Suppose that an alpha particle of 4.50 MeV approaches head-on a uranium nucleus (Z = 92). Assuming that the uranium nucleus remains at rest and the alpha particle momentarily comes to rest and reverses its direction at a distance much more than the radius of the uranium nucleus, the distance of its closest approach is close to:
59 fm
This problem involves the concept of conservation of energy during a head-on collision between an alpha particle and a uranium nucleus. In such a scenario, the initial kinetic energy of the alpha particle is converted entirely into electrostatic potential energy at the point of closest approach, where the alpha particle momentarily comes to rest before reversing its direction.
The fundamental principle governing this interaction is the conservation of energy. As the alpha particle approaches the positively charged uranium nucleus, the electrostatic repulsive force causes it to slow down. At the distance of closest approach ($r_{min}$), all of its initial kinetic energy ($K$) is transformed into electrostatic potential energy ($U$).
Mathematically, this can be expressed as:
$$K_{initial} = U_{final}$$
Where:
Let's list the given values and necessary physical constants:
First, we convert the kinetic energy of the alpha particle from Mega-electron Volts (MeV) to Joules (J):
$$K = 4.50 \text{ MeV}$$
$$K = 4.50 \times 10^6 \text{ eV}$$
$$K = 4.50 \times 10^6 \times (1.6 \times 10^{-19} \text{ J})$$
$$K = 7.2 \times 10^{-13} \text{ J}$$
Next, we write the charges of the alpha particle and uranium nucleus in Coulombs:
The electrostatic potential energy ($U$) between two point charges $q_1$ and $q_2$ separated by a distance $r$ is given by:
$$U = k \frac{q_1 q_2}{r}$$
At the distance of closest approach ($r_{min}$), $K = U$. So, we have:
$$K = k \frac{q_1 q_2}{r_{min}}$$
Rearranging the equation to solve for $r_{min}$:
$$r_{min} = k \frac{q_1 q_2}{K}$$
Now, we substitute the calculated values into the equation for $r_{min}$:
$$r_{min} = (9 \times 10^9 \text{ N m}^2/\text{C}^2) \times \frac{(3.2 \times 10^{-19} \text{ C}) \times (1.472 \times 10^{-17} \text{ C})}{7.2 \times 10^{-13} \text{ J}}$$
$$r_{min} = \frac{9 \times 10^9 \times 3.2 \times 10^{-19} \times 1.472 \times 10^{-17}}{7.2 \times 10^{-13}} \text{ m}$$
$$r_{min} = \frac{4.23936 \times 10^{-26}}{7.2 \times 10^{-13}} \text{ m}$$
$$r_{min} = 5.888 \times 10^{-14} \text{ m}$$
Since nuclear distances are typically expressed in femtometers (fm), where $1 \text{ fm} = 10^{-15} \text{ m}$, we convert our result:
$$r_{min} = 5.888 \times 10^{-14} \text{ m} = 58.88 \times 10^{-15} \text{ m}$$
$$r_{min} \approx 59 \text{ fm}$$
| Parameter | Value (SI Units) |
|---|---|
| Initial Kinetic Energy ($K$) | $7.2 \times 10^{-13} \text{ J}$ |
| Alpha Particle Charge ($q_1$) | $3.2 \times 10^{-19} \text{ C}$ |
| Uranium Nucleus Charge ($q_2$) | $1.472 \times 10^{-17} \text{ C}$ |
| Coulomb's Constant ($k$) | $9 \times 10^9 \text{ N m}^2/\text{C}^2$ |
| Distance of Closest Approach ($r_{min}$) | $5.888 \times 10^{-14} \text{ m}$ or $59 \text{ fm}$ |
The calculated distance of closest approach is approximately 59 fm, which aligns with one of the provided options.
Which of the following was not observed by Rutherford using the scattering of α-rays?
1. Most of the α-particles get slightly deflected from their path.
2. Fewer α-particles get deflected at greater angles.
After completing the gold foil experiment, Rutherford concluded that the size of the nucleus is very small compared to the size of the atom. This is because:
The nucleus of an atom was discovered by:
_______ specifies the preferred orientation in the orbital space of the given energy and size.
What is the ratio of total kinetic energies in laboratory system (TL) and centre of mass system (TC ) in the scattering with projectile of mass m1 and target of mass m2?