To solve the problem of finding the ratio of the radius of the deuteron path (\( r_d \)) to the radius of the proton path (\( r_p \)) in a uniform magnetic field, we follow a step-by-step approach:
The radius \( r \) of a charged particle's path moving perpendicular to a magnetic field is given by the expression: \(r = \frac{mv}{qB}\) where:
The kinetic energy \( KE \) for both particles is:
\(KE = \frac{1}{2}mv^2\)
Given that their kinetic energies are equal, set the kinetic energy equations equal and solve for velocity:
\(\frac{1}{2}m_pv_p^2 = \frac{1}{2}m_dv_d^2\)
where:
From here, find the relationship between their velocities:
\(v_p^2 = \frac{m_d}{m_p} v_d^2\)
Thus, \(v_p = \sqrt{\frac{m_d}{m_p}} v_d\)
For the proton, \(r_p = \frac{m_pv_p}{q_pB}\)
For the deuteron, \(r_d = \frac{m_dv_d}{q_dB}\)
The charge \(q = +e\) for both particles, so it cancels out when comparing
The ratio of the radii is given by:
\(\frac{r_d}{r_p} = \frac{\left(\frac{m_dv_d}{qB}\right)}{\left(\frac{m_pv_p}{qB}\right)} = \frac{m_d v_d}{m_p v_p}\)
Substitute \(v_p = \sqrt{\frac{m_d}{m_p}} v_d\):
\(\frac{r_d}{r_p} = \frac{m_d v_d}{m_p \left(\sqrt{\frac{m_d}{m_p}} v_d\right)} = \sqrt{\frac{m_d}{m_p}}\)
Given that \(m_d = 2m_p\) (for a deuteron which is made up of a proton and a neutron), we have:
\(\frac{r_d}{r_p} = \sqrt{2}\)
The ratio of the radii of the paths of the deuteron and proton is \(\sqrt{2} : 1\). Thus, the correct answer is \( \sqrt{2} : 1 \).
The radius of the path of a charged particle moving in a magnetic field is given by:
\( r = \frac{mv}{qB} \),
where \( m \) is the mass, \( v \) is the velocity, \( q \) is the charge, and \( B \) is the magnetic field strength.
Since both particles have the same kinetic energy, \( \frac{1}{2}mv^2 = K \), and the velocity \( v \) can be expressed as:
\( v = \sqrt{\frac{2K}{m}} \).
Thus, the radius of the proton path \( r_p \) is:
\( r_p = \frac{m_p \sqrt{2K/m_p}}{eB} \),
and the radius of the deuteron path \( r_d \) is:
\( r_d = \frac{m_d \sqrt{2K/m_d}}{eB} \).
Since \( m_d = 2m_p \), the ratio of the radii is:
\( \frac{r_d}{r_p} = \frac{\sqrt{2m_p}}{\sqrt{m_p}} = \sqrt{2} \).
Thus, the ratio is \( \sqrt{2} : 1 \), and the correct answer is Option (3).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)