Given: The number of radioactive nuclei \( N(t) \) at a given time \( t \) is given by:
\(N(t) = N_0 \times \exp(-\lambda t)\)
The activity \( A \) of a radioactive source is defined as the rate of decay, which is the derivative of the number of radioactive nuclei with respect to time:
\(A = - \frac{dN}{dt} = \lambda \times N(t)\)
Given that the activities of sources \( S_1 \) and \( S_2 \) are \( A_1 \) and \( A_2 \), respectively, we can write:
\(A_1 = \lambda_1 \times N_1(t)\)
\(A_2 = \lambda_2 \times N_2(t)\)
After the completion of the 3rd half-life for source \( S_1 \), the remaining number of radioactive nuclei is:
\(N_1(t) = N_0 \times \left( \frac{1}{2} \right)^3 = N_0 \times \frac{1}{8}\)
Similarly, after the completion of the 7th half-life for source \( S_2 \), the remaining number of radioactive nuclei is:
\(N_2(t) = N_0 \times \left( \frac{1}{2} \right)^7 = N_0 \times \frac{1}{128}\)
Now, let's substitute these values into the equations for activities \( A_1 \) and \( A_2 \):
\(A_1 = \lambda_1 \times N_0 \times \left( \frac{1}{8} \right)\)
\(A_2 = \lambda_2 \times N_0 \times \left( \frac{1}{128} \right)\)
To find the ratio \( \frac{A_1}{A_2} \), we can simplify:
\(\frac{A_1}{A_2} = \frac{\lambda_1}{\lambda_2} \times \left( \frac{1}{8} \right) \times \left( \frac{128}{1} \right)\)
Since both sources have the same activity at time \( t = 0 \), we can assume their decay constants are the same (\( \lambda_1 = \lambda_2 \)). Therefore, the ratio simplifies to:
\(\frac{A_1}{A_2} = \frac{1}{8} \times \frac{128}{1} = \frac{128}{8} = 16\)
Thus, the ratio \( \frac{A_1}{A_2} \) is 16.
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is:
Nuclear physics is the field of physics that studies atomic nuclei and their constituents and interactions, in addition to the study of other forms of nuclear matter. Nuclear physics should not be confused with atomic physics, which studies the atom as a whole, including its electrons
βRβ represents the radius of the nucleus. R = RoA1/3
Where,
The mass number (A), also known as the nucleon number, is the total number of neutrons and protons in a nucleus.
A = Z + N
Where, N is the neutron number, A is the mass number, Z is the proton number
Mass defect is the difference between the sum of masses of the nucleons (neutrons + protons) constituting a nucleus and the rest mass of the nucleus and is given as:
Ξm = Zmp + (A - Z) mn - M
Where Z = atomic number, A = mass number, mp = mass of 1 proton, mn = mass of 1 neutron and M = mass of nucleus.