To determine the mass ratio of two particles, \( X \) and \( Y \), we consider that they possess identical charges and undergo acceleration through the same potential difference. Subsequently, they enter a uniform magnetic field, traversing circular paths with radii \( R_1 \) for particle \( X \) and \( R_2 \) for particle \( Y \).
The radius \( R \) of a charged particle's circular trajectory in a magnetic field is defined by the formula:
\(R = \frac{mv}{qB}\)
Where:
The kinetic energy \(\left( KE \right)\) of a particle accelerated by a potential difference \( V \) is expressed as:
\(\frac{1}{2}mv^2 = qV\)
From this kinetic energy equation, the velocity can be derived as:
\(v = \sqrt{\frac{2qV}{m}}\)
Substituting this velocity expression into the radius formula:
\(R = \frac{\sqrt{\frac{2qV}{m}} \cdot m}{qB} = \frac{m}{qB} \cdot \sqrt{\frac{2qV}{m}}\)
Upon simplification, the radius equation becomes:
\(R = \sqrt{\frac{2Vm}{qB^2}}\)
Given that particles \( X \) and \( Y \) share the same charge \( q \), potential difference \( V \), and magnetic field strength \( B \), with radii \( R_1 \) and \( R_2 \) respectively, we have:
\(R_1 = \sqrt{\frac{2Vm_1}{qB^2}} \quad \text{and} \quad R_2 = \sqrt{\frac{2Vm_2}{qB^2}}\)
Squaring both sides for \( R_1 \) and \( R_2 \):
\(R_1^2 = \frac{2Vm_1}{qB^2} \quad \text{and} \quad R_2^2 = \frac{2Vm_2}{qB^2}\)
To ascertain the mass ratio \(\frac{m_1}{m_2}\), we divide these two squared radius equations:
\(\frac{R_1^2}{R_2^2} = \frac{m_1}{m_2}\)
Therefore, the mass ratio \(\frac{m_1}{m_2}\) is determined by:
\(\frac{m_1}{m_2} = \left( \frac{R_1}{R_2} \right)^2\)
The correct result is:
\(<\left( \frac{R_1}{R_2} \right)^2 \)
Three long straight wires carrying current are arranged mutually parallel as shown in the figure. The force experienced by \(15\) cm length of wire \(Q\) is ________. (\( \mu_0 = 4\pi \times 10^{-7}\,\text{T m A}^{-1} \)) 