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 \( 3.64 \times 10^{-13} \, \text{J} \).
Assertion (A): We cannot form a p-n junction diode by taking a slab of a p-type semiconductor and physically joining it to another slab of an n-type semiconductor.
Reason (R): In a p-type semiconductor, \( n_e \gg n_h \) while in an n-type semiconductor \( n_h \gg n_e \).
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: