When an alpha particle collides head-on with a gold nucleus, the potential energy at the closest approach can be calculated using Coulomb’s law. The total energy at the closest approach is purely electrostatic potential energy because the kinetic energy of the alpha particle becomes zero at the point of closest approach.
The potential energy at the closest approach, \( U \), is given by the formula: \[ U = \frac{k_e \cdot Z_1 \cdot Z_2 \cdot e^2}{r} \] Where: - \( k_e = 9 \times 10^9 \, \text{Nm}^2/\text{C}^2 \) (Coulomb constant), - \( Z_1 = 2 \) (charge of the alpha particle), - \( Z_2 = 79 \) (charge of the gold nucleus), - \( e = 1.6 \times 10^{-19} \, \text{C} \) (elementary charge), - \( r = 10 \times 10^{-14} \, \text{m} \) (closest approach). Now, substitute the values into the equation: \[ U = \frac{(9 \times 10^9) \times (2) \times (79) \times (1.6 \times 10^{-19})^2}{10 \times 10^{-14}} \] Simplifying: \[ U = \frac{9 \times 10^9 \times 2 \times 79 \times (2.56 \times 10^{-38})}{10 \times 10^{-14}} = 3.64 \times 10^{-13} \, \text{J} \] Thus, the kinetic energy of the alpha particle is \( 3.64 \times 10^{-13} \, \text{J} \).
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:
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: