The problem involves calculating the ratio of the radii of circular paths of two charged particles moving in a magnetic field, specifically ionized hydrogen atoms (protons) and alpha particles (He2+). Both particles enter the magnetic field perpendicularly, and their momenta are given as equal.
Key Concepts:
r = \frac{mv}{qB}
Given that the momenta (\( p = mv \)) for both particles are the same, we can express the radius as:
r = \frac{p}{qB}
Thus, the ratio of the radii of the paths of the ionized hydrogen atom (\( r_H \)) and the alpha particle (\( r_\alpha \)) is:
\frac{r_H}{r_\alpha} = \frac{\frac{p}{q_H B}}{\frac{p}{q_\alpha B}} = \frac{q_\alpha}{q_H}
Plugging in the charges for hydrogen and alpha particles:
Substituting these values, we get:
\frac{r_H}{r_\alpha} = \frac{2e}{e} = 2:1
This shows that the radius of the path of the ionized hydrogen atom is twice that of the alpha particle when both have the same momentum. Therefore, the correct answer is 2:1.
In a uniform magnetic field of \(0.049 T\), a magnetic needle performs \(20\) complete oscillations in \(5\) seconds as shown. The moment of inertia of the needle is \(9.8 \times 10 kg m^2\). If the magnitude of magnetic moment of the needle is \(x \times 10^{-5} Am^2\); then the value of '\(x\)' is
