The number of radioactive nuclei N(t) at a given time t is given by:
N(t) = N0 \(\times\)exp(-λt)
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 = -\(\frac {dN}{dt}\) = λ\(\times\) N(t)
Given that the activities of sources S1 and S2 are A1 and A2, respectively, we can write:
A1 = λ1 \(\times\) N1(t)
A2 = λ2 \(\times\) N2(t)
After the completion of the 3rd half-life for source S1, the remaining number of radioactive nuclei is:
N1(t) = N0 \(\times\) (\(\frac{1}{2}\))3 = N0 \(\times\) \(\frac {1}{8}\)
Similarly, after the completion of the 7th half-life for source S2, the remaining number of radioactive nuclei is:
N2(t) = N0 \(\times\) \([\frac{1}{2}]\)7 = N0 \(\times\) \(\frac {1}{128}\)
Now, let's substitute these values into the equations for activities A1 and A2 :
A1 = λ1 \(\times\) N0 \(\times\) (\(\frac {1}{8}\))
A2 = λ2 \(\times\) N0 \(\times\) (\(\frac {1}{128}\))
To find the ratio \(\frac{A_1}{A_2}\), we can simplify:
(\(\frac{A_1}{A_2}\)) = (\(\frac{\lambda_1}{\lambda_2}\)) \(\times\) (\(\frac {1}{8}\) ) \(\times\) (\(\frac {128}{1}\))
Since both sources have the same activity at time t = 0, we can assume their decay constants are the same (λ1 = λ2). Therefore, the ratio simplifies to:
(\(\frac{A_1}{A_2}\)) = \(\frac {1}{8}\) \(\times\) \(\frac {128}{1}\) = \(\frac {128}{8}\) = 16
Therefore, the ratio \(\frac{A_1}{A_2}\) is 16.
So, the answer is \(16\).
Given
S1 has just completed its 3rd half-life.
S2 has just completed its 7th half-life.
Initially, both sources have the same activity, \(A(0) = \lambda N_0\)
Calculating Activities After Given Half-Lives:
For S1 after 3 half-lives:
\(N_1 = N_0 \left( \frac{1}{2} \right)^3 = N_0 \left( \frac{1}{8} \right) = \frac{N_0}{8}\)
Hence, the activity A1A_1A1 at this time is:
\(A_1 = \lambda N_1 = \lambda \left( \frac{N_0}{8} \right) = \frac{\lambda N_0}{8}\)
For S2 after 7 half-lives:
\(N_2 = N_0 \left( \frac{1}{2} \right)^7 = N_0 \left( \frac{1}{128} \right) = \frac{N_0}{128}\)
Hence, the activity A2 at this time is:
\(A_2 = \lambda N_2 = \lambda \left( \frac{N_0}{128} \right) = \frac{\lambda N_0}{128}\)
Calculating the Ratio of Activities:
The ratio \(\frac{A_1}{A_2}\) is:
\(\frac{A_1}{A_2} = \frac{\frac{\lambda N_0}{8}}{\frac{\lambda N_0}{128}} = \frac{\frac{1}{8}}{\frac{1}{128}} = \frac{128}{8} = 16\)
So, the answer is 16.
List-I shows various functional dependencies of energy $ E $ on the atomic number $ Z $. Energies associated with certain phenomena are given in List-II. Choose the option that describes the correct match between the entries in List-I to those in List-II.
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
Figure 1 shows the configuration of main scale and Vernier scale before measurement. Fig. 2 shows the configuration corresponding to the measurement of diameter $ D $ of a tube. The measured value of $ D $ is:
A solid glass sphere of refractive index $ n = \sqrt{3} $ and radius $ R $ contains a spherical air cavity of radius $ \dfrac{R}{2} $, as shown in the figure. A very thin glass layer is present at the point $ O $ so that the air cavity (refractive index $ n = 1 $) remains inside the glass sphere. An unpolarized, unidirectional and monochromatic light source $ S $ emits a light ray from a point inside the glass sphere towards the periphery of the glass sphere. If the light is reflected from the point $ O $ and is fully polarized, then the angle of incidence at the inner surface of the glass sphere is $ \theta $. The value of $ \sin \theta $ 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
‘R’ 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:
Δm = 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.