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).
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}