other ball $Q$ of equal mass which is initially at rest Neglecting the effect of friction and assume the collision to be elastic, the velocity of ball $Q$ after collision will be :$\left( g =10 \,m / s ^2\right)$
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)