Question:

A positive, singly ionized atom of mass number \(A_M\) is accelerated from rest by the voltage \(192 V\). Thereafter, it enters a rectangular region of width 𝑀 with magnetic field \(\bar{B_0} = 0.1π‘˜Μ‚\)Tesla, as shown in the figure. The ion finally hits a detector at the distance π‘₯ below its starting trajectory. [Given: Mass of neutron/proton =\((5/3) Γ— 10^{βˆ’27}\) kg, charge of the electron \(= 1.6 Γ— 10^{βˆ’19} C.\)]
Alternative_Text
Which of the following option(s) is(are) correct?

Updated On: Mar 8, 2025
  • The value of π‘₯ for \(𝐻^{ +}\) ion is \(4 cm\)
  • The value of π‘₯ for an ion with \(𝐴M = 144\) is \( 48 \  cm\)
  • For detecting ions with 1 ≀ 𝐴M ≀ 196, the minimum height \((π‘₯_1 βˆ’ π‘₯_0)\)of the detector is 55 cm
  • The minimum width 𝑀 of the region of the magnetic field for detecting ions with \(𝐴_M = 196\) is 56 cm.
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The Correct Option is A, B

Solution and Explanation

Displacement of the Particle in a Magnetic Field 

The displacement of the particle is given by:

\[ x = \frac{2R}{\frac{2mv}{qB}} \] where \( R \) is the radius of the circular path, \( m \) is the mass of the particle, \( v \) is its velocity, \( q \) is its charge, and \( B \) is the magnetic field strength.

Substituting \( v = \frac{2qV}{m} \), we get:

\[ x = \frac{2 \cdot m \cdot \frac{2qV}{m}}{qB} \] Simplifying: \[ x = \frac{4m(qV)}{qB} \] For a proton (\( H^+ \)): \[ x = 4 \, \text{cm} \]

For a Particle with Atomic Mass \( \text{AM} = 144 \):

The displacement is proportional to the square root of the mass: \[ x \propto \sqrt{m} \] Thus, for \( \text{AM} = 144 \) (144 times the proton mass): \[ x = 4 \, \text{cm} \cdot \sqrt{144} = 4 \cdot 12 = 48 \, \text{cm} \]

Conclusion:

The correct options are:

  • Options (1) and (2)
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