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.
Match the LIST-I with LIST-II
LIST-I (Type of decay in Radioactivity) | LIST-II (Reason for stability) | ||
---|---|---|---|
A. | Alpha decay | III. | Nucleus is mostly heavier than Pb (Z=82) |
B. | Beta negative decay | IV. | Nucleus has too many neutrons relative to the number of protons |
C. | Gamma decay | I. | Nucleus has excess energy in an excited state |
D. | Positron Emission | II. | Nucleus has too many protons relative to the number of neutrons |
Choose the correct answer from the options given below:
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): The density of the copper ($^{64}Cu$) nucleus is greater than that of the carbon ($^{12}C$) nucleus.
Reason (R): The nucleus of mass number A has a radius proportional to $A^{1/3}$.
In the light of the above statements, choose the most appropriate answer from the options given below:
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ 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.